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CDAWeb Served Heliophysics Datasets Beginning with 'M'

MARINER2_HELIO1HR_POSITION: Position in heliocentric coordinates from SPDF Helioweb - Natalia Papitashvili (NASA/GSFC/SPDF)
MARINER2_R0_MAGPLASMA: Mariner2 merged magnetic field and plasma hourly data from COHOWeb Service
MARS_HELIO1HR_POSITION: Position in heliocentric coordinates from SPDF Helioweb - Natalia Papitashvili (NASA/GSFC/SPDF)
MAVEN_HELIO1HR_POSITION: Position in heliocentric coordinates from SPDF Helioweb - Natalia Papitashvili (NASA/GSFC/SPDF)
MERCURY_HELIO1HR_POSITION: Position in heliocentric coordinates from SPDF Helioweb - Natalia Papitashvili (NASA/GSFC/SPDF)
MESSENGER_HELIO1HR_POSITION: Position in heliocentric coordinates from SPDF Helioweb - Natalia Papitashvili (NASA/GSFC/SPDF)
MESSENGER_MAG_RTN: MESSENGER interplanetary magnetic field (1-second/high resolution) in RTN coordinates - Prof. Sean C. Solomon (Carnegie Institution of Washington)
METOP1_POES-SEM2_FLUXES-2SEC: POES-SEM2 2-second Particle Precipitation Data, MetOp-B (MetOp-1 before Sept2012 launch) [Important: these data have known contamination problems: please consult Rob Redmon (sem.poes@noaa.gov) for usage recommendations.] - NGDC and SWPC (NOAA)
METOP2_POES-SEM2_FLUXES-2SEC: POES-SEM2 2-second Particle Precipitation Data, MetOp-A (MetOp-2 before Oct2006 launch) [Important: these data have known contamination problems: please consult Rob Redmon (sem.poes@noaa.gov) for usage recommendations.] - NGDC and SWPC (NOAA)
METOP3_POES-SEM2_FLUXES-2SEC: POES-SEM2 2-second Particle Precipitation Data, MetOp-C (MetOp-3 launched 07 November 2018) [Important: these data have known contamination problems: please consult Rob Redmon (sem.poes@noaa.gov) for usage recommendations.] - NCEI (NOAA)
MGS_MAG_HIGH: Mars Global Surveyor Magnetometer High Resolution - M. Acuna (NASA/GSFC)
MGS_MAG_LOW: Mars Global Surveyor Magnetometer Modified Data - M. Acuna (NASA/GSFC)
MMS1_ASPOC_SRVY_L2: Level 2 Active Spacecraft Potential Control Survey Data - K. Torkar, R. Nakamura (IWF)
MMS1_DSP_FAST_L2_BPSD: search coil magnetometer spectral density - J. Burch, R. Ergun, O. Le Contel (SWRI, LASP, LPP)
MMS1_DSP_FAST_L2_EPSD: electric spectral density - J. Burch, R. Ergun (SWRI, LASP)
MMS1_DSP_SLOW_L2_BPSD: search coil magnetometer spectral density - J. Burch, R. Ergun, O. Le Contel (SWRI, LASP, LPP)
MMS1_DSP_SLOW_L2_EPSD: electric spectral density - J. Burch, R. Ergun (SWRI, LASP)
MMS1_EDI_BRST_L2_AMB: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS1_EDI_BRST_L2_AMB-PM2: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS1_EDI_BRST_L2_EFIELD: Level 2 EDI electric field - Roy Torbert and Hans Vaith (UNH)
MMS1_EDI_BRST_L2_Q0: Level 2 EDI Quality 0 Counts - Roy Torbert, Hans Vaith (UNH)
MMS1_EDI_SRVY_L2_AMB: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS1_EDI_SRVY_L2_AMB-PM2: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS1_EDI_SRVY_L2_EFIELD: Level 2 EDI electric field - Roy Torbert and Hans Vaith (UNH)
MMS1_EDI_SRVY_L2_Q0: Level 2 EDI Quality 0 Counts - Roy Torbert, Hans Vaith (UNH)
MMS1_EDP_BRST_L2_DCE: MMS1 L2 (brst), 3D Electric field - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS1_EDP_BRST_L2_HMFE: MMS1 l2 (brst), 3D HMFE Electric field - Burch, J, Ergun, R., Lindqvist, P. (SwRI, LASP, KTH)
MMS1_EDP_BRST_L2_SCPOT: MMS 1 dual probe scpot (brst), Spacecraft potential - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS1_EDP_FAST_L2_DCE: MMS1 L2 (fast), 3D Electric field - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS1_EDP_FAST_L2_SCPOT: MMS 1 dual probe scpot (fast), Spacecraft potential - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS1_EDP_SLOW_L2_DCE: MMS1 L2 (slow), 3D Electric field - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS1_EDP_SLOW_L2_SCPOT: MMS 1 dual probe scpot (slow), Spacecraft potential - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS1_EDP_SRVY_L2_HFESP: MMS1 L2 (srvy), HF ACE Spectra - Burch, J, Ergun, R., Lindqvist, P. (SwRI, LASP, KTH)
MMS1_EPD-EIS_BRST_L2_EXTOF: Level 2 Energetic Ion Spectrometer EnergyxTOF Brst - B. Mauk (JHU/APL)
MMS1_EPD-EIS_BRST_L2_PHXTOF: Level 2 Energetic Ion Spectrometer PulseHeightxTOF Brst - B. Mauk (JHU/APL)
MMS1_EPD-EIS_SRVY_L2_ELECTRONENERGY: Level 2 Energetic Ion Spectrometer Electron Spectra Srvy - B. Mauk (JHU/APL)
MMS1_EPD-EIS_SRVY_L2_EXTOF: Level 2 Energetic Ion Spectrometer EnergyxTOF Srvy - B. Mauk (JHU/APL)
MMS1_EPD-EIS_SRVY_L2_PHXTOF: Level 2 Energetic Ion Spectrometer PulseHeightxTOF Srvy - B. Mauk (JHU/APL)
MMS1_FEEPS_BRST_L2_ELECTRON: Level 2 Flys Eye Energetic Particle Sensor Burst Data - STP (LASP)
MMS1_FEEPS_BRST_L2_ION: Level 2 Flys Eye Energetic Particle Sensor Burst Data - STP (LASP)
MMS1_FEEPS_SRVY_L2_ELECTRON: Level 2 Flys Eye Energetic Particle Sensor Survey Data - STP (LASP)
MMS1_FEEPS_SRVY_L2_ION: Level 2 Flys Eye Energetic Particle Sensor Survey Data - STP (LASP)
MMS1_FGM_BRST_L2: Level2 Flux Gate Magnetometer Burst DC Magnetic Field for MMS Satellite Number 1 - J. Burch, C. Russell, W. Magnus (SWRI, UCLA, IWF)
MMS1_FGM_SRVY_L2: Level2 Flux Gate Magnetometer Combined Fast/Slow Survey DC Magnetic Field for MMS Satellite Number 1 - J. Burch, C. Russell, W. Magnus (SWRI, UCLA, IWF)
MMS1_FPI_BRST_L2_DES-DIST: MMS Satellite Number 1 Dual Electron Spectrometer Burst-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS1_FPI_BRST_L2_DES-MOMS: MMS Satellite Number 1 Dual Electron Spectrometer Burst-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS1_FPI_BRST_L2_DES-PARTMOMS: MMS Satellite Number 1 Dual Electron Spectrometer Burst-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS1_FPI_BRST_L2_DIS-DIST: MMS Satellite Number 1 Dual Ion Spectrometer Burst-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS1_FPI_BRST_L2_DIS-MOMS: MMS Satellite Number 1 Dual Ion Spectrometer Burst-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS1_FPI_BRST_L2_DIS-PARTMOMS: MMS Satellite Number 1 Dual Ion Spectrometer Burst-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS1_FPI_FAST_L2_DES-DIST: MMS Satellite Number 1 Dual Electron Spectrometer FastSurvey-resolution instrument distributions - J. Burch, B. Giles (SwRI, GSFC)
MMS1_FPI_FAST_L2_DES-MOMS: MMS Satellite Number 1 Dual Electron Spectrometer FastSurvey-resolution distribution moments - J. Burch, B. Giles (SwRI, GSFC)
MMS1_FPI_FAST_L2_DES-MOMSAUX: MMS Satellite Number 1 Dual Electron Spectrometer FastSurvey-resolution auxiliary moments - J. Burch, B. Giles (SwRI, GSFC)
MMS1_FPI_FAST_L2_DES-PARTMOMS: MMS Satellite Number 1 Dual Electron Spectrometer FastSurvey-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS1_FPI_FAST_L2_DIS-DIST: MMS Satellite Number 1 Dual Ion Spectrometer FastSurvey-resolution instrument distributions - J. Burch, B. Giles (SwRI, GSFC)
MMS1_FPI_FAST_L2_DIS-MOMS: MMS Satellite Number 1 Dual Ion Spectrometer FastSurvey-resolution distribution moments - J. Burch, B. Giles (SwRI, GSFC)
MMS1_FPI_FAST_L2_DIS-MOMSAUX: MMS Satellite Number 1 Dual Ion Spectrometer FastSurvey-resolution auxiliary moments - J. Burch, B. Giles (SwRI, GSFC)
MMS1_FPI_FAST_L2_DIS-PARTMOMS: MMS Satellite Number 1 Dual Ion Spectrometer FastSurvey-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS1_FPI_SLOW_L2_DES-DIST: MMS Satellite Number 1 Dual Electron Spectrometer SlowSurvey-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS1_FPI_SLOW_L2_DES-MOMS: MMS Satellite Number 1 Dual Electron Spectrometer SlowSurvey-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS1_FPI_SLOW_L2_DES-MOMSAUX: MMS Satellite Number 1 Dual Electron Spectrometer SlowSurvey-resolution auxiliary moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS1_FPI_SLOW_L2_DIS-DIST: MMS Satellite Number 1 Dual Ion Spectrometer SlowSurvey-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS1_FPI_SLOW_L2_DIS-MOMS: MMS Satellite Number 1 Dual Ion Spectrometer SlowSurvey-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS1_FPI_SLOW_L2_DIS-MOMSAUX: MMS Satellite Number 1 Dual Ion Spectrometer SlowSurvey-resolution auxiliary moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS1_HPCA_BRST_L2_ION: Level 2> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS1_HPCA_BRST_L2_MOMENTS: Level 2 Moments> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS1_HPCA_SRVY_L2_ION: Level 2> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS1_HPCA_SRVY_L2_MOMENTS: Level 2 Moments> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS1_HPCA_SRVY_L2_TOF-COUNTS: Level 1b> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS1_MEC_BRST_L2_EPHT89D: Magnetic ephemeris and support data for MMS satellite number 1 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS1_MEC_BRST_L2_EPHT89Q: Magnetic ephemeris and support data for MMS satellite number 1 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS1_MEC_BRST_L2_EPHTS04D: Magnetic ephemeris and support data for MMS satellite number 1 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS1_MEC_SRVY_L2_EPHT89D: Magnetic ephemeris and support data for MMS satellite number 1 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS1_MEC_SRVY_L2_EPHT89Q: Magnetic ephemeris and support data for MMS satellite number 1 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS1_MEC_SRVY_L2_EPHTS04D: Magnetic ephemeris and support data for MMS satellite number 1 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS1_R0_SUMMARY: Links to MMS-1 pre-generated Quicklook Summary plots - James Burch (SWRI)
MMS1_SCM_BRST_L2_SCB: Level 2 Search Coil Magnetometer AC Magnetic Field Burst (8192S/s) Data - J. Burch, O. Le Contel (SWRI, LPP)
MMS1_SCM_BRST_L2_SCHB: Level 2 Search Coil Magnetometer AC Magnetic Field High Burst (16384S/s) Data - J. Burch, O. Le Contel (SWRI, LPP)
MMS1_SCM_SRVY_L2_SCSRVY: Level 2 Search Coil Magnetometer AC Magnetic Field Survey (32S/s) Data - J. Burch, O. Le Contel (SWRI, LPP)
MMS2_ASPOC_SRVY_L2: Level 2 Active Spacecraft Potential Control Survey Data - K. Torkar, R. Nakamura (IWF)
MMS2_DSP_FAST_L2_BPSD: search coil magnetometer spectral density - J. Burch, R. Ergun, O. Le Contel (SWRI, LASP, LPP)
MMS2_DSP_FAST_L2_EPSD: electric spectral density - J. Burch, R. Ergun (SWRI, LASP)
MMS2_DSP_SLOW_L2_BPSD: search coil magnetometer spectral density - J. Burch, R. Ergun, O. Le Contel (SWRI, LASP, LPP)
MMS2_DSP_SLOW_L2_EPSD: electric spectral density - J. Burch, R. Ergun (SWRI, LASP)
MMS2_EDI_BRST_L2_AMB: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS2_EDI_BRST_L2_AMB-PM2: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS2_EDI_BRST_L2_EFIELD: Level 2 EDI electric field - Roy Torbert and Hans Vaith (UNH)
MMS2_EDI_BRST_L2_Q0: Level 2 EDI Quality 0 Counts - Roy Torbert, Hans Vaith (UNH)
MMS2_EDI_SRVY_L2_AMB: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS2_EDI_SRVY_L2_AMB-PM2: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS2_EDI_SRVY_L2_EFIELD: Level 2 EDI electric field - Roy Torbert and Hans Vaith (UNH)
MMS2_EDI_SRVY_L2_Q0: Level 2 EDI Quality 0 Counts - Roy Torbert, Hans Vaith (UNH)
MMS2_EDP_BRST_L2_DCE: MMS2 L2 (brst), 3D Electric field - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS2_EDP_BRST_L2_HMFE: MMS2 l2 (brst), 3D HMFE Electric field - Burch, J, Ergun, R., Lindqvist, P. (SwRI, LASP, KTH)
MMS2_EDP_BRST_L2_SCPOT: MMS 2 dual probe scpot (brst), Spacecraft potential - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS2_EDP_FAST_L2_DCE: MMS2 L2 (fast), 3D Electric field - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS2_EDP_FAST_L2_SCPOT: MMS 2 dual probe scpot (fast), Spacecraft potential - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS2_EDP_SLOW_L2_DCE: MMS2 L2 (slow), 3D Electric field - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS2_EDP_SLOW_L2_SCPOT: MMS 2 dual probe scpot (slow), Spacecraft potential - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS2_EDP_SRVY_L2_HFESP: MMS2 L2 (srvy), HF ACE Spectra - Burch, J, Ergun, R., Lindqvist, P. (SwRI, LASP, KTH)
MMS2_EPD-EIS_BRST_L2_EXTOF: Level 2 Energetic Ion Spectrometer EnergyxTOF Brst - B. Mauk (JHU/APL)
MMS2_EPD-EIS_BRST_L2_PHXTOF: Level 2 Energetic Ion Spectrometer PulseHeightxTOF Brst - B. Mauk (JHU/APL)
MMS2_EPD-EIS_SRVY_L2_ELECTRONENERGY: Level 2 Energetic Ion Spectrometer Electron Spectra Srvy - B. Mauk (JHU/APL)
MMS2_EPD-EIS_SRVY_L2_EXTOF: Level 2 Energetic Ion Spectrometer EnergyxTOF Srvy - B. Mauk (JHU/APL)
MMS2_EPD-EIS_SRVY_L2_PHXTOF: Level 2 Energetic Ion Spectrometer PulseHeightxTOF Srvy - B. Mauk (JHU/APL)
MMS2_FEEPS_BRST_L2_ELECTRON: Level 2 Flys Eye Energetic Particle Sensor Burst Data - STP (LASP)
MMS2_FEEPS_BRST_L2_ION: Level 2 Flys Eye Energetic Particle Sensor Burst Data - STP (LASP)
MMS2_FEEPS_SRVY_L2_ELECTRON: Level 2 Flys Eye Energetic Particle Sensor Survey Data - STP (LASP)
MMS2_FEEPS_SRVY_L2_ION: Level 2 Flys Eye Energetic Particle Sensor Survey Data - STP (LASP)
MMS2_FGM_BRST_L2: Level2 Flux Gate Magnetometer Burst DC Magnetic Field for MMS Satellite Number 2 - J. Burch, C. Russell, W. Magnus (SWRI, UCLA, IWF)
MMS2_FGM_SRVY_L2: Level2 Flux Gate Magnetometer Combined Fast/Slow Survey DC Magnetic Field for MMS Satellite Number 2 - J. Burch, C. Russell, W. Magnus (SWRI, UCLA, IWF)
MMS2_FPI_BRST_L2_DES-DIST: MMS Satellite Number 2 Dual Electron Spectrometer Burst-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS2_FPI_BRST_L2_DES-MOMS: MMS Satellite Number 2 Dual Electron Spectrometer Burst-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS2_FPI_BRST_L2_DES-PARTMOMS: MMS Satellite Number 2 Dual Electron Spectrometer Burst-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS2_FPI_BRST_L2_DIS-DIST: MMS Satellite Number 2 Dual Ion Spectrometer Burst-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS2_FPI_BRST_L2_DIS-MOMS: MMS Satellite Number 2 Dual Ion Spectrometer Burst-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS2_FPI_BRST_L2_DIS-PARTMOMS: MMS Satellite Number 2 Dual Ion Spectrometer Burst-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS2_FPI_FAST_L2_DES-DIST: MMS Satellite Number 2 Dual Electron Spectrometer FastSurvey-resolution instrument distributions - J. Burch, B. Giles (SwRI, GSFC)
MMS2_FPI_FAST_L2_DES-MOMS: MMS Satellite Number 2 Dual Electron Spectrometer FastSurvey-resolution distribution moments - J. Burch, B. Giles (SwRI, GSFC)
MMS2_FPI_FAST_L2_DES-MOMSAUX: MMS Satellite Number 2 Dual Electron Spectrometer FastSurvey-resolution auxiliary moments - J. Burch, B. Giles (SwRI, GSFC)
MMS2_FPI_FAST_L2_DES-PARTMOMS: MMS Satellite Number 2 Dual Electron Spectrometer FastSurvey-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS2_FPI_FAST_L2_DIS-DIST: MMS Satellite Number 2 Dual Ion Spectrometer FastSurvey-resolution instrument distributions - J. Burch, B. Giles (SwRI, GSFC)
MMS2_FPI_FAST_L2_DIS-MOMS: MMS Satellite Number 2 Dual Ion Spectrometer FastSurvey-resolution distribution moments - J. Burch, B. Giles (SwRI, GSFC)
MMS2_FPI_FAST_L2_DIS-MOMSAUX: MMS Satellite Number 2 Dual Ion Spectrometer FastSurvey-resolution auxiliary moments - J. Burch, B. Giles (SwRI, GSFC)
MMS2_FPI_FAST_L2_DIS-PARTMOMS: MMS Satellite Number 2 Dual Ion Spectrometer FastSurvey-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS2_FPI_SLOW_L2_DES-DIST: MMS Satellite Number 2 Dual Electron Spectrometer SlowSurvey-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS2_FPI_SLOW_L2_DES-MOMS: MMS Satellite Number 2 Dual Electron Spectrometer SlowSurvey-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS2_FPI_SLOW_L2_DES-MOMSAUX: MMS Satellite Number 2 Dual Electron Spectrometer SlowSurvey-resolution auxiliary moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS2_FPI_SLOW_L2_DIS-DIST: MMS Satellite Number 2 Dual Ion Spectrometer SlowSurvey-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS2_FPI_SLOW_L2_DIS-MOMS: MMS Satellite Number 2 Dual Ion Spectrometer SlowSurvey-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS2_FPI_SLOW_L2_DIS-MOMSAUX: MMS Satellite Number 2 Dual Ion Spectrometer SlowSurvey-resolution auxiliary moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS2_HPCA_BRST_L2_ION: Level 2> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS2_HPCA_BRST_L2_MOMENTS: Level 2 Moments> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS2_HPCA_SRVY_L2_ION: Level 2> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS2_HPCA_SRVY_L2_MOMENTS: Level 2 Moments> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS2_HPCA_SRVY_L2_TOF-COUNTS: Level 1b> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS2_MEC_BRST_L2_EPHT89D: Magnetic ephemeris and support data for MMS satellite number 2 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS2_MEC_BRST_L2_EPHT89Q: Magnetic ephemeris and support data for MMS satellite number 2 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS2_MEC_BRST_L2_EPHTS04D: Magnetic ephemeris and support data for MMS satellite number 2 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS2_MEC_SRVY_L2_EPHT89D: Magnetic ephemeris and support data for MMS satellite number 2 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS2_MEC_SRVY_L2_EPHT89Q: Magnetic ephemeris and support data for MMS satellite number 2 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS2_MEC_SRVY_L2_EPHTS04D: Magnetic ephemeris and support data for MMS satellite number 2 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS2_R0_SUMMARY: Links to MMS-2 pre-generated Quicklook Summary plots - James Burch (SWRI)
MMS2_SCM_BRST_L2_SCB: Level 2 Search Coil Magnetometer AC Magnetic Field Burst (8192S/s) Data - J. Burch, O. Le Contel (SWRI, LPP)
MMS2_SCM_BRST_L2_SCHB: Level 2 Search Coil Magnetometer AC Magnetic Field High Burst (16384S/s) Data - J. Burch, O. Le Contel (SWRI, LPP)
MMS2_SCM_SRVY_L2_SCSRVY: Level 2 Search Coil Magnetometer AC Magnetic Field Survey (32S/s) Data - J. Burch, O. Le Contel (SWRI, LPP)
MMS3_ASPOC_SRVY_L2: Level 2 Active Spacecraft Potential Control Survey Data - K. Torkar, R. Nakamura (IWF)
MMS3_DSP_FAST_L2_BPSD: search coil magnetometer spectral density - J. Burch, R. Ergun, O. Le Contel (SWRI, LASP, LPP)
MMS3_DSP_FAST_L2_EPSD: electric spectral density - J. Burch, R. Ergun (SWRI, LASP)
MMS3_DSP_SLOW_L2_BPSD: search coil magnetometer spectral density - J. Burch, R. Ergun, O. Le Contel (SWRI, LASP, LPP)
MMS3_DSP_SLOW_L2_EPSD: electric spectral density - J. Burch, R. Ergun (SWRI, LASP)
MMS3_EDI_BRST_L2_AMB: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS3_EDI_BRST_L2_AMB-PM2: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS3_EDI_BRST_L2_EFIELD: Level 2 EDI electric field - Roy Torbert and Hans Vaith (UNH)
MMS3_EDI_BRST_L2_Q0: Level 2 EDI Quality 0 Counts - Roy Torbert, Hans Vaith (UNH)
MMS3_EDI_SRVY_L2_AMB: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS3_EDI_SRVY_L2_AMB-PM2: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS3_EDI_SRVY_L2_EFIELD: Level 2 EDI electric field - Roy Torbert and Hans Vaith (UNH)
MMS3_EDI_SRVY_L2_Q0: Level 2 EDI Quality 0 Counts - Roy Torbert, Hans Vaith (UNH)
MMS3_EDP_BRST_L2_DCE: MMS3 L2 (brst), 3D Electric field - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS3_EDP_BRST_L2_HMFE: MMS3 l2 (brst), 3D HMFE Electric field - Burch, J, Ergun, R., Lindqvist, P. (SwRI, LASP, KTH)
MMS3_EDP_BRST_L2_SCPOT: MMS 3 dual probe scpot (brst), Spacecraft potential - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS3_EDP_FAST_L2_DCE: MMS3 L2 (fast), 3D Electric field - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS3_EDP_FAST_L2_SCPOT: MMS 3 dual probe scpot (fast), Spacecraft potential - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS3_EDP_SLOW_L2_DCE: MMS3 L2 (slow), 3D Electric field - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS3_EDP_SLOW_L2_SCPOT: MMS 3 dual probe scpot (slow), Spacecraft potential - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS3_EDP_SRVY_L2_HFESP: MMS3 L2 (srvy), HF ACE Spectra - Burch, J, Ergun, R., Lindqvist, P. (SwRI, LASP, KTH)
MMS3_EPD-EIS_BRST_L2_EXTOF: Level 2 Energetic Ion Spectrometer EnergyxTOF Brst - B. Mauk (JHU/APL)
MMS3_EPD-EIS_BRST_L2_PHXTOF: Level 2 Energetic Ion Spectrometer PulseHeightxTOF Brst - B. Mauk (JHU/APL)
MMS3_EPD-EIS_SRVY_L2_ELECTRONENERGY: Level 2 Energetic Ion Spectrometer Electron Spectra Srvy - B. Mauk (JHU/APL)
MMS3_EPD-EIS_SRVY_L2_EXTOF: Level 2 Energetic Ion Spectrometer EnergyxTOF Srvy - B. Mauk (JHU/APL)
MMS3_EPD-EIS_SRVY_L2_PHXTOF: Level 2 Energetic Ion Spectrometer PulseHeightxTOF Srvy - B. Mauk (JHU/APL)
MMS3_FEEPS_BRST_L2_ELECTRON: Level 2 Flys Eye Energetic Particle Sensor Burst Data - STP (LASP)
MMS3_FEEPS_BRST_L2_ION: Level 2 Flys Eye Energetic Particle Sensor Burst Data - STP (LASP)
MMS3_FEEPS_SRVY_L2_ELECTRON: Level 2 Flys Eye Energetic Particle Sensor Survey Data - STP (LASP)
MMS3_FEEPS_SRVY_L2_ION: Level 2 Flys Eye Energetic Particle Sensor Survey Data - STP (LASP)
MMS3_FGM_BRST_L2: Level2 Flux Gate Magnetometer Burst DC Magnetic Field for MMS Satellite Number 3 - J. Burch, C. Russell, W. Magnus (SWRI, UCLA, IWF)
MMS3_FGM_SRVY_L2: Level2 Flux Gate Magnetometer Combined Fast/Slow Survey DC Magnetic Field for MMS Satellite Number 3 - J. Burch, C. Russell, W. Magnus (SWRI, UCLA, IWF)
MMS3_FPI_BRST_L2_DES-DIST: MMS Satellite Number 3 Dual Electron Spectrometer Burst-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS3_FPI_BRST_L2_DES-MOMS: MMS Satellite Number 3 Dual Electron Spectrometer Burst-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS3_FPI_BRST_L2_DES-PARTMOMS: MMS Satellite Number 3 Dual Electron Spectrometer Burst-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS3_FPI_BRST_L2_DIS-DIST: MMS Satellite Number 3 Dual Ion Spectrometer Burst-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS3_FPI_BRST_L2_DIS-MOMS: MMS Satellite Number 3 Dual Ion Spectrometer Burst-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS3_FPI_BRST_L2_DIS-PARTMOMS: MMS Satellite Number 3 Dual Ion Spectrometer Burst-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS3_FPI_FAST_L2_DES-DIST: MMS Satellite Number 3 Dual Electron Spectrometer FastSurvey-resolution instrument distributions - J. Burch, B. Giles (SwRI, GSFC)
MMS3_FPI_FAST_L2_DES-MOMS: MMS Satellite Number 3 Dual Electron Spectrometer FastSurvey-resolution distribution moments - J. Burch, B. Giles (SwRI, GSFC)
MMS3_FPI_FAST_L2_DES-MOMSAUX: MMS Satellite Number 3 Dual Electron Spectrometer FastSurvey-resolution auxiliary moments - J. Burch, B. Giles (SwRI, GSFC)
MMS3_FPI_FAST_L2_DES-PARTMOMS: MMS Satellite Number 3 Dual Electron Spectrometer FastSurvey-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS3_FPI_FAST_L2_DIS-DIST: MMS Satellite Number 3 Dual Ion Spectrometer FastSurvey-resolution instrument distributions - J. Burch, B. Giles (SwRI, GSFC)
MMS3_FPI_FAST_L2_DIS-MOMS: MMS Satellite Number 3 Dual Ion Spectrometer FastSurvey-resolution distribution moments - J. Burch, B. Giles (SwRI, GSFC)
MMS3_FPI_FAST_L2_DIS-MOMSAUX: MMS Satellite Number 3 Dual Ion Spectrometer FastSurvey-resolution auxiliary moments - J. Burch, B. Giles (SwRI, GSFC)
MMS3_FPI_FAST_L2_DIS-PARTMOMS: MMS Satellite Number 3 Dual Ion Spectrometer FastSurvey-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS3_FPI_SLOW_L2_DES-DIST: MMS Satellite Number 3 Dual Electron Spectrometer SlowSurvey-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS3_FPI_SLOW_L2_DES-MOMS: MMS Satellite Number 3 Dual Electron Spectrometer SlowSurvey-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS3_FPI_SLOW_L2_DES-MOMSAUX: MMS Satellite Number 3 Dual Electron Spectrometer SlowSurvey-resolution auxiliary moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS3_FPI_SLOW_L2_DIS-DIST: MMS Satellite Number 3 Dual Ion Spectrometer SlowSurvey-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS3_FPI_SLOW_L2_DIS-MOMS: MMS Satellite Number 3 Dual Ion Spectrometer SlowSurvey-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS3_FPI_SLOW_L2_DIS-MOMSAUX: MMS Satellite Number 3 Dual Ion Spectrometer SlowSurvey-resolution auxiliary moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS3_HPCA_BRST_L2_ION: Level 2> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS3_HPCA_BRST_L2_MOMENTS: Level 2 Moments> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS3_HPCA_SRVY_L2_ION: Level 2> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS3_HPCA_SRVY_L2_MOMENTS: Level 2 Moments> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS3_HPCA_SRVY_L2_TOF-COUNTS: Level 1b> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS3_MEC_BRST_L2_EPHT89D: Magnetic ephemeris and support data for MMS satellite number 3 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS3_MEC_BRST_L2_EPHT89Q: Magnetic ephemeris and support data for MMS satellite number 3 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS3_MEC_BRST_L2_EPHTS04D: Magnetic ephemeris and support data for MMS satellite number 3 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS3_MEC_SRVY_L2_EPHT89D: Magnetic ephemeris and support data for MMS satellite number 3 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS3_MEC_SRVY_L2_EPHT89Q: Magnetic ephemeris and support data for MMS satellite number 3 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS3_MEC_SRVY_L2_EPHTS04D: Magnetic ephemeris and support data for MMS satellite number 3 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS3_R0_SUMMARY: Links to MMS-3 pre-generated Quicklook Summary plots - James Burch (SWRI)
MMS3_SCM_BRST_L2_SCB: Level 2 Search Coil Magnetometer AC Magnetic Field Burst (8192S/s) Data - J. Burch, O. Le Contel (SWRI, LPP)
MMS3_SCM_BRST_L2_SCHB: Level 2 Search Coil Magnetometer AC Magnetic Field High Burst (16384S/s) Data - J. Burch, O. Le Contel (SWRI, LPP)
MMS3_SCM_SRVY_L2_SCSRVY: Level 2 Search Coil Magnetometer AC Magnetic Field Survey (32S/s) Data - J. Burch, O. Le Contel (SWRI, LPP)
MMS4_ASPOC_SRVY_L2: Level 2 Active Spacecraft Potential Control Survey Data - K. Torkar, R. Nakamura (IWF)
MMS4_DSP_FAST_L2_BPSD: search coil magnetometer spectral density - J. Burch, R. Ergun, O. Le Contel (SWRI, LASP, LPP)
MMS4_DSP_FAST_L2_EPSD: electric spectral density - J. Burch, R. Ergun (SWRI, LASP)
MMS4_DSP_SLOW_L2_BPSD: search coil magnetometer spectral density - J. Burch, R. Ergun, O. Le Contel (SWRI, LASP, LPP)
MMS4_DSP_SLOW_L2_EPSD: electric spectral density - J. Burch, R. Ergun (SWRI, LASP)
MMS4_EDI_BRST_L2_AMB: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS4_EDI_BRST_L2_AMB-PM2: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS4_EDI_BRST_L2_EFIELD: Level 2 EDI electric field - Roy Torbert and Hans Vaith (UNH)
MMS4_EDI_BRST_L2_Q0: Level 2 EDI Quality 0 Counts - Roy Torbert, Hans Vaith (UNH)
MMS4_EDI_SRVY_L2_AMB: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS4_EDI_SRVY_L2_AMB-PM2: Level 2 EDI Ambient electron flux - Roy Torbert, Hans Vaith (UNH)
MMS4_EDI_SRVY_L2_EFIELD: Level 2 EDI electric field - Roy Torbert and Hans Vaith (UNH)
MMS4_EDI_SRVY_L2_Q0: Level 2 EDI Quality 0 Counts - Roy Torbert, Hans Vaith (UNH)
MMS4_EDP_BRST_L2_DCE: MMS4 L2 (brst), 3D Electric field - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS4_EDP_BRST_L2_HMFE: MMS4 l2 (brst), 3D HMFE Electric field - Burch, J, Ergun, R., Lindqvist, P. (SwRI, LASP, KTH)
MMS4_EDP_BRST_L2_SCPOT: MMS 4 dual probe scpot (brst), Spacecraft potential - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS4_EDP_FAST_L2_DCE: MMS4 L2 (fast), 3D Electric field - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS4_EDP_FAST_L2_SCPOT: MMS 4 dual probe scpot (fast), Spacecraft potential - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS4_EDP_SLOW_L2_DCE: MMS4 L2 (slow), 3D Electric field - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS4_EDP_SLOW_L2_SCPOT: MMS 4 dual probe scpot (slow), Spacecraft potential - J.Burch, R.Ergun, P.Lindqvist. (SWRI, LASP, KTH)
MMS4_EDP_SRVY_L2_HFESP: MMS4 L2 (srvy), HF ACE Spectra - Burch, J, Ergun, R., Lindqvist, P. (SwRI, LASP, KTH)
MMS4_EPD-EIS_BRST_L2_EXTOF: Level 2 Energetic Ion Spectrometer EnergyxTOF Brst - B. Mauk (JHU/APL)
MMS4_EPD-EIS_BRST_L2_PHXTOF: Level 2 Energetic Ion Spectrometer PulseHeightxTOF Brst - B. Mauk (JHU/APL)
MMS4_EPD-EIS_SRVY_L2_ELECTRONENERGY: Level 2 Energetic Ion Spectrometer Electron Spectra Srvy - B. Mauk (JHU/APL)
MMS4_EPD-EIS_SRVY_L2_EXTOF: Level 2 Energetic Ion Spectrometer EnergyxTOF Srvy - B. Mauk (JHU/APL)
MMS4_EPD-EIS_SRVY_L2_PHXTOF: Level 2 Energetic Ion Spectrometer PulseHeightxTOF Srvy - B. Mauk (JHU/APL)
MMS4_FEEPS_BRST_L2_ELECTRON: Level 2 Flys Eye Energetic Particle Sensor Burst Data - STP (LASP)
MMS4_FEEPS_BRST_L2_ION: Level 2 Flys Eye Energetic Particle Sensor Burst Data - STP (LASP)
MMS4_FEEPS_SRVY_L2_ELECTRON: Level 2 Flys Eye Energetic Particle Sensor Survey Data - STP (LASP)
MMS4_FEEPS_SRVY_L2_ION: Level 2 Flys Eye Energetic Particle Sensor Survey Data - STP (LASP)
MMS4_FGM_BRST_L2: Level2 Flux Gate Magnetometer Burst DC Magnetic Field for MMS Satellite Number 4 - J. Burch, C. Russell, W. Magnus (SWRI, UCLA, IWF)
MMS4_FGM_SRVY_L2: Level2 Flux Gate Magnetometer Combined Fast/Slow Survey DC Magnetic Field for MMS Satellite Number 4 - J. Burch, C. Russell, W. Magnus (SWRI, UCLA, IWF)
MMS4_FPI_BRST_L2_DES-DIST: MMS Satellite Number 4 Dual Electron Spectrometer Burst-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS4_FPI_BRST_L2_DES-MOMS: MMS Satellite Number 4 Dual Electron Spectrometer Burst-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS4_FPI_BRST_L2_DES-PARTMOMS: MMS Satellite Number 4 Dual Electron Spectrometer Burst-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS4_FPI_BRST_L2_DIS-DIST: MMS Satellite Number 4 Dual Ion Spectrometer Burst-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS4_FPI_BRST_L2_DIS-MOMS: MMS Satellite Number 4 Dual Ion Spectrometer Burst-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS4_FPI_BRST_L2_DIS-PARTMOMS: MMS Satellite Number 4 Dual Ion Spectrometer Burst-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS4_FPI_FAST_L2_DES-DIST: MMS Satellite Number 4 Dual Electron Spectrometer FastSurvey-resolution instrument distributions - J. Burch, B. Giles (SwRI, GSFC)
MMS4_FPI_FAST_L2_DES-MOMS: MMS Satellite Number 4 Dual Electron Spectrometer FastSurvey-resolution distribution moments - J. Burch, B. Giles (SwRI, GSFC)
MMS4_FPI_FAST_L2_DES-MOMSAUX: MMS Satellite Number 4 Dual Electron Spectrometer FastSurvey-resolution auxiliary moments - J. Burch, B. Giles (SwRI, GSFC)
MMS4_FPI_FAST_L2_DES-PARTMOMS: MMS Satellite Number 4 Dual Electron Spectrometer FastSurvey-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS4_FPI_FAST_L2_DIS-DIST: MMS Satellite Number 4 Dual Ion Spectrometer FastSurvey-resolution instrument distributions - J. Burch, B. Giles (SwRI, GSFC)
MMS4_FPI_FAST_L2_DIS-MOMS: MMS Satellite Number 4 Dual Ion Spectrometer FastSurvey-resolution distribution moments - J. Burch, B. Giles (SwRI, GSFC)
MMS4_FPI_FAST_L2_DIS-MOMSAUX: MMS Satellite Number 4 Dual Ion Spectrometer FastSurvey-resolution auxiliary moments - J. Burch, B. Giles (SwRI, GSFC)
MMS4_FPI_FAST_L2_DIS-PARTMOMS: MMS Satellite Number 4 Dual Ion Spectrometer FastSurvey-resolution partial moments - J. Burch, B. Giles (SwRI, GSFC)
MMS4_FPI_SLOW_L2_DES-DIST: MMS Satellite Number 4 Dual Electron Spectrometer SlowSurvey-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS4_FPI_SLOW_L2_DES-MOMS: MMS Satellite Number 4 Dual Electron Spectrometer SlowSurvey-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS4_FPI_SLOW_L2_DES-MOMSAUX: MMS Satellite Number 4 Dual Electron Spectrometer SlowSurvey-resolution auxiliary moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS4_FPI_SLOW_L2_DIS-DIST: MMS Satellite Number 4 Dual Ion Spectrometer SlowSurvey-resolution instrument distributions - J. Burch, D. Gershman (SwRI, GSFC)
MMS4_FPI_SLOW_L2_DIS-MOMS: MMS Satellite Number 4 Dual Ion Spectrometer SlowSurvey-resolution distribution moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS4_FPI_SLOW_L2_DIS-MOMSAUX: MMS Satellite Number 4 Dual Ion Spectrometer SlowSurvey-resolution auxiliary moments - J. Burch, D. Gershman (SwRI, GSFC)
MMS4_HPCA_BRST_L2_ION: Level 2> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS4_HPCA_BRST_L2_MOMENTS: Level 2 Moments> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS4_HPCA_SRVY_L2_ION: Level 2> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS4_HPCA_SRVY_L2_MOMENTS: Level 2 Moments> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS4_HPCA_SRVY_L2_TOF-COUNTS: Level 1b> Hot Plasma Composition Analyzer - J. Burch, S. Fuselier (SWRI)
MMS4_MEC_BRST_L2_EPHT89D: Magnetic ephemeris and support data for MMS satellite number 4 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS4_MEC_BRST_L2_EPHT89Q: Magnetic ephemeris and support data for MMS satellite number 4 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS4_MEC_BRST_L2_EPHTS04D: Magnetic ephemeris and support data for MMS satellite number 4 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS4_MEC_SRVY_L2_EPHT89D: Magnetic ephemeris and support data for MMS satellite number 4 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS4_MEC_SRVY_L2_EPHT89Q: Magnetic ephemeris and support data for MMS satellite number 4 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS4_MEC_SRVY_L2_EPHTS04D: Magnetic ephemeris and support data for MMS satellite number 4 - M. G. Henderson, S. K. Morley (Los Alamos National Laboratory (LANL))
MMS4_R0_SUMMARY: Links to MMS-4 pre-generated Quicklook Summary plots - James Burch (SWRI)
MMS4_SCM_BRST_L2_SCB: Level 2 Search Coil Magnetometer AC Magnetic Field Burst (8192S/s) Data - J. Burch, O. Le Contel (SWRI, LPP)
MMS4_SCM_BRST_L2_SCHB: Level 2 Search Coil Magnetometer AC Magnetic Field High Burst (16384S/s) Data - J. Burch, O. Le Contel (SWRI, LPP)
MMS4_SCM_SRVY_L2_SCSRVY: Level 2 Search Coil Magnetometer AC Magnetic Field Survey (32S/s) Data - J. Burch, O. Le Contel (SWRI, LPP)
MOON_HELIO1HR_POSITION: Position in heliocentric coordinates from SPDF Helioweb - Natalia Papitashvili (NASA/GSFC/SPDF)
MSL_RAD_OBS-L1: MSL/RAD Level 1 observational counter data - D. Hassler (SwRI-Boulder)
MSL_RAD_OBS-L2: MSL/RAD Level 2 observational radiation data - D. Hassler (SwRI-Boulder)
MUNIN_M1_MDSE: MUNIN, MEDUSA IDFS format - David Winningham (Southwest Research Institute)
MUNIN_M1_MDSI: MUNIN, MEDUSA IDFS format - David Winningham (Southwest Research Institute)
MUNIN_M1_OA: MUNIN, Orbit and attitude data IDFS format - Rymd Plasma Gruppen (Swedish Institute of Space Physics)
MVN_INSITU_KP-4SEC: MAVEN In-situ Key Parameters - B.M. Jakosky (LASP/U. Colorado)
MVN_MAG_L2-SUNSTATE-1SEC: MAVEN Magnetometer Sun-State 1 Second Magnetic Field - J. Connerney (NASA GSFC)
MVN_SEP_L2_S1-CAL-SVY-FULL: DERIVED FROM: MAVEN SEP (Solar Energetic Particle) Instrument - D. Larson (davin@ssl.berkeley.edu) (U.C. Berkeley Space Sciences Laboratory)
MVN_SEP_L2_S2-CAL-SVY-FULL: DERIVED FROM: MAVEN SEP (Solar Energetic Particle) Instrument - D. Larson (davin@ssl.berkeley.edu) (U.C. Berkeley Space Sciences Laboratory)
MVN_STA_L2_D8-12R1E: MAVEN Supra-Thermal And Thermal Ion Composition Particle Distributions - J. P. McFadden (U.C. Berkeley Space Sciences Laboratory)
MVN_STA_L2_D9-12R64E: MAVEN Supra-Thermal And Thermal Ion Composition Particle Distributions - J. P. McFadden (U.C. Berkeley Space Sciences Laboratory)
MVN_STA_L2_DA-1R64E: MAVEN Supra-Thermal And Thermal Ion Composition Particle Distributions - J. P. McFadden (U.C. Berkeley Space Sciences Laboratory)
MVN_SWE_L2_ARC3D: DERIVED FROM: MAVEN SWEA (Solar Wind Electron Analyzer) 3D Distributions - David L. Mitchell (mitchell@ssl.berkeley.edu) (UC Berkeley Space Sciences Laboratory)
MVN_SWE_L2_ARCPAD: DERIVED FROM: MAVEN SWEA (Solar Wind Electron Analyzer) Pitch Angle Distributions - David L. Mitchell (mitchell@ssl.berkeley.edu) (UC Berkeley Space Sciences Laboratory)
MVN_SWE_L2_SVY3D: DERIVED FROM: MAVEN SWEA (Solar Wind Electron Analyzer) 3D Distributions - David L. Mitchell (mitchell@ssl.berkeley.edu) (UC Berkeley Space Sciences Laboratory)
MVN_SWE_L2_SVYPAD: DERIVED FROM: MAVEN SWEA (Solar Wind Electron Analyzer) Pitch Angle Distributions - David L. Mitchell (mitchell@ssl.berkeley.edu) (UC Berkeley Space Sciences Laboratory)
MVN_SWE_L2_SVYSPEC: DERIVED FROM: MAVEN SWEA (Solar Wind Electron Analyzer) Energy Spectra - David L. Mitchell (mitchell@ssl.berkeley.edu) (UC Berkeley Space Sciences Laboratory)
MVN_SWI_L2_COARSEARC3D: DERIVED FROM: MAVEN SWIA (Solar Wind Ion Analyzer), Coarse 3d Distributions - J.S. Halekas (U Iowa)
MVN_SWI_L2_COARSESVY3D: DERIVED FROM: MAVEN SWIA (Solar Wind Ion Analyzer), Coarse 3d Distributions - J.S. Halekas (U Iowa)
MVN_SWI_L2_FINEARC3D: DERIVED FROM: MAVEN SWIA (Solar Wind Ion Analyzer), Fine 3d Distributions - J.S. Halekas (U Iowa)
MVN_SWI_L2_FINESVY3D: DERIVED FROM: MAVEN SWIA (Solar Wind Ion Analyzer), Fine 3d Distributions - J.S. Halekas (U Iowa)
MVN_SWI_L2_ONBOARDSVYMOM: DERIVED FROM: MAVEN SWIA (Solar Wind Ion Analyzer), Onboard Moments - J.S. Halekas (U Iowa)
MVN_SWI_L2_ONBOARDSVYSPEC: DERIVED FROM: MAVEN SWIA (Solar Wind Ion Analyzer), Onboard Energy Spectra - J.S. Halekas (U Iowa)

MARINER2_HELIO1HR_POSITION doi:10.48322/me2b-8q74
Proper citations should include the "Accessed on date" in the form .
Description
No TEXT global attribute value.
 
  • Data Variable Descriptions
      Distance from Sun to object [RAD_AU]
      
      
      Latitude in Solar Ecliptic Coordinate System (SE) [SE_LAT]
      
      
      Longitude in Solar Ecliptic Coordinate System (SE) [SE_LON]
      
      
      Latitude in heliographic Rotating Coordinate System (HG) [HG_LAT]
      
      
      Longitude in Heliographic Rotating Coordinate System (HG) [HG_LON]
      
      
      Latitude in heliographic Inertial Coordinate System (HGI) [HGI_LAT]
      
      
      Longitude in heliographic Inertial Coordinate System (HGI) [HGI_LON]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MARINER2_R0_MAGPLASMA
Description
Mariner2 COHOweb connection
 
  • Data Variable Descriptions
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MARS_HELIO1HR_POSITION
Description
No TEXT global attribute value.
 
  • Data Variable Descriptions
      Distance from Sun to object [RAD_AU]
      
      
      Latitude in Solar Ecliptic Coordinate System (SE) [SE_LAT]
      
      
      Longitude in Solar Ecliptic Coordinate System (SE) [SE_LON]
      
      
      Latitude in heliographic Rotating Coordinate System (HG) [HG_LAT]
      
      
      Longitude in Heliographic Rotating Coordinate System (HG) [HG_LON]
      
      
      Latitude in heliographic Inertial Coordinate System (HGI) [HGI_LAT]
      
      
      Longitude in heliographic Inertial Coordinate System (HGI) [HGI_LON]
      
      
Dataset in CDAWeb
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MAVEN_HELIO1HR_POSITION doi:10.48322/90ar-hx32
Proper citations should include the "Accessed on date" in the form .
Description
No TEXT global attribute value.
 
  • Data Variable Descriptions
      Distance from Sun to object [RAD_AU]
      
      
      Latitude in Solar Ecliptic Coordinate System (SE) [SE_LAT]
      
      
      Longitude in Solar Ecliptic Coordinate System (SE) [SE_LON]
      
      
      Latitude in heliographic Rotating Coordinate System (HG) [HG_LAT]
      
      
      Longitude in Heliographic Rotating Coordinate System (HG) [HG_LON]
      
      
      Latitude in heliographic Inertial Coordinate System (HGI) [HGI_LAT]
      
      
      Longitude in heliographic Inertial Coordinate System (HGI) [HGI_LON]
      
      
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MERCURY_HELIO1HR_POSITION
Description
No TEXT global attribute value.
 
  • Data Variable Descriptions
      Distance from Sun to object [RAD_AU]
      
      
      Latitude in Solar Ecliptic Coordinate System (SE) [SE_LAT]
      
      
      Longitude in Solar Ecliptic Coordinate System (SE) [SE_LON]
      
      
      Latitude in heliographic Rotating Coordinate System (HG) [HG_LAT]
      
      
      Longitude in Heliographic Rotating Coordinate System (HG) [HG_LON]
      
      
      Latitude in heliographic Inertial Coordinate System (HGI) [HGI_LAT]
      
      
      Longitude in heliographic Inertial Coordinate System (HGI) [HGI_LON]
      
      
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MESSENGER_HELIO1HR_POSITION doi:10.48322/sx90-xh93
Proper citations should include the "Accessed on date" in the form .
Description
No TEXT global attribute value.
 
  • Data Variable Descriptions
      Distance from Sun to object [RAD_AU]
      
      
      Latitude in Solar Ecliptic Coordinate System (SE) [SE_LAT]
      
      
      Longitude in Solar Ecliptic Coordinate System (SE) [SE_LON]
      
      
      Latitude in heliographic Rotating Coordinate System (HG) [HG_LAT]
      
      
      Longitude in Heliographic Rotating Coordinate System (HG) [HG_LON]
      
      
      Latitude in heliographic Inertial Coordinate System (HGI) [HGI_LAT]
      
      
      Longitude in heliographic Inertial Coordinate System (HGI) [HGI_LON]
      
      
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MESSENGER_MAG_RTN (spase://NASA/NumericalData/MESSENGER/MAG/PT0.05S)
Description
The Mercury Surface, Space Environment, Geochemistry and Ranging (MESSENGER)
mission is designed to study the characteristics and environment of Mercury from
orbit. Specifically, the scientific objectives of the mission are to
characterize the chemical composition of Mercury's surface, the geologic
history, the nature of the magnetic field, the size and state of the core, the
volatile inventory at the poles, and the nature of Mercurys exosphere and
magnetosphere over a nominal orbital mission of one Earth year
MESSENGER launched on 3 August 2004 at 6:15:56 UT (2:15:56 a.m. EDT) on a Delta
7925H (a Delta II Heavy launch vehicle with nine strap-on solid-rocket
boosters). The spacecraft was injected into solar orbit 57 minutes later.  The
solar panels were then deployed and the spacecraft began sending data on its
status. One year after launch, on 2 August 2005, MESSENGER flew by Earth at an
altitude of 2347 km. On 12 December 2005 at 11:30 UT, MESSENGER fired its large
thruster for 524 seconds, changing the spacecraft velocity by 316 m/s and
putting it on course for its 24 October 2006 Venus flyby at an altitude of 2990
km. The second Venus flyby took place on 5 June 2007 at 23:08 UT (7:08 p.m. EDT)
at an altitude of approximately 337 km. The first of three Mercury flybys, all
at roughly 200 km altitude, occurred on 14 January 2008 at 19:04:39 UT, and the
second on 6 October 2008 at 08:40:22 UT.  The third will be on 29 September
2009. There are also five deep space manuevers. Data collected during the
Mercury flybys will be used to help plan the scientific campaign during the
orbital phase. Mercury orbit insertion will take place on 18 March 2011,
requiring a delta-V of 0.867 km/s. The nominal orbit is planned to have a
periapsis of 200 km at 60 degrees N latitude, an apoapsis of 15,193 km, a period
of 12 hours and an inclination of 80 degrees. The periapsis will slowly rise due
to solar perturbations to over 400 km at the end of 88 days (one Mercury year)
at which point it will be readjusted to a 200 km, 12 hour orbit via a two burn
sequence. Data will be collected from orbit for one Earth year, the nominal end
of the primary mission will be in March 2012.  Global stereo image coverage at
250 m/pixel resolution is expected. The mission should also yield global
composition maps, a 3-D model of Mercury's magnetosphere, topographic profiles
of the northern hemisphere, gravity field to degree and order 16, altitude
profiles of elemental species, and a characterization of the volatiles in
permanently shadowed craters at the poles.
The MESSENGER spacecraft is a squat box (1.27 m x 1.42 m x 1.85 m) with a
semi-cylindrical thermal shade (roughly 2.5 meters tall and 2 meters wide) for
protection from the Sun and two solar panel wings extending radially about 6
meters from tip to tip.  A 3.6 m magnetometer boom also extends from the craft.
The total mass of the spacecraft is 1093 kg, 607.8 kg of this is propellant and
helium. The structure is primarily graphite-cyanate-ester (GrCE) composite and
consists of two vertical panels which support two large fuel tanks and two
vertical panels which support the oxidizer tank and plumbing panel. The four
vertical panels make up the center column and are bolted at their aft ends to an
aluminum adapter. A single top deck panel mounts the LVA (large velocity adjust)
thruster, small thrusters, helium and auxiliary fuel tanks, star trackers and
battery.
Main propulsion is via the 645-N, 317-s bipropellant LVA thruster, four 22-N
monopropellant thrusters provide spacecraft steering during main thruster burns,
and ten 4-N monopropellant thrusters are used for attitude control. There is
also a reaction-wheel attitude control system. Knowledge for attitude control is
provided by star tracking cameras, an inertial measurement unit, and six solar
sensors. Power is provided by the solar panels, which extend beyond the sunshade
and are rotatable to balance panel temperature and power generation, which
provides a nominal 450 W in Mercury orbit. The panels are 70% optical solar
reflectors and 30% GaAs/Ge cells. The power is stored in a
common-pressure-vessel nickel-hydrogen battery, with 11 vessels and 2 cells per
vessel.
Communications are in X-band with downlink through two fixed phased-array
antenna clusters and uplink and downlink through medium- and low-gain antennas
on the forward and aft sides of the spacecraft. Passive thermal control,
primarily a fixed opaque ceramic cloth sunshade, is utilized to maintain
operating temperatures near the Sun. Radiators are built into the structure and
the orbit is optimized to minimize infrared and visible light heating of the
spacecraft from the surface of Mercury. Multilayer insulation, low conductivity
couplings, and heaters are also used to maintain temperatures within operating
limits.
Five science instruments are mounted externally on the bottom deck of the main
body: the Mercury Dual Imaging System (MDIS), Gamma-Ray and Neutron Spectrometer
(GRNS), X-ray Spectrometer (XRS), Mercury Laser Altimeter (MLA), and Atmospheric
and Surface Composition Spectrometer (MASCS). The Energetic Particle and Plasma
Spectrometer (EPPS) is mounted on the side and top deck and the magnetometer
(MAG) is at the end of the 3.6 m boom. Radio Science (RS) experiments will use
the existing communications system.
The Messenger MAG instrument is a miniature three-axis ring-core fluxgate
magnetometer with low-noise electronics. It is mounted on a 3.6 m boom in the
anti-sunward direction. The MAG has .. 1530 and ..51300 nT ranges with 20-bit
internal resolution and 17-bit output resolution. The MAG probe samples magnetic
field values along the X, Y, and Z axes at a rate of up to 20 samples/second
(commandable and can vary). This dataset has 3-axis calibrated samples of the
magnetic field in heliospheric RTN coordinates in units of nano-Tesla, Br, Bt,
Bn. The spacecraft position is identified by radial distance from the Sun,
latitude above the ecliptic plane, and azimuth with respect to the Earth-Sun
line in the ecliptic plane. 
Anderson, B. J., M. H. Acuna, D. A. Lohr , J. Scheifele, A. Raval, H. Korth, and
J. A. Slavin, \'The Magnetometer instrument on MESSENGER\', Space Science
Reviews, 2007.[ANDREWSETAL2007]
 
  • Data Variable Descriptions
      Radial distance of MESSENGER from the Sun [radialDistance]
      
      
      ----> North latitude from the ecliptic plane [latitude_ecliptic]
      
      
      ----> Azimuthal angle from Earth-Sun line in ecliptic plane, positive in the direction of Earth's motion [azimuth_ecliptic]
      Azimuthal angle of MESSENGER spacecraft in the instantaneous ecliptic plane with
      respect to the Earth-Sun line in units of degrees, positive in direction of the
      Earth's orbital motion with Z in J2000 coordinates
      
      Radial distance of MESSENGER from the Sun (0.5 sec cadence) [radialDistance_200]
      
      
      ----> North latitude from the ecliptic plane (0.5 sec cadence) [latitude_ecliptic_200]
      
      
      ----> Azimuthal angle from Earth-Sun line in ecliptic plane, positive in the direction of Earth's motion (0.5 sec cadence) [azimuth_ecliptic_200]
      Azimuthal angle of MESSENGER spacecraft in the instantaneous ecliptic plane with
      respect to the Earth-Sun line in units of degrees, positive in direction of the
      Earth's orbital motion with Z in J2000 coordinates
      
      (Good values only) B radial (Br) in RTN coordinates [B_radial_q]
      
      
      ----> (Good values only) B tangential (Bt) [B_tangential_q]
      
      
      ----> (Good values only) B normal (Bn) [B_normal_q]
      
      
      (Good values at 0.5 sec cadence only) B radial (Br) in RTN coordinates [B_radial_200]
      
      
      ----> (Good values at 0.5 sec cadence only) B tangential (Bt) [B_tangential_200]
      
      
      ----> (Good values at 0.5 sec cadence only) B normal (Bn) [B_normal_200]
      
      
      (All qualities) B radial (Br) in RTN coordinates [B_radial]
      
      
      ----> (All qualities) B tangential (Bt) [B_tangential]
      
      
      ----> (All qualities) B normal (Bn) [B_normal]
      
      
      3-digit daily quality flag (222 or 223 = good = boom deployed, sensor in shadow, any heater contamination corrected) [Quality_Flag]
      
      
      Data Cadence [Epoch_cadence]
      Computed on the fly to determine the time res. between points 
      
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METOP1_POES-SEM2_FLUXES-2SEC (spase://NOAA/NumericalData/MetOp/B/SEM-2/CDF/PT2S)
Description
POES N19 data: POES/MetOp: Particle Precipitation Data (These data have known
contamination problems. Please consult provider rob.redmon@noaa.gov for usage
recommendations.) 
 
  • Data Variable Descriptions
      Electron differential flux, TED, 0 degree telescope, 189-7980 eV [ted_ele_flux_stackt0]
      
      
      ---> 30 degree telescope [ted_ele_flux_stackt30]
      
      
      Electron differential flux, TED, 0 and 30 degree telescopes, 189 eV [ted_ele_flux_t_stacke1]
      
      
      ---> 844 eV [ted_ele_flux_t_stacke2]
      
      
      ---> 2595 eV [ted_ele_flux_t_stacke3]
      
      
      ---> 7980 eV [ted_ele_flux_t_stacke4]
      
      
      Proton differential flux, TED, 0 degree telescope, 189-7980 eV [ted_pro_flux_stackt0]
      
      
      ---> 30 degree telescope [ted_pro_flux_stackt30]
      
      
      Proton differential flux, TED, 0 and 30 degree telescopes, 189 eV [ted_pro_flux_t_stacke1]
      
      
      ---> 844 eV [ted_pro_flux_t_stacke2]
      
      
      ---> 2595 eV [ted_pro_flux_t_stacke3]
      
      
      ---> 7980 eV [ted_pro_flux_t_stacke4]
      
      
      Electron integral energy flux, TED, 0 degree telescope, low energy (50-1000 eV) [ted_ele_tel0_low_eflux]
      
      
      ---> 30 degree telescope [ted_ele_tel30_low_eflux]
      
      
      ---> % error, 0 degree telescope [ted_ele_tel0_low_eflux_error]
      
      
      ---> % error, 30 degree telescope [ted_ele_tel30_low_eflux_error]
      
      
      Electron integral energy flux, TED, 0 degree telescope, high energy (1-20 keV) [ted_ele_tel0_hi_eflux]
      
      
      ---> 30 degree telescope [ted_ele_tel30_hi_eflux]
      
      
      ---> % error, 0 degree telescope [ted_ele_tel0_hi_eflux_error]
      
      
      ---> % error, 30 degree telescope [ted_ele_tel30_hi_eflux_error]
      
      
      Proton integral energy flux, TED, 0 degree telescope, low energy (50-1000 eV) [ted_pro_tel0_low_eflux]
      
      
      ---> 30 degree telescope [ted_pro_tel30_low_eflux]
      
      
      ---> % error, 0 degree telescope [ted_pro_tel0_low_eflux_error]
      
      
      ---> % error, 30 degree telescope [ted_pro_tel30_low_eflux_error]
      
      
      Proton integral energy flux, TED, 0 degree telescope, high energy (1-20 keV) [ted_pro_tel0_hi_eflux]
      
      
      ---> 30 degree telescope [ted_pro_tel30_hi_eflux]
      
      
      ---> % error, 0 degree telescope [ted_pro_tel0_hi_eflux_error]
      
      
      ---> % error, 30 degree telescope [ted_pro_tel30_hi_eflux_error]
      
      
      Electron atmospheric integral energy flux, TED, low energy (50-1000 eV), at 120 km [ted_ele_eflux_atmo_low]
      
      
      ---> high energy (1-20 keV) [ted_ele_eflux_atmo_hi]
      
      
      ---> % error, low energy [ted_ele_eflux_atmo_low_err]
      
      
      ---> % error, high energy [ted_ele_eflux_atmo_hi_err]
      
      
      Electron total atmospheric integral energy flux, TED, at 120 km [ted_ele_eflux_atmo_total]
      
      
      ---> % error [ted_ele_eflux_atmo_total_err]
      
      
      Proton atmospheric integral energy flux, TED, low energy (50-1000 eV), at 120 km [ted_pro_eflux_atmo_low]
      
      
      ---> high energy (1-20 keV) [ted_pro_eflux_atmo_hi]
      
      
      ---> % error, low energy [ted_pro_eflux_atmo_low_err]
      
      
      ---> % error, high energy [ted_pro_eflux_atmo_hi_err]
      
      
      Proton total atmospheric integral energy flux, TED, at 120 km [ted_pro_eflux_atmo_total]
      
      
      ---> % error [ted_pro_eflux_atmo_total_err]
      
      
      Electron and Proton total atmospheric integral energy flux, TED, at 120 km [ted_total_eflux_atmo]
      
      
      ---> % error [ted_total_eflux_atmo_err]
      
      
      Electron characteristic energy channel, TED, 0 degree telescope [ted_ele_energy_tel0]
      
      
      ---> 30 degree telescope [ted_ele_energy_tel30]
      
      
      Proton characteristic energy channel, TED, 0 degree telescope [ted_pro_energy_tel0]
      
      
      ---> 30 degree telescope [ted_pro_energy_tel30]
      
      
      Electron maximum differential flux, TED, 0 degree telescope [ted_ele_max_flux_tel0]
      
      
      ---> 30 degree telescope [ted_ele_max_flux_tel30]
      
      
      Proton maximum differential flux, TED, 0 degree telescope [ted_pro_max_flux_tel0]
      
      
      ---> 30 degree telescope [ted_pro_max_flux_tel30]
      
      
      Electron background integral energy flux, TED, 0 degree telescope, low energy [ted_ele_eflux_bg_tel0_low]
      
      
      ---> 30 degree telescope, low energy [ted_ele_eflux_bg_tel30_low]
      
      
      ---> 0 degree telescope, high energy [ted_ele_eflux_bg_tel0_hi]
      
      
      ---> 30 degree telescope, high energy [ted_ele_eflux_bg_tel30_hi]
      
      
      Proton background integral energy flux, TED, 0 degree telescope, low energy [ted_pro_eflux_bg_tel0_low]
      
      
      ---> 30 degree telescope, low energy [ted_pro_eflux_bg_tel30_low]
      
      
      ---> 0 degree telescope, high energy [ted_pro_eflux_bg_tel0_hi]
      
      
      ---> 30 degree telescope, high energy [ted_pro_eflux_bg_tel30_hi]
      
      
      Electron background counts, TED, 0 degree telescope, low energy [ted_ele_eflux_bg_tel0_low_cps]
      
      
      ---> 30 degree telescope, low energy [ted_ele_eflux_bg_tel30_low_cps]
      
      
      ---> 0 degree telescope, high energy [ted_ele_eflux_bg_tel0_hi_cps]
      
      
      ---> 30 degree telescope, high energy [ted_ele_eflux_bg_tel30_hi_cps]
      
      
      Proton background counts, TED, 0 degree telescope, low energy [ted_pro_eflux_bg_tel0_low_cps]
      
      
      ---> 30 degree telescope, low energy [ted_pro_eflux_bg_tel30_low_cps]
      
      
      ---> 0 degree telescope, high energy [ted_pro_eflux_bg_tel0_hi_cps]
      
      
      ---> 30 degree telescope, high energy [ted_pro_eflux_bg_tel30_hi_cps]
      
      
      Pitch angle (satellite), TED, 0 degree telescope [ted_alpha_0_sat]
      
      
      ---> 30 degree telescope [ted_alpha_30_sat]
      
      
      Pitch angle (foot of field line), TED, 0 degree telescope [ted_alpha_0_foot]
      
      
      ---> 30 degree telescope [ted_alpha_30_foot]
      
      
      IFC flag (0=off, 1=on), TED [ted_ifc_on]
      
      
      Electron integral flux, MEPED, 0 degree telescope, >40 to >612 keV [mep_ele_flux_stackt0]
      
      
      ---> % Error [mep_ele_flux_err_stackt0]
      
      
      Electron integral flux, MEPED, 90 degree telescope, >40 to >612 keV [mep_ele_flux_stackt90]
      
      
      ---> % Error [mep_ele_flux_err_stackt90]
      
      
      Electron integral flux, MEPED, 0 and 90 degree telescopes, >40 keV [mep_ele_flux_t_stacke1]
      
      
      ---> >130 keV [mep_ele_flux_t_stacke2]
      
      
      ---> >287 keV [mep_ele_flux_t_stacke3]
      
      
      ---> >612 keV [mep_ele_flux_t_stacke4]
      
      
      Proton differential flux, MEPED, 0 degree telescope, 39-2723 keV [mep_pro_flux_stackt0]
      
      
      ---> % Error [mep_pro_flux_err_stackt0]
      
      
      Proton differential flux, MEPED, 90 degree telescope, 39-2723 keV [mep_pro_flux_stackt90]
      
      
      ---> % Error [mep_pro_flux_err_stackt90]
      
      
      Proton differential flux, MEPED, 0 and 90 degree telescopes, 39 keV [mep_pro_flux_t_stacke1]
      
      
      ---> 115 keV [mep_pro_flux_t_stacke2]
      
      
      ---> 332 keV [mep_pro_flux_t_stacke3]
      
      
      ---> 1105 keV [mep_pro_flux_t_stacke4]
      
      
      ---> 2723 keV [mep_pro_flux_t_stacke5]
      
      
      Proton integral flux, MEPED, 0 and 90 degree telescopes, >6174 keV [mep_pro_flux_p6]
      
      
      ---> % Error [mep_pro_flux_p6_err]
      
      
      Proton differential flux, MEPED Omni telescope, at center energies 25, 50, and 100 MeV, [mep_omni_flux_stack]
      
      
      ---> Fit flag [mep_omni_flux_flag_fit]
      
      
      ---> Gamma [mep_omni_gamma_stack]
      
      
      Pitch angle (satellite), MEPED, 0 degree telescope [meped_alpha_0_sat]
      
      
      ---> 90 degree telescope [meped_alpha_90_sat]
      
      
      Pitch angle (foot of field line), MEPED, 0 degree telescope [meped_alpha_0_foot]
      
      
      ---> 90 degree telescope [meped_alpha_90_foot]
      
      
      IFC flag (0=off, 1=on), MEPED [mep_ifc_on]
      
      
      Satellite Designation ID [satid]
      
      
      Altitude [alt]
      
      
      Geodetic latitude (satellite) [lat]
      
      
      ---> Geodetic longitude (satellite) [lon]
      
      
      Magnetic latitude (satellite) [mag_lat_sat]
      
      
      ---> Magnetic longitude (satellite) [mag_lon_sat]
      
      
      L value of the satellite from IGRF field [l_igrf]
      
      
      Magnetic local time (hours) [mlt]
      
      
      Geodetic latitude (foot of field line) [geod_lat_foot]
      
      
      ---> Geodetic longitude (foot of field line) [geod_lon_foot]
      
      
      AACGM latitude (foot of field line) [aacgm_lat_foot]
      
      
      ---> AACGM longitude (foot of field line) [aacgm_lon_foot]
      
      
      Magnetic latitude (foot of field line) [mag_lat_foot]
      
      
      ---> Magnetic longitude (foot of field line) [mag_lon_foot]
      
      
      B-radial IGRF (satellite) [br_sat]
      
      
      ---> B-theta IGRF (satellite) [bt_sat]
      
      
      ---> B-phi IGRF (satellite) [bp_sat]
      
      
      ---> B-total IGRF (satellite) [btot_sat]
      
      
      B-radial IGRF (foot of field line) [br_foot]
      
      
      ---> B-theta IGRF (foot of field line) [bt_foot]
      
      
      ---> B-phi IGRF (foot of field line) [bp_foot]
      
      
      ---> B-total IGRF (foot of field line) [btot_foot]
      
      
      Bx IGRF satellite coordinates (towards Earth) [bx_sat]
      
      
      ---> By IGRF satellite coordinates (opposite velocity direction) [by_sat]
      
      
      ---> Bz IGRF satellite coordinates (XxY direction) [bz_sat]
      
      
      [TEXT LABEL] Altitude of the satellite [alt_text]
      
      
      ---> Geodetic latitude (satellite) [lat_text]
      
      
      ---> Geodetic longitude (satellite) [lon_text]
      
      
      ---> L value of the satellite from IGRF field [l_igrf_text]
      
      
      ---> Magnetic local time (hours) [mlt_text]
      
      
      ---> Geodetic latitude (foot of field line) [geod_lat_foot_text]
      
      
      ---> Geodetic longitude (foot of field line) [geod_lon_foot_text]
      
      
      ---> AACGM latitude (foot of field line) [aacgm_lat_foot_text]
      
      
      ---> AACGM longitude (foot of field line) [aacgm_lon_foot_text]
      
      
      ---> Magnetic latitude (foot of field line) [mag_lat_foot_text]
      
      
      ---> Magnetic longitude (foot of field line) [mag_lon_foot_text]
      
      
      [TEXT LABEL] B-radial IGRF (satellite) [br_sat_text]
      
      
      ---> B-theta IGRF (satellite) [bt_sat_text]
      
      
      ---> B-phi IGRF (satellite) [bp_sat_text]
      
      
      ---> B-total IGRF (satellite) [btot_sat_text]
      
      
      ---> B-radial IGRF (foot of field line) [br_foot_text]
      
      
      ---> B-theta IGRF (foot of field line) [bt_foot_text]
      
      
      ---> B-phi IGRF (foot of field line) [bp_foot_text]
      
      
      ---> B-total IGRF (foot of field line) [btot_foot_text]
      
      
      ---> Bx IGRF satellite coordinates (towards Earth) [bx_sat_text]
      
      
      ---> By IGRF satellite coordinates (opposite velocity direction) [by_sat_text]
      
      
      ---> Bz IGRF satellite coordinates (XxY direction) [bz_sat_text]
      
      
Dataset in CDAWeb
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METOP2_POES-SEM2_FLUXES-2SEC (spase://NOAA/NumericalData/MetOp/A/SEM-2/CDF/PT2S)
Description
POES N19 data: POES/MetOp: Particle Precipitation Data (These data have known
contamination problems. Please consult provider rob.redmon@noaa.gov for usage
recommendations.) 
 
  • Data Variable Descriptions
      Electron differential flux, TED, 0 degree telescope, 189-7980 eV [ted_ele_flux_stackt0]
      
      
      ---> 30 degree telescope [ted_ele_flux_stackt30]
      
      
      Electron differential flux, TED, 0 and 30 degree telescopes, 189 eV [ted_ele_flux_t_stacke1]
      
      
      ---> 844 eV [ted_ele_flux_t_stacke2]
      
      
      ---> 2595 eV [ted_ele_flux_t_stacke3]
      
      
      ---> 7980 eV [ted_ele_flux_t_stacke4]
      
      
      Proton differential flux, TED, 0 degree telescope, 189-7980 eV [ted_pro_flux_stackt0]
      
      
      ---> 30 degree telescope [ted_pro_flux_stackt30]
      
      
      Proton differential flux, TED, 0 and 30 degree telescopes, 189 eV [ted_pro_flux_t_stacke1]
      
      
      ---> 844 eV [ted_pro_flux_t_stacke2]
      
      
      ---> 2595 eV [ted_pro_flux_t_stacke3]
      
      
      ---> 7980 eV [ted_pro_flux_t_stacke4]
      
      
      Electron integral energy flux, TED, 0 degree telescope, low energy (50-1000 eV) [ted_ele_tel0_low_eflux]
      
      
      ---> 30 degree telescope [ted_ele_tel30_low_eflux]
      
      
      ---> % error, 0 degree telescope [ted_ele_tel0_low_eflux_error]
      
      
      ---> % error, 30 degree telescope [ted_ele_tel30_low_eflux_error]
      
      
      Electron integral energy flux, TED, 0 degree telescope, high energy (1-20 keV) [ted_ele_tel0_hi_eflux]
      
      
      ---> 30 degree telescope [ted_ele_tel30_hi_eflux]
      
      
      ---> % error, 0 degree telescope [ted_ele_tel0_hi_eflux_error]
      
      
      ---> % error, 30 degree telescope [ted_ele_tel30_hi_eflux_error]
      
      
      Proton integral energy flux, TED, 0 degree telescope, low energy (50-1000 eV) [ted_pro_tel0_low_eflux]
      
      
      ---> 30 degree telescope [ted_pro_tel30_low_eflux]
      
      
      ---> % error, 0 degree telescope [ted_pro_tel0_low_eflux_error]
      
      
      ---> % error, 30 degree telescope [ted_pro_tel30_low_eflux_error]
      
      
      Proton integral energy flux, TED, 0 degree telescope, high energy (1-20 keV) [ted_pro_tel0_hi_eflux]
      
      
      ---> 30 degree telescope [ted_pro_tel30_hi_eflux]
      
      
      ---> % error, 0 degree telescope [ted_pro_tel0_hi_eflux_error]
      
      
      ---> % error, 30 degree telescope [ted_pro_tel30_hi_eflux_error]
      
      
      Electron atmospheric integral energy flux, TED, low energy (50-1000 eV), at 120 km [ted_ele_eflux_atmo_low]
      
      
      ---> high energy (1-20 keV) [ted_ele_eflux_atmo_hi]
      
      
      ---> % error, low energy [ted_ele_eflux_atmo_low_err]
      
      
      ---> % error, high energy [ted_ele_eflux_atmo_hi_err]
      
      
      Electron total atmospheric integral energy flux, TED, at 120 km [ted_ele_eflux_atmo_total]
      
      
      ---> % error [ted_ele_eflux_atmo_total_err]
      
      
      Proton atmospheric integral energy flux, TED, low energy (50-1000 eV), at 120 km [ted_pro_eflux_atmo_low]
      
      
      ---> high energy (1-20 keV) [ted_pro_eflux_atmo_hi]
      
      
      ---> % error, low energy [ted_pro_eflux_atmo_low_err]
      
      
      ---> % error, high energy [ted_pro_eflux_atmo_hi_err]
      
      
      Proton total atmospheric integral energy flux, TED, at 120 km [ted_pro_eflux_atmo_total]
      
      
      ---> % error [ted_pro_eflux_atmo_total_err]
      
      
      Electron and Proton total atmospheric integral energy flux, TED, at 120 km [ted_total_eflux_atmo]
      
      
      ---> % error [ted_total_eflux_atmo_err]
      
      
      Electron characteristic energy channel, TED, 0 degree telescope [ted_ele_energy_tel0]
      
      
      ---> 30 degree telescope [ted_ele_energy_tel30]
      
      
      Proton characteristic energy channel, TED, 0 degree telescope [ted_pro_energy_tel0]
      
      
      ---> 30 degree telescope [ted_pro_energy_tel30]
      
      
      Electron maximum differential flux, TED, 0 degree telescope [ted_ele_max_flux_tel0]
      
      
      ---> 30 degree telescope [ted_ele_max_flux_tel30]
      
      
      Proton maximum differential flux, TED, 0 degree telescope [ted_pro_max_flux_tel0]
      
      
      ---> 30 degree telescope [ted_pro_max_flux_tel30]
      
      
      Electron background integral energy flux, TED, 0 degree telescope, low energy [ted_ele_eflux_bg_tel0_low]
      
      
      ---> 30 degree telescope, low energy [ted_ele_eflux_bg_tel30_low]
      
      
      ---> 0 degree telescope, high energy [ted_ele_eflux_bg_tel0_hi]
      
      
      ---> 30 degree telescope, high energy [ted_ele_eflux_bg_tel30_hi]
      
      
      Proton background integral energy flux, TED, 0 degree telescope, low energy [ted_pro_eflux_bg_tel0_low]
      
      
      ---> 30 degree telescope, low energy [ted_pro_eflux_bg_tel30_low]
      
      
      ---> 0 degree telescope, high energy [ted_pro_eflux_bg_tel0_hi]
      
      
      ---> 30 degree telescope, high energy [ted_pro_eflux_bg_tel30_hi]
      
      
      Electron background counts, TED, 0 degree telescope, low energy [ted_ele_eflux_bg_tel0_low_cps]
      
      
      ---> 30 degree telescope, low energy [ted_ele_eflux_bg_tel30_low_cps]
      
      
      ---> 0 degree telescope, high energy [ted_ele_eflux_bg_tel0_hi_cps]
      
      
      ---> 30 degree telescope, high energy [ted_ele_eflux_bg_tel30_hi_cps]
      
      
      Proton background counts, TED, 0 degree telescope, low energy [ted_pro_eflux_bg_tel0_low_cps]
      
      
      ---> 30 degree telescope, low energy [ted_pro_eflux_bg_tel30_low_cps]
      
      
      ---> 0 degree telescope, high energy [ted_pro_eflux_bg_tel0_hi_cps]
      
      
      ---> 30 degree telescope, high energy [ted_pro_eflux_bg_tel30_hi_cps]
      
      
      Pitch angle (satellite), TED, 0 degree telescope [ted_alpha_0_sat]
      
      
      ---> 30 degree telescope [ted_alpha_30_sat]
      
      
      Pitch angle (foot of field line), TED, 0 degree telescope [ted_alpha_0_foot]
      
      
      ---> 30 degree telescope [ted_alpha_30_foot]
      
      
      IFC flag (0=off, 1=on), TED [ted_ifc_on]
      
      
      Electron integral flux, MEPED, 0 degree telescope, >40 to >612 keV [mep_ele_flux_stackt0]
      
      
      ---> % Error [mep_ele_flux_err_stackt0]
      
      
      Electron integral flux, MEPED, 90 degree telescope, >40 to >612 keV [mep_ele_flux_stackt90]
      
      
      ---> % Error [mep_ele_flux_err_stackt90]
      
      
      Electron integral flux, MEPED, 0 and 90 degree telescopes, >40 keV [mep_ele_flux_t_stacke1]
      
      
      ---> >130 keV [mep_ele_flux_t_stacke2]
      
      
      ---> >287 keV [mep_ele_flux_t_stacke3]
      
      
      ---> >612 keV [mep_ele_flux_t_stacke4]
      
      
      Proton differential flux, MEPED, 0 degree telescope, 39-2723 keV [mep_pro_flux_stackt0]
      
      
      ---> % Error [mep_pro_flux_err_stackt0]
      
      
      Proton differential flux, MEPED, 90 degree telescope, 39-2723 keV [mep_pro_flux_stackt90]
      
      
      ---> % Error [mep_pro_flux_err_stackt90]
      
      
      Proton differential flux, MEPED, 0 and 90 degree telescopes, 39 keV [mep_pro_flux_t_stacke1]
      
      
      ---> 115 keV [mep_pro_flux_t_stacke2]
      
      
      ---> 332 keV [mep_pro_flux_t_stacke3]
      
      
      ---> 1105 keV [mep_pro_flux_t_stacke4]
      
      
      ---> 2723 keV [mep_pro_flux_t_stacke5]
      
      
      Proton integral flux, MEPED, 0 and 90 degree telescopes, >6174 keV [mep_pro_flux_p6]
      
      
      ---> % Error [mep_pro_flux_p6_err]
      
      
      Proton differential flux, MEPED Omni telescope, at center energies 25, 50, and 100 MeV, [mep_omni_flux_stack]
      
      
      ---> Fit flag [mep_omni_flux_flag_fit]
      
      
      ---> Gamma [mep_omni_gamma_stack]
      
      
      Pitch angle (satellite), MEPED, 0 degree telescope [meped_alpha_0_sat]
      
      
      ---> 90 degree telescope [meped_alpha_90_sat]
      
      
      Pitch angle (foot of field line), MEPED, 0 degree telescope [meped_alpha_0_foot]
      
      
      ---> 90 degree telescope [meped_alpha_90_foot]
      
      
      IFC flag (0=off, 1=on), MEPED [mep_ifc_on]
      
      
      Satellite Designation ID [satid]
      
      
      Altitude [alt]
      
      
      Geodetic latitude (satellite) [lat]
      
      
      ---> Geodetic longitude (satellite) [lon]
      
      
      Magnetic latitude (satellite) [mag_lat_sat]
      
      
      ---> Magnetic longitude (satellite) [mag_lon_sat]
      
      
      L value of the satellite from IGRF field [l_igrf]
      
      
      Magnetic local time (hours) [mlt]
      
      
      Geodetic latitude (foot of field line) [geod_lat_foot]
      
      
      ---> Geodetic longitude (foot of field line) [geod_lon_foot]
      
      
      AACGM latitude (foot of field line) [aacgm_lat_foot]
      
      
      ---> AACGM longitude (foot of field line) [aacgm_lon_foot]
      
      
      Magnetic latitude (foot of field line) [mag_lat_foot]
      
      
      ---> Magnetic longitude (foot of field line) [mag_lon_foot]
      
      
      B-radial IGRF (satellite) [br_sat]
      
      
      ---> B-theta IGRF (satellite) [bt_sat]
      
      
      ---> B-phi IGRF (satellite) [bp_sat]
      
      
      ---> B-total IGRF (satellite) [btot_sat]
      
      
      B-radial IGRF (foot of field line) [br_foot]
      
      
      ---> B-theta IGRF (foot of field line) [bt_foot]
      
      
      ---> B-phi IGRF (foot of field line) [bp_foot]
      
      
      ---> B-total IGRF (foot of field line) [btot_foot]
      
      
      Bx IGRF satellite coordinates (towards Earth) [bx_sat]
      
      
      ---> By IGRF satellite coordinates (opposite velocity direction) [by_sat]
      
      
      ---> Bz IGRF satellite coordinates (XxY direction) [bz_sat]
      
      
      [TEXT LABEL] Altitude of the satellite [alt_text]
      
      
      ---> Geodetic latitude (satellite) [lat_text]
      
      
      ---> Geodetic longitude (satellite) [lon_text]
      
      
      ---> L value of the satellite from IGRF field [l_igrf_text]
      
      
      ---> Magnetic local time (hours) [mlt_text]
      
      
      ---> Geodetic latitude (foot of field line) [geod_lat_foot_text]
      
      
      ---> Geodetic longitude (foot of field line) [geod_lon_foot_text]
      
      
      ---> AACGM latitude (foot of field line) [aacgm_lat_foot_text]
      
      
      ---> AACGM longitude (foot of field line) [aacgm_lon_foot_text]
      
      
      ---> Magnetic latitude (foot of field line) [mag_lat_foot_text]
      
      
      ---> Magnetic longitude (foot of field line) [mag_lon_foot_text]
      
      
      [TEXT LABEL] B-radial IGRF (satellite) [br_sat_text]
      
      
      ---> B-theta IGRF (satellite) [bt_sat_text]
      
      
      ---> B-phi IGRF (satellite) [bp_sat_text]
      
      
      ---> B-total IGRF (satellite) [btot_sat_text]
      
      
      ---> B-radial IGRF (foot of field line) [br_foot_text]
      
      
      ---> B-theta IGRF (foot of field line) [bt_foot_text]
      
      
      ---> B-phi IGRF (foot of field line) [bp_foot_text]
      
      
      ---> B-total IGRF (foot of field line) [btot_foot_text]
      
      
      ---> Bx IGRF satellite coordinates (towards Earth) [bx_sat_text]
      
      
      ---> By IGRF satellite coordinates (opposite velocity direction) [by_sat_text]
      
      
      ---> Bz IGRF satellite coordinates (XxY direction) [bz_sat_text]
      
      
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METOP3_POES-SEM2_FLUXES-2SEC
Description
POES N19 data: POES/MetOp: Particle Precipitation Data (These data have known
contamination problems. Please consult provider rob.redmon@noaa.gov for usage
recommendations.) 
 
  • Data Variable Descriptions
      Electron differential flux, TED, 0 degree telescope, 189-7980 eV [ted_ele_flux_stackt0]
      
      
      ---> 30 degree telescope [ted_ele_flux_stackt30]
      
      
      Electron differential flux, TED, 0 and 30 degree telescopes, 189 eV [ted_ele_flux_t_stacke1]
      
      
      ---> 844 eV [ted_ele_flux_t_stacke2]
      
      
      ---> 2595 eV [ted_ele_flux_t_stacke3]
      
      
      ---> 7980 eV [ted_ele_flux_t_stacke4]
      
      
      Proton differential flux, TED, 0 degree telescope, 189-7980 eV [ted_pro_flux_stackt0]
      
      
      ---> 30 degree telescope [ted_pro_flux_stackt30]
      
      
      Proton differential flux, TED, 0 and 30 degree telescopes, 189 eV [ted_pro_flux_t_stacke1]
      
      
      ---> 844 eV [ted_pro_flux_t_stacke2]
      
      
      ---> 2595 eV [ted_pro_flux_t_stacke3]
      
      
      ---> 7980 eV [ted_pro_flux_t_stacke4]
      
      
      Electron integral energy flux, TED, 0 degree telescope, low energy (50-1000 eV) [ted_ele_tel0_low_eflux]
      
      
      ---> 30 degree telescope [ted_ele_tel30_low_eflux]
      
      
      ---> % error, 0 degree telescope [ted_ele_tel0_low_eflux_error]
      
      
      ---> % error, 30 degree telescope [ted_ele_tel30_low_eflux_error]
      
      
      Electron integral energy flux, TED, 0 degree telescope, high energy (1-20 keV) [ted_ele_tel0_hi_eflux]
      
      
      ---> 30 degree telescope [ted_ele_tel30_hi_eflux]
      
      
      ---> % error, 0 degree telescope [ted_ele_tel0_hi_eflux_error]
      
      
      ---> % error, 30 degree telescope [ted_ele_tel30_hi_eflux_error]
      
      
      Proton integral energy flux, TED, 0 degree telescope, low energy (50-1000 eV) [ted_pro_tel0_low_eflux]
      
      
      ---> 30 degree telescope [ted_pro_tel30_low_eflux]
      
      
      ---> % error, 0 degree telescope [ted_pro_tel0_low_eflux_error]
      
      
      ---> % error, 30 degree telescope [ted_pro_tel30_low_eflux_error]
      
      
      Proton integral energy flux, TED, 0 degree telescope, high energy (1-20 keV) [ted_pro_tel0_hi_eflux]
      
      
      ---> 30 degree telescope [ted_pro_tel30_hi_eflux]
      
      
      ---> % error, 0 degree telescope [ted_pro_tel0_hi_eflux_error]
      
      
      ---> % error, 30 degree telescope [ted_pro_tel30_hi_eflux_error]
      
      
      Electron atmospheric integral energy flux, TED, low energy (50-1000 eV), at 120 km [ted_ele_eflux_atmo_low]
      
      
      ---> high energy (1-20 keV) [ted_ele_eflux_atmo_hi]
      
      
      ---> % error, low energy [ted_ele_eflux_atmo_low_err]
      
      
      ---> % error, high energy [ted_ele_eflux_atmo_hi_err]
      
      
      Electron total atmospheric integral energy flux, TED, at 120 km [ted_ele_eflux_atmo_total]
      
      
      ---> % error [ted_ele_eflux_atmo_total_err]
      
      
      Proton atmospheric integral energy flux, TED, low energy (50-1000 eV), at 120 km [ted_pro_eflux_atmo_low]
      
      
      ---> high energy (1-20 keV) [ted_pro_eflux_atmo_hi]
      
      
      ---> % error, low energy [ted_pro_eflux_atmo_low_err]
      
      
      ---> % error, high energy [ted_pro_eflux_atmo_hi_err]
      
      
      Proton total atmospheric integral energy flux, TED, at 120 km [ted_pro_eflux_atmo_total]
      
      
      ---> % error [ted_pro_eflux_atmo_total_err]
      
      
      Electron and Proton total atmospheric integral energy flux, TED, at 120 km [ted_total_eflux_atmo]
      
      
      ---> % error [ted_total_eflux_atmo_err]
      
      
      Electron characteristic energy channel, TED, 0 degree telescope [ted_ele_energy_tel0]
      
      
      ---> 30 degree telescope [ted_ele_energy_tel30]
      
      
      Proton characteristic energy channel, TED, 0 degree telescope [ted_pro_energy_tel0]
      
      
      ---> 30 degree telescope [ted_pro_energy_tel30]
      
      
      Electron maximum differential flux, TED, 0 degree telescope [ted_ele_max_flux_tel0]
      
      
      ---> 30 degree telescope [ted_ele_max_flux_tel30]
      
      
      Proton maximum differential flux, TED, 0 degree telescope [ted_pro_max_flux_tel0]
      
      
      ---> 30 degree telescope [ted_pro_max_flux_tel30]
      
      
      Electron background integral energy flux, TED, 0 degree telescope, low energy [ted_ele_eflux_bg_tel0_low]
      
      
      ---> 30 degree telescope, low energy [ted_ele_eflux_bg_tel30_low]
      
      
      ---> 0 degree telescope, high energy [ted_ele_eflux_bg_tel0_hi]
      
      
      ---> 30 degree telescope, high energy [ted_ele_eflux_bg_tel30_hi]
      
      
      Proton background integral energy flux, TED, 0 degree telescope, low energy [ted_pro_eflux_bg_tel0_low]
      
      
      ---> 30 degree telescope, low energy [ted_pro_eflux_bg_tel30_low]
      
      
      ---> 0 degree telescope, high energy [ted_pro_eflux_bg_tel0_hi]
      
      
      ---> 30 degree telescope, high energy [ted_pro_eflux_bg_tel30_hi]
      
      
      Electron background counts, TED, 0 degree telescope, low energy [ted_ele_eflux_bg_tel0_low_cps]
      
      
      ---> 30 degree telescope, low energy [ted_ele_eflux_bg_tel30_low_cps]
      
      
      ---> 0 degree telescope, high energy [ted_ele_eflux_bg_tel0_hi_cps]
      
      
      ---> 30 degree telescope, high energy [ted_ele_eflux_bg_tel30_hi_cps]
      
      
      Proton background counts, TED, 0 degree telescope, low energy [ted_pro_eflux_bg_tel0_low_cps]
      
      
      ---> 30 degree telescope, low energy [ted_pro_eflux_bg_tel30_low_cps]
      
      
      ---> 0 degree telescope, high energy [ted_pro_eflux_bg_tel0_hi_cps]
      
      
      ---> 30 degree telescope, high energy [ted_pro_eflux_bg_tel30_hi_cps]
      
      
      Pitch angle (satellite), TED, 0 degree telescope [ted_alpha_0_sat]
      
      
      ---> 30 degree telescope [ted_alpha_30_sat]
      
      
      Pitch angle (foot of field line), TED, 0 degree telescope [ted_alpha_0_foot]
      
      
      ---> 30 degree telescope [ted_alpha_30_foot]
      
      
      IFC flag (0=off, 1=on), TED [ted_ifc_on]
      
      
      Electron integral flux, MEPED, 0 degree telescope, >40 to >612 keV [mep_ele_flux_stackt0]
      
      
      ---> % Error [mep_ele_flux_err_stackt0]
      
      
      Electron integral flux, MEPED, 90 degree telescope, >40 to >612 keV [mep_ele_flux_stackt90]
      
      
      ---> % Error [mep_ele_flux_err_stackt90]
      
      
      Electron integral flux, MEPED, 0 and 90 degree telescopes, >40 keV [mep_ele_flux_t_stacke1]
      
      
      ---> >130 keV [mep_ele_flux_t_stacke2]
      
      
      ---> >287 keV [mep_ele_flux_t_stacke3]
      
      
      ---> >612 keV [mep_ele_flux_t_stacke4]
      
      
      Proton differential flux, MEPED, 0 degree telescope, 39-2723 keV [mep_pro_flux_stackt0]
      
      
      ---> % Error [mep_pro_flux_err_stackt0]
      
      
      Proton differential flux, MEPED, 90 degree telescope, 39-2723 keV [mep_pro_flux_stackt90]
      
      
      ---> % Error [mep_pro_flux_err_stackt90]
      
      
      Proton differential flux, MEPED, 0 and 90 degree telescopes, 39 keV [mep_pro_flux_t_stacke1]
      
      
      ---> 115 keV [mep_pro_flux_t_stacke2]
      
      
      ---> 332 keV [mep_pro_flux_t_stacke3]
      
      
      ---> 1105 keV [mep_pro_flux_t_stacke4]
      
      
      ---> 2723 keV [mep_pro_flux_t_stacke5]
      
      
      Proton integral flux, MEPED, 0 and 90 degree telescopes, >6174 keV [mep_pro_flux_p6]
      
      
      ---> % Error [mep_pro_flux_p6_err]
      
      
      Proton differential flux, MEPED Omni telescope, at center energies 25, 50, and 100 MeV, [mep_omni_flux_stack]
      
      
      ---> Fit flag [mep_omni_flux_flag_fit]
      
      
      ---> Gamma [mep_omni_gamma_stack]
      
      
      Pitch angle (satellite), MEPED, 0 degree telescope [meped_alpha_0_sat]
      
      
      ---> 90 degree telescope [meped_alpha_90_sat]
      
      
      Pitch angle (foot of field line), MEPED, 0 degree telescope [meped_alpha_0_foot]
      
      
      ---> 90 degree telescope [meped_alpha_90_foot]
      
      
      IFC flag (0=off, 1=on), MEPED [mep_ifc_on]
      
      
      Satellite Designation ID [satid]
      
      
      Altitude [alt]
      
      
      Geodetic latitude (satellite) [lat]
      
      
      ---> Geodetic longitude (satellite) [lon]
      
      
      Magnetic latitude (satellite) [mag_lat_sat]
      
      
      ---> Magnetic longitude (satellite) [mag_lon_sat]
      
      
      L value of the satellite from IGRF field [l_igrf]
      
      
      Magnetic local time (hours) [mlt]
      
      
      Geodetic latitude (foot of field line) [geod_lat_foot]
      
      
      ---> Geodetic longitude (foot of field line) [geod_lon_foot]
      
      
      AACGM latitude (foot of field line) [aacgm_lat_foot]
      
      
      ---> AACGM longitude (foot of field line) [aacgm_lon_foot]
      
      
      Magnetic latitude (foot of field line) [mag_lat_foot]
      
      
      ---> Magnetic longitude (foot of field line) [mag_lon_foot]
      
      
      B-radial IGRF (satellite) [br_sat]
      
      
      ---> B-theta IGRF (satellite) [bt_sat]
      
      
      ---> B-phi IGRF (satellite) [bp_sat]
      
      
      ---> B-total IGRF (satellite) [btot_sat]
      
      
      B-radial IGRF (foot of field line) [br_foot]
      
      
      ---> B-theta IGRF (foot of field line) [bt_foot]
      
      
      ---> B-phi IGRF (foot of field line) [bp_foot]
      
      
      ---> B-total IGRF (foot of field line) [btot_foot]
      
      
      Bx IGRF satellite coordinates (towards Earth) [bx_sat]
      
      
      ---> By IGRF satellite coordinates (opposite velocity direction) [by_sat]
      
      
      ---> Bz IGRF satellite coordinates (XxY direction) [bz_sat]
      
      
      [TEXT LABEL] Altitude of the satellite [alt_text]
      
      
      ---> Geodetic latitude (satellite) [lat_text]
      
      
      ---> Geodetic longitude (satellite) [lon_text]
      
      
      ---> L value of the satellite from IGRF field [l_igrf_text]
      
      
      ---> Magnetic local time (hours) [mlt_text]
      
      
      ---> Geodetic latitude (foot of field line) [geod_lat_foot_text]
      
      
      ---> Geodetic longitude (foot of field line) [geod_lon_foot_text]
      
      
      ---> AACGM latitude (foot of field line) [aacgm_lat_foot_text]
      
      
      ---> AACGM longitude (foot of field line) [aacgm_lon_foot_text]
      
      
      ---> Magnetic latitude (foot of field line) [mag_lat_foot_text]
      
      
      ---> Magnetic longitude (foot of field line) [mag_lon_foot_text]
      
      
      [TEXT LABEL] B-radial IGRF (satellite) [br_sat_text]
      
      
      ---> B-theta IGRF (satellite) [bt_sat_text]
      
      
      ---> B-phi IGRF (satellite) [bp_sat_text]
      
      
      ---> B-total IGRF (satellite) [btot_sat_text]
      
      
      ---> B-radial IGRF (foot of field line) [br_foot_text]
      
      
      ---> B-theta IGRF (foot of field line) [bt_foot_text]
      
      
      ---> B-phi IGRF (foot of field line) [bp_foot_text]
      
      
      ---> B-total IGRF (foot of field line) [btot_foot_text]
      
      
      ---> Bx IGRF satellite coordinates (towards Earth) [bx_sat_text]
      
      
      ---> By IGRF satellite coordinates (opposite velocity direction) [by_sat_text]
      
      
      ---> Bz IGRF satellite coordinates (XxY direction) [bz_sat_text]
      
      
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MGS_MAG_HIGH
Description
The Mars Global Surveyor magnetic field instrument consists of dual, triaxial
fluxgate magnetometers, capable of measuring fields between +/- 4 nT and +/-
65536 nT. Automated range switching allows the instrument to maintain maximum
digital resolution over a wide range of field strengths. The text of this
instrument description has been abstracted from the   instrument paper:  Acuna,
M. A., J. E. P. Connerney, P. Wasilewski, R. P. Lin,     K. A. Anderson, C. W.
Carlson, J. McFadden, D. W. Curtis, H. Reme,  A. Cros, J. L. Medale, J. A.
Sauvaud, C. d'Uston, S. J. Bauer,  P. Cloutier, M. Mayhew, and N. F. Ness, Mars
Observer Magnetic   Fields Investigation, J. Geophys. Res., 97, 7799-7814, 1992.
 
  • Data Variable Descriptions
      Spacecraft Position x in MSO coordinates. [sc_position_x_ss]
      
      
      Spacecraft Position y in MSO coordinates. [sc_position_y_ss]
      
      
      Spacecraft Position z in MSO coordinates. [sc_position_z_ss]
      
      
      Spacecraft Position x in planetocentric coordinates. [sc_position_x_pc]
      
      
      Spacecraft Position y in planetocentric coordinates. [sc_position_y_pc]
      
      
      Spacecraft Position z in planetocentric coordinates. [sc_position_z_pc]
      
      
      Altitude [altitude]
      High Resolution. Interpolated from low resolution (which uses the radius of Mars
      = 3389.5 km)
      
      Decimal Day [decimal_day]
      
      
      Magnetic Field Range Sunstate [b_range_hss]
      sun-state, ss, or MSO
      
      Magnetic Field X MSO [bx_hss]
      High resolution in sun-state or MSO coordinates. Outboard.
      
      Magnetic Field Y MSO [by_hss]
      High resolution in sun-state or MSO coordinates. Outboard.
      
      Magnetic Field Z MSO [bz_hss]
      High resolution in sun-state or MSO coordinates. Outboard.
      
      Magnetic Field Range Payload [b_range_high_pl]
      High resolution in payload coordinates.
      
      Magnetic Field X Payload [bx_high_pl]
      High resolution in payload coordinates. Outboard.
      
      Magnetic Field Y Payload [by_high_pl]
      High resolution in payload coordinates. Outboard.
      
      Magnetic Field Z Payload [bz_high_pl]
      High resolution in payload coordinates. Outboard.
      
      Magnetic Field Magnitude [magnitude]
      Magnitude calculated via the square root of the sum of the squares.
      
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MGS_MAG_LOW
Description
The Mars Global Surveyor magnetic field instrument consists of dual, triaxial
fluxgate magnetometers, capable of measuring fields between +/- 4 nT and +/-
65536 nT. Automated range switching allows the instrument to maintain maximum
digital resolution over a wide range of field strengths. The text of this
instrument description has been abstracted from the   instrument paper:  Acuna,
M. A., J. E. P. Connerney, P. Wasilewski, R. P. Lin,     K. A. Anderson, C. W.
Carlson, J. McFadden, D. W. Curtis, H. Reme,  A. Cros, J. L. Medale, J. A.
Sauvaud, C. d'Uston, S. J. Bauer,  P. Cloutier, M. Mayhew, and N. F. Ness, Mars
Observer Magnetic   Fields Investigation, J. Geophys. Res., 97, 7799-7814, 1992.
 
  • Data Variable Descriptions
      Altitude [altitude]
      Low Resolution. Calculated as the radius of Mars (= 3389.5 km) subtracted from
      the spacecraft position.
      
      Decimal Day [decimal_day]
      Low resolution
      
      Dynamic Range [dynamic_b_pl_range]
      Gain range of the instrument at the time of the sample. Sample quantization is
      gain range dependent. A negative value indicate a detail word (versus fullword)
      entry.
      
      Dynamic Spacecraft Field X [dynamic_bx_lpl]
      Dynamic spacecraft field in payload  coordinates (this has been removed from the
      measured field to compensate for spacecraft field); see sc_mod.ker at
      https://pds-ppi.igpp.ucla.edu/search/view/?f=yes&id=pds://PPI/MGS-M-MAG-3-MAP1_F
      ULLWORD-RES-MAG-V1.0/GEOMETRY and
      https://pds-ppi.igpp.ucla.edu/search/view/?f=yes&id=pds://PPI/MGS-M-MAG-3-PREMAP
      _FULLWORD-RES-MAG-V1.0/GEOMETRY Low resolution.
      
      Dynamic Spacecraft Field Y [dynamic_by_lpl]
      Dynamic spacecraft field in payload  coordinates (this has been removed from the
      measured field to compensate for spacecraft field); see sc_mod.ker at
      https://pds-ppi.igpp.ucla.edu/search/view/?f=yes&id=pds://PPI/MGS-M-MAG-3-MAP1_F
      ULLWORD-RES-MAG-V1.0/GEOMETRY and
      https://pds-ppi.igpp.ucla.edu/search/view/?f=yes&id=pds://PPI/MGS-M-MAG-3-PREMAP
      _FULLWORD-RES-MAG-V1.0/GEOMETRY Low resolution.
      
      Dynamic Spacecraft Field Z [dynamic_bz_lpl]
      Dynamic spacecraft field in payload  coordinates (this has been removed from the
      measured field to compensate for spacecraft field); see sc_mod.ker at
      https://pds-ppi.igpp.ucla.edu/search/view/?f=yes&id=pds://PPI/MGS-M-MAG-3-MAP1_F
      ULLWORD-RES-MAG-V1.0/GEOMETRY and
      https://pds-ppi.igpp.ucla.edu/search/view/?f=yes&id=pds://PPI/MGS-M-MAG-3-PREMAP
      _FULLWORD-RES-MAG-V1.0/GEOMETRY Low resolution.
      
      Static Spacecraft Field Range [static_b_pl_range]
      Static spacecraft fields are due to permanent magnetization, for example,
      magnets or magnetized objects.
      
      Static Spacecraft Field X [static_bx_lpl]
      Static spacecraft field in payload X coordinates (this has been removed from the
      measured field to compensate for spacecraft fields); see sc_mod.ker at
      https://pds-ppi.igpp.ucla.edu/search/view/?f=yes&id=pds://PPI/MGS-M-MAG-3-MAP1_F
      ULLWORD-RES-MAG-V1.0/GEOMETRY and
      https://pds-ppi.igpp.ucla.edu/search/view/?f=yes&id=pds://PPI/MGS-M-MAG-3-PREMAP
      _FULLWORD-RES-MAG-V1.0/GEOMETRY Low resolution.
      
      Static Spacecraft Field Y [static_by_lpl]
      
      
      Static Spacecraft Field Z [static_bz_lpl]
      
      
      Magnetic Field Range Planetocentric [b_range_lpc]
      Planetocentric, low resolution.
      
      Magnetic Field Range MSO [b_range_lss]
      Sun-state, ss, or MSO. Low resolution.
      
      Magnetic Field X Planetocentric [bx_lpc]
      Low resolution in planetocentric coordinates. Outboard.
      
      Magnetic Field X MSO [bx_lss]
      
      
      Magnetic Field Y Planetocentric [by_lpc]
      Low resolution in planetocentric coordinates. Outboard.
      
      Magnetic Field Y MSO [by_lss]
      Low resolution in sun-state or MSO coordinates. Outboard.
      
      Magnetic Field Z Planetocentric [bz_lpc]
      Low resolution in planetocentric coordinates. Outboard.
      
      Magnetic Field Z MSO [bz_lss]
      Low resolution in sun-state or MSO coordinates. Outboard.
      
      RMS Range Planetocentric [rms_range_lpc]
      Low resolution, planetocentric.
      
      RMS Range MSO [rms_range_lss]
      Low resolution, sun-state/ss/MSO
      
      RMS X Planetocentric [rms_x_lpc]
      Root mean square of the outboard delta words (there are 23 delta words between
      fullwords, sampled at either 32, 16, or 8 per second depending on date rate
      allocation. Planetocentric, low resolution.
      
      RMS X MSO [rms_x_lss]
      
      
      RMS Y Planetocentric [rms_y_lpc]
      
      
      RMS Y MSO [rms_y_lss]
      Low resolution, sun-state/ss/MSO
      
      RMS Z Planetocentric [rms_z_lpc]
      Low resolution, planetocentric.
      
      RMS Z MSO [rms_z_lss]
      Low resolution, sun-state/ss/MSO
      
      Solar Array Negative Y Current [sa_neg_y_low]
      Solar array (-Y panel) current from sc engineering data base. A fill value of
      '-99' is used when the solar array currents are negative.'-999' is used as a
      fill value when the data is not available for the time.
      
      Total Solar Array Current [sa_total_low]
      Solar array output current (total) from sc engineering data base. A fill value
      of '-99' is used when the solar array currents are negative.'-999' is used as a
      fill value when the data is not available for the time.
      
      Solar Array Positive Y Current [sa_plus_y_low]
      Solar array (+Y panel) current from sc engineering data base. A fill value of
      '-99' is used when the solar array currents are negative. '-999' is used as a
      fill value when the data is not available for the time.
      
      Spacecraft Position X Planetocentric [sc_pos_x_lpc]
      Low resolution in planeocentric coordinates.
      
      Spacecraft Position X MSO [sc_pos_x_lss]
      Low resolution in sun-state or MSO coordinates.
      
      Spacecraft Position Y Planetocentric [sc_pos_y_lpc]
      Low resolution in planetocentric coordinates.
      
      Spacecraft Position Y MSO [sc_pos_y_lss]
      Low resolution in sun-state or MSO coordinates.
      
      Spacecraft Position Z Planetocentric [sc_pos_z_lpc]
      Low resolution in planetocentric coordinates.
      
      Spacecraft Position Z MSO [sc_pos_z_lss]
      Low resolution in sun-state or MSO coordinates.
      
      Magnetic Field Magnitude [magnitude]
      Magnitude calculated via the square root of the sum of the squares. Low
      resolution data.
      
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MMS1_ASPOC_SRVY_L2 (spase://NASA/NumericalData/MMS/1/ASPOC/Survey/Level2/PT1S)
Description
K. Torkar et al, Active Spacecraft Potential Control Investigation
Space Science Reviews, 2014, DOI: 10.1007/s11214-014-0049-3
Further information:
- http://www.iwf.oeaw.ac.at/en/research/near-earth-space/mms/ 
- http://mms.space.swri.edu/ 
Modification History
150224 Initial version
150831 Minor updates and fixes
160205 CDF file format guide compliant
 
  • Data Variable Descriptions
      ASPOC Ion Emission Current Sum, 1s resolution [mms1_aspoc_ionc]
      
      
      ASPOC Unit 1 Ion Emission Current, 1s resolution [mms1_asp1_ionc]
      
      
      ASPOC Unit 2 Ion Emission Current, 1s resolution [mms1_asp2_ionc]
      
      
      ASPOC Unit 1 Emitted Beam Energy, 1s resolution [mms1_asp1_energy]
      
      
      ASPOC Unit 2 Emitted Beam Energy, 1s resolution [mms1_asp2_energy]
      
      
      ASPOC Data Quality and Instrument Status, 1s resolution [mms1_aspoc_status]
      
      
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MMS1_DSP_FAST_L2_BPSD (spase://NASA/NumericalData/MMS/1/FIELDS/DSP/Fast/Level2/MagneticFieldPowerSpectralDensity/PT2S)
Description
BPSD is the low frequency B spectral density covering the frequency range of .2
to 6000 Hz.
 
  • Data Variable Descriptions
      SCM Axis 1 (X) component magnetic power spectral density [mms1_dsp_bpsd_scm1_fast_l2]
      
      
      SCM Axis 2 (Y, ~direction of S/C Z) component magnetic power spectral density [mms1_dsp_bpsd_scm2_fast_l2]
      
      
      SCM Axis 3 (Z) component magnetic power spectral density [mms1_dsp_bpsd_scm3_fast_l2]
      
      
      Omni-directional magnetic power spectral density: square root of the sum of the squares of 3 components [mms1_dsp_bpsd_omni_fast_l2]
      
      
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MMS1_DSP_FAST_L2_EPSD (spase://NASA/NumericalData/MMS/1/FIELDS/DSP/Fast/Level2/ElectricFieldPowerSpectralDensity/PT2S)
Description
EPSD combines the low frequency E spectral density covering the frequency range
of 1 to 8000 Hz and the  medium frequency E spectral density covering the
frequency range of .25 to 100 kHz.
 
  • Data Variable Descriptions
      null [mms1_dsp_epsd_x]
      
      
      null [mms1_dsp_epsd_y]
      
      
      null [mms1_dsp_epsd_z]
      
      
      null [mms1_dsp_epsd_omni]
      
      
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MMS1_DSP_SLOW_L2_BPSD (spase://NASA/NumericalData/MMS/1/FIELDS/DSP/Slow/Level2/MagneticFieldPowerSpectralDensity/PT16S)
Description
search coil magnetometer spectral density
 
  • Data Variable Descriptions
      SCM1 component magnetic power spectral density [mms1_dsp_bpsd_scm1_slow_l2]
      
      
      SCM2 component magnetic power spectral density - NO DATA in Slow Survey [mms1_dsp_bpsd_scm2_slow_l2]
      
      
      SCM3 component magnetic power spectral density [mms1_dsp_bpsd_scm3_slow_l2]
      
      
      Omni-directional magnetic power spectral density: square root of the sum of the squares of 2 components [mms1_dsp_bpsd_omni_slow_l2]
      
      
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MMS1_DSP_SLOW_L2_EPSD (spase://NASA/NumericalData/MMS/1/FIELDS/DSP/Slow/Level2/ElectricFieldPowerSpectralDensity/PT16S)
Description
electric spectral density
 
  • Data Variable Descriptions
      null [mms1_dsp_epsd_x]
      
      
      null [mms1_dsp_epsd_y]
      
      
      null [mms1_dsp_epsd_z]
      
      
      null [mms1_dsp_epsd_omni]
      
      
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MMS1_EDI_BRST_L2_AMB (spase://NASA/NumericalData/MMS/1/FIELDS/EDI/Burst/Level2/ElectronFluxAmbient/ProjectionMethod1/PT0.0009765625S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - Original version.
v1.0.0 - Include trajectory vectors and optics state.
v1.1.0 - Update metadata: counts -> flux.
v1.2.0 - Added flux error.
v1.3.0 - Trajectory vector errors are now deltas.
v1.4.0 - Fixed dead-time correction and error values.
v1.5.0 - Factor of 2 for accumulation time & 2 for abscal factor in srvy mode.
v1.6.0 - No factor of 2 for accumulation time in srvy mode.
v2.0.0 - Reduced file size with scalar errors. Update metadata.
v2.1.0 - Correct fill value for fluxes.
v3.0.0 - Omni-directional error for trajectories. Y-Version linked to cal file.
Single epoch for counts.
v4.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
 
  • Data Variable Descriptions
      Optics state [mms1_edi_optics_state_brst_l2]
      
      
      ---> GDU1 energy [mms1_edi_energy_gdu1_brst_l2]
      
      
      ---> GDU2 energy [mms1_edi_energy_gdu2_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-1 0PA [mms1_edi_flux1_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-1 0PA [mms1_edi_flux1_0_brst_l2_noerr]
      
      
      ---> Error for flux1 0-degree pitch angle electron flux. [mms1_edi_flux1_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-2 0PA [mms1_edi_flux2_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-2 0PA [mms1_edi_flux2_0_brst_l2_noerr]
      
      
      ---> Error for flux2 0-degree pitch angle electron flux. [mms1_edi_flux2_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-3 0PA [mms1_edi_flux3_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-3 0PA [mms1_edi_flux3_0_brst_l2_noerr]
      
      
      ---> Error for flux3 0-degree pitch angle electron flux. [mms1_edi_flux3_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-4 0PA [mms1_edi_flux4_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-4 0PA [mms1_edi_flux4_0_brst_l2_noerr]
      
      
      ---> Error for flux4 0-degree pitch angle electron flux. [mms1_edi_flux4_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-1 180PA [mms1_edi_flux1_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-1 180PA [mms1_edi_flux1_180_brst_l2_noerr]
      
      
      ---> Error for flux1 180-degree pitch angle electron flux. [mms1_edi_flux1_180_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by traj2 180PA [mms1_edi_flux2_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-2 180PA [mms1_edi_flux2_180_brst_l2_noerr]
      
      
      ---> Error for flux2 180-degree pitch angle electron flux. [mms1_edi_flux2_180_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by traj3 180PA [mms1_edi_flux3_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-3 180PA [mms1_edi_flux3_180_brst_l2_noerr]
      
      
      ---> Error for flux3 180-degree pitch angle electron flux. [mms1_edi_flux3_180_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by traj4 180PA [mms1_edi_flux4_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-4 180PA [mms1_edi_flux4_180_brst_l2_noerr]
      
      
      ---> Error for flux4 180-degree pitch angle electron flux. [mms1_edi_flux4_180_delta_brst_l2]
      
      
      Trajectory of flux1 0-degree pitch angle electrons in GSE coordinates. [mms1_edi_traj1_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 0-degree pitch angle electrons in GSE coordinates. [mms1_edi_traj2_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 0-degree pitch angle electrons in GSE coordinates. [mms1_edi_traj3_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 0-degree pitch angle electrons in GSE coordinates. [mms1_edi_traj4_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of flux1 180-degree pitch angle electrons in GSE coordinates. [mms1_edi_traj1_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 180-degree pitch angle electrons in GSE coordinates. [mms1_edi_traj2_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 180-degree pitch angle electrons in GSE coordinates. [mms1_edi_traj3_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 180-degree pitch angle electrons in GSE coordinates. [mms1_edi_traj4_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj1_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 0-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj2_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 0-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj3_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 0-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj4_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj1_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 180-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj2_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 180-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj3_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 180-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj4_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms1_edi_traj1_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms1_edi_traj2_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms1_edi_traj3_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms1_edi_traj4_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms1_edi_traj1_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms1_edi_traj2_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms1_edi_traj3_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms1_edi_traj4_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS1_EDI_BRST_L2_AMB-PM2 (spase://NASA/NumericalData/MMS/1/FIELDS/EDI/Burst/Level2/AmbientElectronFlux/ProjectionMethod2/PT0.0009765625S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v1.0.0 - Original version.
v1.1.0 - Correct fill value for fluxes.
v2.0.0 - Omni-directional error for trajectories. Y-Version linked to cal file.
Single epoch for counts.
v3.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
v4.0.0 - Each trajectory has its own LABL_PTR_1 variable.
 
  • Data Variable Descriptions
      Optics state [mms1_edi_optics_state_brst_l2]
      
      
      ---> GDU1 energy [mms1_edi_energy_gdu1_brst_l2]
      
      
      ---> GDU2 energy [mms1_edi_energy_gdu2_brst_l2]
      
      
      Field-aligned electron flux from channel 1 of both GDUs [mms1_edi_flux1_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 1 of both GDUs [mms1_edi_flux1_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 1 of both GDUs. [mms1_edi_flux1_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 1 of both GDUs [mms1_edi_flux1_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 1 of both GDUs [mms1_edi_flux1_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 1 of both GDUs. [mms1_edi_flux1_180_delta_brst_l2]
      
      
      Field-aligned electron flux from channel 2 of both GDUs [mms1_edi_flux2_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 2 of both GDUs [mms1_edi_flux2_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 2 of both GDUs. [mms1_edi_flux2_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 2 of both GDUs [mms1_edi_flux2_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 2 of both GDUs [mms1_edi_flux2_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 2 of both GDUs. [mms1_edi_flux2_180_delta_brst_l2]
      
      
      Field-aligned electron flux from channel 3 of both GDUs [mms1_edi_flux3_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 3 of both GDUs [mms1_edi_flux3_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 3 of both GDUs. [mms1_edi_flux3_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 3 of both GDUs [mms1_edi_flux3_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 3 of both GDUs [mms1_edi_flux3_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 3 of both GDUs. [mms1_edi_flux3_180_delta_brst_l2]
      
      
      Field-aligned electron flux from channel 4 of both GDUs [mms1_edi_flux4_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 4 of both GDUs [mms1_edi_flux4_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 4 of both GDUs. [mms1_edi_flux4_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 4 of both GDUs [mms1_edi_flux4_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 4 of both GDUs [mms1_edi_flux4_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 4 of both GDUs. [mms1_edi_flux4_180_delta_brst_l2]
      
      
      Trajectory of field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms1_edi_traj1_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms1_edi_traj1_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 1 of both GDUs in GSE coordinates. [mms1_edi_traj1_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 1 of both GDUs, in GSE coordinates. [mms1_edi_traj1_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms1_edi_traj2_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms1_edi_traj2_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 2 of both GDUs in GSE coordinates. [mms1_edi_traj2_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 2 of both GDUs, in GSE coordinates. [mms1_edi_traj2_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms1_edi_traj3_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms1_edi_traj3_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 3 of both GDUs in GSE coordinates. [mms1_edi_traj3_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 3 of both GDUs, in GSE coordinates. [mms1_edi_traj3_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms1_edi_traj4_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms1_edi_traj4_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 4 of both GDUs in GSE coordinates. [mms1_edi_traj4_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 4 of both GDUs, in GSE coordinates. [mms1_edi_traj4_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj1_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj1_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS1_EDI_BRST_L2_EFIELD (spase://NASA/NumericalData/MMS/1/FIELDS/EDI/Burst/Level2/ElectricField/PT0.0009765625S)
Description
EDI electric field data. Instrument papers for EDI can be found at:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7
Modification History
v1.0.0 - First version. TRI-TOF selection based on smallest error.
v1.1.0 - TRI-TOF merged by weighted average.
v1.2.0 - Fixed t_delta_plus/minus CDF_type.
v1.3.0 - Fixed Fixed vdrift SI conversion.
v1.4.0 - Fixed data duplication caused by multiple l2pre file locations.
v1.5.0 - Inplemented baseline*beams*Bmag filter for triangulation.
v1.6.0 - Inplemented null files for no or low quality data.
 
  • Data Variable Descriptions
      ExB drift velocity in DSL coordinates. [mms1_edi_vdrift_dsl_brst_l2]
      
      
      ---> ExB drift velocity in DSL coordinates (no error bars) [mms1_edi_vdrift_dsl_brst_l2_noerr]
      
      
      ExB drift velocity in GSE coordinates. [mms1_edi_vdrift_gse_brst_l2]
      
      
      ---> ExB drift velocity in GSE coordinates (no error bars) [mms1_edi_vdrift_gse_brst_l2_noerr]
      
      
      ExB drift velocity in GSM coordinates. [mms1_edi_vdrift_gsm_brst_l2]
      
      
      ---> ExB drift velocity in GSM coordinates (no error bars) [mms1_edi_vdrift_gsm_brst_l2_noerr]
      
      
      Electric field in DSL coordinates. [mms1_edi_e_dsl_brst_l2]
      
      
      ---> Electric field in DSL coordinates (no error bars) [mms1_edi_e_dsl_brst_l2_noerr]
      
      
      Electric field in GSE coordinates. [mms1_edi_e_gse_brst_l2]
      
      
      ---> Electric field in GSE coordinates (no error bars) [mms1_edi_e_gse_brst_l2_noerr]
      
      
      Electric field in GSM coordinates. [mms1_edi_e_gsm_brst_l2]
      
      
      ---> Electric field in GSM coordinates (no error bars) [mms1_edi_e_gsm_brst_l2_noerr]
      
      
      Weighted use of TRI method in L2 results. [mms1_edi_tri_weight_brst_l2]
      
      
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MMS1_EDI_BRST_L2_Q0 (spase://NASA/NumericalData/MMS/1/FIELDS/EDI/Burst/Level2/QualityZero/PT0.0078125S)
Description
EDI Q0 data. The EDI instrument paper and data products guidescan be found at
the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - First version.
v0.0.1 - Filled energy variables.
v0.0.2 - Energy written properly.
v1.0.0 - Update variable names.
v1.1.0 - Added optics state.
v2.0.0 - Added electron trajectories.
v2.1.0 - Deltas on trajectory vectors are now deltas.
v3.0.0 - Reduced file size with scalar errors. Add VAR_NOTES.
v3.1.0 - Fixed optics datatype.
v4.0.0 - Removed unused Epoch variable.
v5.0.0 - Trajectories are provided in DBCS coordinates.
 
  • Data Variable Descriptions
      Optics state [mms1_edi_optics_state_brst_l2]
      
      
      ---> GDU1 energy [mms1_edi_energy_gdu1_brst_l2]
      
      
      ---> GDU2 energy [mms1_edi_energy_gdu2_brst_l2]
      
      
      GDU1 quality 0 counts. [mms1_edi_counts_gdu1_brst_l2]
      Q0 data consists of raw electron counts. The error at any one time is the
      square-root of the counts. Note that there may be contamination from the EDI
      electron beams. See the data products guide or contact an EDI team member to
      learn about beam contamination.
      
      GDU2 quality 0 counts. [mms1_edi_counts_gdu2_brst_l2]
      
      
      GDU1 electron incident trajectory vectors in spherical BCS coordinates. [mms1_edi_traj_bcs_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical BCS coordinates. [mms1_edi_traj_bcs_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical DBCS coordinates. [mms1_edi_traj_dbcs_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical DBCS coordinates. [mms1_edi_traj_dbcs_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSE coordinates. [mms1_edi_traj_gse_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSE coordinates. [mms1_edi_traj_gse_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSM coordinates. [mms1_edi_traj_gsm_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSM coordinates. [mms1_edi_traj_gsm_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS1_EDI_SRVY_L2_AMB (spase://NASA/NumericalData/MMS/1/FIELDS/EDI/Survey/Level2/ElectronFluxAmbient/ProjectionMethod1/PT0.03125S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - Original version.
v1.0.0 - Include trajectory vectors and optics state.
v1.1.0 - Update metadata: counts -> flux.
v1.2.0 - Added flux error.
v1.3.0 - Trajectory vector errors are now deltas.
v1.4.0 - Fixed dead-time correction and error values.
v1.5.0 - Factor of 2 for accumulation time & 2 for abscal factor in srvy mode.
v1.6.0 - No factor of 2 for accumulation time in srvy mode.
v2.0.0 - Reduced file size with scalar errors. Update metadata.
v2.1.0 - Correct fill value for fluxes.
v3.0.0 - Omni-directional error for trajectories. Correct time deltas. Y-Version
linked to cal file. Single epoch for counts.
v4.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
 
  • Data Variable Descriptions
      Optics state [mms1_edi_optics_state_srvy_l2]
      
      
      ---> GDU1 energy [mms1_edi_energy_gdu1_srvy_l2]
      
      
      ---> GDU2 energy [mms1_edi_energy_gdu2_srvy_l2]
      
      
      Field-aligned electron flux from both GDUs [mms1_edi_flux1_0_srvy_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from both GDUs [mms1_edi_flux1_0_srvy_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from both GDUs. [mms1_edi_flux1_0_delta_srvy_l2]
      
      
      Anti-field-aligned electron flux from both GDUs [mms1_edi_flux1_180_srvy_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from both GDUs [mms1_edi_flux1_180_srvy_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from both GDUs. [mms1_edi_flux1_180_delta_srvy_l2]
      
      
      Trajectory of field-aligned electrons from both GDUs in DBCS coordinates. [mms1_edi_traj1_dbcs_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs in DBCS coordinates. [mms1_edi_traj1_dbcs_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from both GDUs in GSE coordinates. [mms1_edi_traj1_gse_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs, in GSE coordinates. [mms1_edi_traj1_gse_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj1_gsm_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj1_gsm_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS1_EDI_SRVY_L2_AMB-PM2 (spase://NASA/NumericalData/MMS/1/FIELDS/EDI/Survey/Level2/ElectronFluxAmbient/ProjectionMethod2/PT0.03125S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v1.0.0 - Original version.
v1.1.0 - Correct fill value for fluxes.
v2.0.0 - Omni-directional error for trajectories. Y-Version linked to cal file.
Single epoch for counts.
v3.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
v4.0.0 - Each trajectory has its own LABL_PTR_1 variable.
 
  • Data Variable Descriptions
      Optics state [mms1_edi_optics_state_srvy_l2]
      
      
      ---> GDU1 energy [mms1_edi_energy_gdu1_srvy_l2]
      
      
      ---> GDU2 energy [mms1_edi_energy_gdu2_srvy_l2]
      
      
      Field-aligned electron flux from both GDUs [mms1_edi_flux1_0_srvy_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from both GDUs [mms1_edi_flux1_0_srvy_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from both GDUs. [mms1_edi_flux1_0_delta_srvy_l2]
      
      
      Anti-field-aligned electron flux from both GDUs [mms1_edi_flux1_180_srvy_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from both GDUs [mms1_edi_flux1_180_srvy_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from both GDUs. [mms1_edi_flux1_180_delta_srvy_l2]
      
      
      Trajectory of field-aligned electrons from both GDUs in DBCS coordinates. [mms1_edi_traj1_dbcs_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs in DBCS coordinates. [mms1_edi_traj1_dbcs_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from both GDUs in GSE coordinates. [mms1_edi_traj1_gse_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs, in GSE coordinates. [mms1_edi_traj1_gse_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj1_gsm_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms1_edi_traj1_gsm_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS1_EDI_SRVY_L2_EFIELD (spase://NASA/NumericalData/MMS/1/FIELDS/EDI/Survey/Level2/ElectricField/PT5S)
Description
EDI electric field data. Instrument papers for EDI can be found at:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7
Modification History
v1.0.0 - First version. TRI-TOF selection based on smallest error.
v1.1.0 - TRI-TOF merged by weighted average.
v1.2.0 - Fixed t_delta_plus/minus CDF_type.
v1.3.0 - Fixed Fixed vdrift SI conversion.
v1.4.0 - Fixed data duplication caused by multiple l2pre file locations.
v1.5.0 - Inplemented baseline*beams*Bmag filter for triangulation.
v1.6.0 - Inplemented null files for no or low quality data.
 
  • Data Variable Descriptions
      ExB drift velocity in DSL coordinates. [mms1_edi_vdrift_dsl_srvy_l2]
      
      
      ---> ExB drift velocity in DSL coordinates (no error bars) [mms1_edi_vdrift_dsl_srvy_l2_noerr]
      
      
      ExB drift velocity in GSE coordinates. [mms1_edi_vdrift_gse_srvy_l2]
      
      
      ---> ExB drift velocity in GSE coordinates (no error bars) [mms1_edi_vdrift_gse_srvy_l2_noerr]
      
      
      ExB drift velocity in GSM coordinates. [mms1_edi_vdrift_gsm_srvy_l2]
      
      
      ---> ExB drift velocity in GSM coordinates (no error bars) [mms1_edi_vdrift_gsm_srvy_l2_noerr]
      
      
      Electric field in DSL coordinates. [mms1_edi_e_dsl_srvy_l2]
      
      
      ---> Electric field in DSL coordinates (no error bars) [mms1_edi_e_dsl_srvy_l2_noerr]
      
      
      Electric field in GSE coordinates. [mms1_edi_e_gse_srvy_l2]
      
      
      ---> Electric field in GSE coordinates (no error bars) [mms1_edi_e_gse_srvy_l2_noerr]
      
      
      Electric field in GSM coordinates. [mms1_edi_e_gsm_srvy_l2]
      
      
      ---> Electric field in GSM coordinates (no error bars) [mms1_edi_e_gsm_srvy_l2_noerr]
      
      
      Weighted use of TRI method in L2 results. [mms1_edi_tri_weight_srvy_l2]
      
      
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MMS1_EDI_SRVY_L2_Q0 (spase://NASA/NumericalData/MMS/1/FIELDS/EDI/Survey/Level2/QualityZero/PT0.125S)
Description
EDI Q0 data. The EDI instrument paper and data products guidescan be found at
the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - First version.
v0.0.1 - Filled energy variables.
v0.0.2 - Energy written properly.
v1.0.0 - Update variable names.
v1.1.0 - Added optics state.
v2.0.0 - Added electron trajectories.
v2.1.0 - Deltas on trajectory vectors are now deltas.
v3.0.0 - Reduced file size with scalar errors. Add VAR_NOTES.
v4.0.0 - Removed unused Epoch variable.
v5.0.0 - Trajectories are provided in DBCS coordinates.
 
  • Data Variable Descriptions
      Optics state [mms1_edi_optics_state_srvy_l2]
      
      
      ---> GDU1 energy [mms1_edi_energy_gdu1_srvy_l2]
      
      
      ---> GDU2 energy [mms1_edi_energy_gdu2_srvy_l2]
      
      
      GDU1 quality 0 counts. [mms1_edi_counts_gdu1_srvy_l2]
      Q0 data consists of raw electron counts. The error at any one time is the
      square-root of the counts. Note that there may be contamination from the EDI
      electron beams. See the data products guide or contact an EDI team member to
      learn about beam contamination.
      
      GDU2 quality 0 counts. [mms1_edi_counts_gdu2_srvy_l2]
      
      
      GDU1 electron incident trajectory vectors in spherical BCS coordinates. [mms1_edi_traj_bcs_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical BCS coordinates. [mms1_edi_traj_bcs_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical DBCS coordinates. [mms1_edi_traj_dbcs_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical DBCS coordinates. [mms1_edi_traj_dbcs_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSE coordinates. [mms1_edi_traj_gse_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSE coordinates. [mms1_edi_traj_gse_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSM coordinates. [mms1_edi_traj_gsm_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSM coordinates. [mms1_edi_traj_gsm_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS1_EDP_BRST_L2_DCE (spase://NASA/NumericalData/MMS/1/FIELDS/EDP/Burst/Level2/DCElectricField/PT0.0001220703125S)
Description
http://mms.gsfc.nasa.gov/
Modification History
V.0. Initial release.
 
  • Data Variable Descriptions
      L2 DC E Field (GSE coords) calibrated for SDP and ADP, all flag values included [mms1_edp_dce_gse_brst_l2]
      
      
      L2 DC E Field (DSL coords) calibrated for SDP and ADP, all flag values included [mms1_edp_dce_dsl_brst_l2]
      
      
      L2 DC E Parallel Field calibrated for SDP and ADP [mms1_edp_dce_par_epar_brst_l2]
      
      
      Quality indicator (3 good), (2 ok data, use with some caution), (1 bad data, use with caution), (0 Really bad data or no data at all) [mms1_edp_quality_brst_l2]
      
      
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MMS1_EDP_BRST_L2_HMFE (spase://NASA/NumericalData/MMS/1/FIELDS/EDP/Burst/Level2Pre/HMFE/PT0.00001525878906S)
Description
 d
 
  • Data Variable Descriptions
      DC E Field calibrated for SDP and ADP [mms1_edp_hmfe_dsl_brst_l2]
      
      
      DC E parallel Field from calibrated SDP and ADP [mms1_edp_hmfe_par_epar_brst_l2]
      
      
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MMS1_EDP_BRST_L2_SCPOT doi:10.48322/7t5y-eq71
Proper citations should include the "Accessed on date" in the form .
Description
http://mms.gsfc.nasa.gov/
The full name of PI affiliations: SWRI - Southwest Research Institute. LASP -
Laboratory for Atmospheric and Space Physics. KTH - Kungliga Tekniska Hogskolan
(Swedish Royal Institute of Technology). 
Modification History
V.0. Initial release.
V.1. QL (v1.0.z), SCPOT (v1.0.z), L2A (v0.1.z) now uses ASPOC srvy l2 and
DEFATT, if these are available. Brst QL uses intermediate L2A file from Fast
mode for delta offsets. Bitmask changed to uint16 and Quality to uint8.
V.2. SCPOT (v2.0.z), L2A (v1.0.z) now uses variable names in accordance with new
recommended standard for FIELDS, All products change shortening factor to 1.25
on SDP, offsets applied indicated by GlobalAttribute Calibration_file.
V.2. L2a (v2.0.z), QL (v1.6.z) now try to remove solar wind wake which
previously left a clear sinusodial signal in the data.
V.3. L2a (v3.0.z) Slow Mode probe Gain set to 1.0 when orbital radius less than
5 RE (1.25 otherwise), L2pre (v2.0.z) DSL offsets removed from field is now
included in the file as the Slow mode is dependent on scpot product (Fast/Brst
is simply based on offset in Calibration_file).
 
  • Data Variable Descriptions
      Spacecraft potential [mms1_edp_scpot_brst_l2]
      
      
      Probe to spacecraft potential, averaged [mms1_edp_psp_brst_l2]
      
      
      Probe to spacecraft potential, individual probes [mms1_edp_dcv_brst_l2]
      
      
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MMS1_EDP_FAST_L2_DCE (spase://NASA/NumericalData/MMS/1/FIELDS/EDP/Fast/Level2/DCElectricField/PT0.03125S)
Description
http://mms.gsfc.nasa.gov/
Modification History
V.0. Initial release.
 
  • Data Variable Descriptions
      L2 DC E Field (GSE coords) calibrated for SDP and ADP, all flag values included [mms1_edp_dce_gse_fast_l2]
      
      
      L2 DC E Field (DSL coords) calibrated for SDP and ADP, all flag values included [mms1_edp_dce_dsl_fast_l2]
      
      
      L2 DC E Parallel Field with error calibrated for SDP and ADP [mms1_edp_dce_par_epar_fast_l2]
      
      
      Approximate DC E field error derived from SDP (quality and bitmask) and ADP (residue) [mms1_edp_dce_err_fast_l2]
      
      
      Quality indicator (3 good), (2 ok data, use with some caution), (1 bad data, use with caution), (0 Really bad data or no data at all) [mms1_edp_quality_fast_l2]
      
      
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MMS1_EDP_FAST_L2_SCPOT doi:10.48322/jjsp-6g51
Proper citations should include the "Accessed on date" in the form .
Description
http://mms.gsfc.nasa.gov/
The full name of PI affiliations: SWRI - Southwest Research Institute. LASP -
Laboratory for Atmospheric and Space Physics. KTH - Kungliga Tekniska Hogskolan
(Swedish Royal Institute of Technology). 
Modification History
V.0. Initial release.
V.1. QL (v1.0.z), SCPOT (v1.0.z), L2A (v0.1.z) now uses ASPOC srvy l2 and
DEFATT, if these are available. Brst QL uses intermediate L2A file from Fast
mode for delta offsets. Bitmask changed to uint16 and Quality to uint8.
V.2. SCPOT (v2.0.z), L2A (v1.0.z) now uses variable names in accordance with new
recommended standard for FIELDS, All products change shortening factor to 1.25
on SDP, offsets applied indicated by GlobalAttribute Calibration_file.
V.2. L2a (v2.0.z), QL (v1.6.z) now try to remove solar wind wake which
previously left a clear sinusodial signal in the data.
V.3. L2a (v3.0.z) Slow Mode probe Gain set to 1.0 when orbital radius less than
5 RE (1.25 otherwise), L2pre (v2.0.z) DSL offsets removed from field is now
included in the file as the Slow mode is dependent on scpot product (Fast/Brst
is simply based on offset in Calibration_file).
 
  • Data Variable Descriptions
      Spacecraft potential [mms1_edp_scpot_fast_l2]
      
      
      Probe to spacecraft potential, averaged [mms1_edp_psp_fast_l2]
      
      
      Probe to spacecraft potential, individual probes [mms1_edp_dcv_fast_l2]
      
      
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MMS1_EDP_SLOW_L2_DCE (spase://NASA/NumericalData/MMS/1/FIELDS/EDP/Slow/Level2/DCElectricField/PT0.125S)
Description
http://mms.gsfc.nasa.gov/
Modification History
V.0. Initial release.
 
  • Data Variable Descriptions
      L2 DC E Field (GSE coords) calibrated for SDP and ADP, all flag values included [mms1_edp_dce_gse_slow_l2]
      
      
      L2 DC E Field (DSL coords) calibrated for SDP and ADP, all flag values included [mms1_edp_dce_dsl_slow_l2]
      
      
      L2 DC E Parallel Field with error calibrated for SDP and ADP [mms1_edp_dce_par_epar_slow_l2]
      
      
      Approximate DC E field error derived from SDP (quality and bitmask) and ADP (residue) [mms1_edp_dce_err_slow_l2]
      
      
      Quality indicator (3 good), (2 ok data, use with some caution), (1 bad data, use with caution), (0 Really bad data or no data at all) [mms1_edp_quality_slow_l2]
      
      
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MMS1_EDP_SLOW_L2_SCPOT doi:10.48322/5t77-ka57
Proper citations should include the "Accessed on date" in the form .
Description
http://mms.gsfc.nasa.gov/
The full name of PI affiliations: SWRI - Southwest Research Institute. LASP -
Laboratory for Atmospheric and Space Physics. KTH - Kungliga Tekniska Hogskolan
(Swedish Royal Institute of Technology). 
Modification History
V.0. Initial release.
V.1. QL (v1.0.z), SCPOT (v1.0.z), L2A (v0.1.z) now uses ASPOC srvy l2 and
DEFATT, if these are available. Brst QL uses intermediate L2A file from Fast
mode for delta offsets. Bitmask changed to uint16 and Quality to uint8.
V.2. SCPOT (v2.0.z), L2A (v1.0.z) now uses variable names in accordance with new
recommended standard for FIELDS, All products change shortening factor to 1.25
on SDP, offsets applied indicated by GlobalAttribute Calibration_file.
V.2. L2a (v2.0.z), QL (v1.6.z) now try to remove solar wind wake which
previously left a clear sinusodial signal in the data.
V.3. L2a (v3.0.z) Slow Mode probe Gain set to 1.0 when orbital radius less than
5 RE (1.25 otherwise), L2pre (v2.0.z) DSL offsets removed from field is now
included in the file as the Slow mode is dependent on scpot product (Fast/Brst
is simply based on offset in Calibration_file).
 
  • Data Variable Descriptions
      Spacecraft potential [mms1_edp_scpot_slow_l2]
      
      
      Probe to spacecraft potential, averaged [mms1_edp_psp_slow_l2]
      
      
      Probe to spacecraft potential, individual probes [mms1_edp_dcv_slow_l2]
      
      
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MMS1_EDP_SRVY_L2_HFESP (spase://NASA/NumericalData/MMS/1/FIELDS/EDP/Survey/Level2/HighFrequencyElectricFieldSpectra/PT16S)
Description
 AC Electric Field
 
  • Data Variable Descriptions
      HF ACE E Field Spectral Density [mms1_edp_hfesp_srvy_l2]
      
      
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MMS1_EPD-EIS_BRST_L2_EXTOF (spase://NASA/NumericalData/MMS/1/EnergeticParticleDetector/EIS/Burst/Level2/EnergyByTimeOfFlight/PT0.605S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms1_epd_eis_brst_l2_extof_duration]
      
      
      ---> Instrument Deadtime [mms1_epd_eis_brst_l2_extof_deadtime]
      
      
      ---> Instrument Large Pixel in Use [mms1_epd_eis_brst_l2_extof_largepixel]
      
      
      ---> Spin [mms1_epd_eis_brst_l2_extof_spin]
      
      
      ---> Sector [mms1_epd_eis_brst_l2_extof_sector]
      
      
      ---> Quality Word [mms1_epd_eis_brst_l2_extof_quality]
      
      
      MMS1 ExTOF-Burst proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_extof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms1_epd_eis_brst_l2_extof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms1_epd_eis_brst_l2_extof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms1_epd_eis_brst_l2_extof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms1_epd_eis_brst_l2_extof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms1_epd_eis_brst_l2_extof_proton_P6_counts_t5]
      
      
      MMS1 ExTOF-Burst proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_extof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms1_epd_eis_brst_l2_extof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms1_epd_eis_brst_l2_extof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms1_epd_eis_brst_l2_extof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms1_epd_eis_brst_l2_extof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms1_epd_eis_brst_l2_extof_proton_P6_cps_t5]
      
      
      MMS1 ExTOF-Burst proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_extof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms1_epd_eis_brst_l2_extof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms1_epd_eis_brst_l2_extof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms1_epd_eis_brst_l2_extof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms1_epd_eis_brst_l2_extof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms1_epd_eis_brst_l2_extof_proton_P6_flux_t5]
      
      
      MMS1 ExTOF-Burst helium_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_extof_helium_P6_counts_t0]
      
      
      ---> helium_P6_counts_t1 [mms1_epd_eis_brst_l2_extof_helium_P6_counts_t1]
      
      
      ---> helium_P6_counts_t2 [mms1_epd_eis_brst_l2_extof_helium_P6_counts_t2]
      
      
      ---> helium_P6_counts_t3 [mms1_epd_eis_brst_l2_extof_helium_P6_counts_t3]
      
      
      ---> helium_P6_counts_t4 [mms1_epd_eis_brst_l2_extof_helium_P6_counts_t4]
      
      
      ---> helium_P6_counts_t5 [mms1_epd_eis_brst_l2_extof_helium_P6_counts_t5]
      
      
      MMS1 ExTOF-Burst helium_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_extof_helium_P6_cps_t0]
      
      
      ---> helium_P6_cps_t1 [mms1_epd_eis_brst_l2_extof_helium_P6_cps_t1]
      
      
      ---> helium_P6_cps_t2 [mms1_epd_eis_brst_l2_extof_helium_P6_cps_t2]
      
      
      ---> helium_P6_cps_t3 [mms1_epd_eis_brst_l2_extof_helium_P6_cps_t3]
      
      
      ---> helium_P6_cps_t4 [mms1_epd_eis_brst_l2_extof_helium_P6_cps_t4]
      
      
      ---> helium_P6_cps_t5 [mms1_epd_eis_brst_l2_extof_helium_P6_cps_t5]
      
      
      MMS1 ExTOF-Burst helium_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_extof_helium_P6_flux_t0]
      
      
      ---> helium_P6_flux_t1 [mms1_epd_eis_brst_l2_extof_helium_P6_flux_t1]
      
      
      ---> helium_P6_flux_t2 [mms1_epd_eis_brst_l2_extof_helium_P6_flux_t2]
      
      
      ---> helium_P6_flux_t3 [mms1_epd_eis_brst_l2_extof_helium_P6_flux_t3]
      
      
      ---> helium_P6_flux_t4 [mms1_epd_eis_brst_l2_extof_helium_P6_flux_t4]
      
      
      ---> helium_P6_flux_t5 [mms1_epd_eis_brst_l2_extof_helium_P6_flux_t5]
      
      
      MMS1 ExTOF-Burst oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_extof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms1_epd_eis_brst_l2_extof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms1_epd_eis_brst_l2_extof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms1_epd_eis_brst_l2_extof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms1_epd_eis_brst_l2_extof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms1_epd_eis_brst_l2_extof_oxygen_P6_counts_t5]
      
      
      MMS1 ExTOF-Burst oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_extof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms1_epd_eis_brst_l2_extof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms1_epd_eis_brst_l2_extof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms1_epd_eis_brst_l2_extof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms1_epd_eis_brst_l2_extof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms1_epd_eis_brst_l2_extof_oxygen_P6_cps_t5]
      
      
      MMS1 ExTOF-Burst oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_extof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms1_epd_eis_brst_l2_extof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms1_epd_eis_brst_l2_extof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms1_epd_eis_brst_l2_extof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms1_epd_eis_brst_l2_extof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms1_epd_eis_brst_l2_extof_oxygen_P6_flux_t5]
      
      
      MMS1 ExTOF-Burst dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_extof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms1_epd_eis_brst_l2_extof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms1_epd_eis_brst_l2_extof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms1_epd_eis_brst_l2_extof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms1_epd_eis_brst_l2_extof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms1_epd_eis_brst_l2_extof_dump_P6_counts_t5]
      
      
      MMS1 ExTOF-Burst dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_extof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms1_epd_eis_brst_l2_extof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms1_epd_eis_brst_l2_extof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms1_epd_eis_brst_l2_extof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms1_epd_eis_brst_l2_extof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms1_epd_eis_brst_l2_extof_dump_P6_cps_t5]
      
      
      MMS1 ExTOF-Burst dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_extof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms1_epd_eis_brst_l2_extof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms1_epd_eis_brst_l2_extof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms1_epd_eis_brst_l2_extof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms1_epd_eis_brst_l2_extof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms1_epd_eis_brst_l2_extof_dump_P6_flux_t5]
      
      
      MMS1 ExTOF-Burst proton_P5_counts_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_extof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms1_epd_eis_brst_l2_extof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms1_epd_eis_brst_l2_extof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms1_epd_eis_brst_l2_extof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms1_epd_eis_brst_l2_extof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms1_epd_eis_brst_l2_extof_proton_P5_counts_t5]
      
      
      MMS1 ExTOF-Burst proton_P5_cps_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_extof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms1_epd_eis_brst_l2_extof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms1_epd_eis_brst_l2_extof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms1_epd_eis_brst_l2_extof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms1_epd_eis_brst_l2_extof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms1_epd_eis_brst_l2_extof_proton_P5_cps_t5]
      
      
      MMS1 ExTOF-Burst proton_P5_flux_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_extof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms1_epd_eis_brst_l2_extof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms1_epd_eis_brst_l2_extof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms1_epd_eis_brst_l2_extof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms1_epd_eis_brst_l2_extof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms1_epd_eis_brst_l2_extof_proton_P5_flux_t5]
      
      
      MMS1 ExTOF-Burst oxygen_P5_counts_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_extof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms1_epd_eis_brst_l2_extof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms1_epd_eis_brst_l2_extof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms1_epd_eis_brst_l2_extof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms1_epd_eis_brst_l2_extof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms1_epd_eis_brst_l2_extof_oxygen_P5_counts_t5]
      
      
      MMS1 ExTOF-Burst oxygen_P5_cps_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_extof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms1_epd_eis_brst_l2_extof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms1_epd_eis_brst_l2_extof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms1_epd_eis_brst_l2_extof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms1_epd_eis_brst_l2_extof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms1_epd_eis_brst_l2_extof_oxygen_P5_cps_t5]
      
      
      MMS1 ExTOF-Burst oxygen_P5_flux_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_extof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms1_epd_eis_brst_l2_extof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms1_epd_eis_brst_l2_extof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms1_epd_eis_brst_l2_extof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms1_epd_eis_brst_l2_extof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms1_epd_eis_brst_l2_extof_oxygen_P5_flux_t5]
      
      
      MMS1 ExTOF-Burst helium_P5_counts_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_extof_helium_P5_counts_t0]
      
      
      ---> helium_P5_counts_t1 [mms1_epd_eis_brst_l2_extof_helium_P5_counts_t1]
      
      
      ---> helium_P5_counts_t2 [mms1_epd_eis_brst_l2_extof_helium_P5_counts_t2]
      
      
      ---> helium_P5_counts_t3 [mms1_epd_eis_brst_l2_extof_helium_P5_counts_t3]
      
      
      ---> helium_P5_counts_t4 [mms1_epd_eis_brst_l2_extof_helium_P5_counts_t4]
      
      
      ---> helium_P5_counts_t5 [mms1_epd_eis_brst_l2_extof_helium_P5_counts_t5]
      
      
      MMS1 ExTOF-Burst helium_P5_cps_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_extof_helium_P5_cps_t0]
      
      
      ---> helium_P5_cps_t1 [mms1_epd_eis_brst_l2_extof_helium_P5_cps_t1]
      
      
      ---> helium_P5_cps_t2 [mms1_epd_eis_brst_l2_extof_helium_P5_cps_t2]
      
      
      ---> helium_P5_cps_t3 [mms1_epd_eis_brst_l2_extof_helium_P5_cps_t3]
      
      
      ---> helium_P5_cps_t4 [mms1_epd_eis_brst_l2_extof_helium_P5_cps_t4]
      
      
      ---> helium_P5_cps_t5 [mms1_epd_eis_brst_l2_extof_helium_P5_cps_t5]
      
      
      MMS1 ExTOF-Burst helium_P5_flux_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_extof_helium_P5_flux_t0]
      
      
      ---> helium_P5_flux_t1 [mms1_epd_eis_brst_l2_extof_helium_P5_flux_t1]
      
      
      ---> helium_P5_flux_t2 [mms1_epd_eis_brst_l2_extof_helium_P5_flux_t2]
      
      
      ---> helium_P5_flux_t3 [mms1_epd_eis_brst_l2_extof_helium_P5_flux_t3]
      
      
      ---> helium_P5_flux_t4 [mms1_epd_eis_brst_l2_extof_helium_P5_flux_t4]
      
      
      ---> helium_P5_flux_t5 [mms1_epd_eis_brst_l2_extof_helium_P5_flux_t5]
      
      
      MMS1 ExTOF-Burst proton_P4_counts_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_extof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms1_epd_eis_brst_l2_extof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms1_epd_eis_brst_l2_extof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms1_epd_eis_brst_l2_extof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms1_epd_eis_brst_l2_extof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms1_epd_eis_brst_l2_extof_proton_P4_counts_t5]
      
      
      MMS1 ExTOF-Burst proton_P4_cps_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_extof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms1_epd_eis_brst_l2_extof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms1_epd_eis_brst_l2_extof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms1_epd_eis_brst_l2_extof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms1_epd_eis_brst_l2_extof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms1_epd_eis_brst_l2_extof_proton_P4_cps_t5]
      
      
      MMS1 ExTOF-Burst proton_P4_flux_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_extof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms1_epd_eis_brst_l2_extof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms1_epd_eis_brst_l2_extof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms1_epd_eis_brst_l2_extof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms1_epd_eis_brst_l2_extof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms1_epd_eis_brst_l2_extof_proton_P4_flux_t5]
      
      
      MMS1 ExTOF-Burst alpha_P4_counts_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_extof_helium_P4_counts_t0]
      
      
      ---> alpha_P4_counts_t1 [mms1_epd_eis_brst_l2_extof_helium_P4_counts_t1]
      
      
      ---> alpha_P4_counts_t2 [mms1_epd_eis_brst_l2_extof_helium_P4_counts_t2]
      
      
      ---> alpha_P4_counts_t3 [mms1_epd_eis_brst_l2_extof_helium_P4_counts_t3]
      
      
      ---> alpha_P4_counts_t4 [mms1_epd_eis_brst_l2_extof_helium_P4_counts_t4]
      
      
      ---> alpha_P4_counts_t5 [mms1_epd_eis_brst_l2_extof_helium_P4_counts_t5]
      
      
      MMS1 ExTOF-Burst alpha_P4_cps_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_extof_helium_P4_cps_t0]
      
      
      ---> alpha_P4_cps_t1 [mms1_epd_eis_brst_l2_extof_helium_P4_cps_t1]
      
      
      ---> alpha_P4_cps_t2 [mms1_epd_eis_brst_l2_extof_helium_P4_cps_t2]
      
      
      ---> alpha_P4_cps_t3 [mms1_epd_eis_brst_l2_extof_helium_P4_cps_t3]
      
      
      ---> alpha_P4_cps_t4 [mms1_epd_eis_brst_l2_extof_helium_P4_cps_t4]
      
      
      ---> alpha_P4_cps_t5 [mms1_epd_eis_brst_l2_extof_helium_P4_cps_t5]
      
      
      MMS1 ExTOF-Burst alpha_P4_flux_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_extof_helium_P4_flux_t0]
      
      
      ---> alpha_P4_flux_t1 [mms1_epd_eis_brst_l2_extof_helium_P4_flux_t1]
      
      
      ---> alpha_P4_flux_t2 [mms1_epd_eis_brst_l2_extof_helium_P4_flux_t2]
      
      
      ---> alpha_P4_flux_t3 [mms1_epd_eis_brst_l2_extof_helium_P4_flux_t3]
      
      
      ---> alpha_P4_flux_t4 [mms1_epd_eis_brst_l2_extof_helium_P4_flux_t4]
      
      
      ---> alpha_P4_flux_t5 [mms1_epd_eis_brst_l2_extof_helium_P4_flux_t5]
      
      
      MMS1 ExTOF-Burst oxygen_P4_counts_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_extof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms1_epd_eis_brst_l2_extof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms1_epd_eis_brst_l2_extof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms1_epd_eis_brst_l2_extof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms1_epd_eis_brst_l2_extof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms1_epd_eis_brst_l2_extof_oxygen_P4_counts_t5]
      
      
      MMS1 ExTOF-Burst oxygen_P4_cps_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_extof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms1_epd_eis_brst_l2_extof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms1_epd_eis_brst_l2_extof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms1_epd_eis_brst_l2_extof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms1_epd_eis_brst_l2_extof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms1_epd_eis_brst_l2_extof_oxygen_P4_cps_t5]
      
      
      MMS1 ExTOF-Burst oxygen_P4_flux_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_extof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms1_epd_eis_brst_l2_extof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms1_epd_eis_brst_l2_extof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms1_epd_eis_brst_l2_extof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms1_epd_eis_brst_l2_extof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms1_epd_eis_brst_l2_extof_oxygen_P4_flux_t5]
      
      
      MMS1 ExTOF-Burst proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_extof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms1_epd_eis_brst_l2_extof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms1_epd_eis_brst_l2_extof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms1_epd_eis_brst_l2_extof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms1_epd_eis_brst_l2_extof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms1_epd_eis_brst_l2_extof_proton_P3_counts_t5]
      
      
      MMS1 ExTOF-Burst proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_extof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms1_epd_eis_brst_l2_extof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms1_epd_eis_brst_l2_extof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms1_epd_eis_brst_l2_extof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms1_epd_eis_brst_l2_extof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms1_epd_eis_brst_l2_extof_proton_P3_cps_t5]
      
      
      MMS1 ExTOF-Burst proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_extof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms1_epd_eis_brst_l2_extof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms1_epd_eis_brst_l2_extof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms1_epd_eis_brst_l2_extof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms1_epd_eis_brst_l2_extof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms1_epd_eis_brst_l2_extof_proton_P3_flux_t5]
      
      
      MMS1 ExTOF-Burst alpha_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_extof_helium_P3_counts_t0]
      
      
      ---> alpha_P3_counts_t1 [mms1_epd_eis_brst_l2_extof_helium_P3_counts_t1]
      
      
      ---> alpha_P3_counts_t2 [mms1_epd_eis_brst_l2_extof_helium_P3_counts_t2]
      
      
      ---> alpha_P3_counts_t3 [mms1_epd_eis_brst_l2_extof_helium_P3_counts_t3]
      
      
      ---> alpha_P3_counts_t4 [mms1_epd_eis_brst_l2_extof_helium_P3_counts_t4]
      
      
      ---> alpha_P3_counts_t5 [mms1_epd_eis_brst_l2_extof_helium_P3_counts_t5]
      
      
      MMS1 ExTOF-Burst alpha_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_extof_helium_P3_cps_t0]
      
      
      ---> alpha_P3_cps_t1 [mms1_epd_eis_brst_l2_extof_helium_P3_cps_t1]
      
      
      ---> alpha_P3_cps_t2 [mms1_epd_eis_brst_l2_extof_helium_P3_cps_t2]
      
      
      ---> alpha_P3_cps_t3 [mms1_epd_eis_brst_l2_extof_helium_P3_cps_t3]
      
      
      ---> alpha_P3_cps_t4 [mms1_epd_eis_brst_l2_extof_helium_P3_cps_t4]
      
      
      ---> alpha_P3_cps_t5 [mms1_epd_eis_brst_l2_extof_helium_P3_cps_t5]
      
      
      MMS1 ExTOF-Burst alpha_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_extof_helium_P3_flux_t0]
      
      
      ---> alpha_P3_flux_t1 [mms1_epd_eis_brst_l2_extof_helium_P3_flux_t1]
      
      
      ---> alpha_P3_flux_t2 [mms1_epd_eis_brst_l2_extof_helium_P3_flux_t2]
      
      
      ---> alpha_P3_flux_t3 [mms1_epd_eis_brst_l2_extof_helium_P3_flux_t3]
      
      
      ---> alpha_P3_flux_t4 [mms1_epd_eis_brst_l2_extof_helium_P3_flux_t4]
      
      
      ---> alpha_P3_flux_t5 [mms1_epd_eis_brst_l2_extof_helium_P3_flux_t5]
      
      
      MMS1 ExTOF-Burst oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_extof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms1_epd_eis_brst_l2_extof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms1_epd_eis_brst_l2_extof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms1_epd_eis_brst_l2_extof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms1_epd_eis_brst_l2_extof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms1_epd_eis_brst_l2_extof_oxygen_P3_counts_t5]
      
      
      MMS1 ExTOF-Burst oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_extof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms1_epd_eis_brst_l2_extof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms1_epd_eis_brst_l2_extof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms1_epd_eis_brst_l2_extof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms1_epd_eis_brst_l2_extof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms1_epd_eis_brst_l2_extof_oxygen_P3_cps_t5]
      
      
      MMS1 ExTOF-Burst oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_extof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms1_epd_eis_brst_l2_extof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms1_epd_eis_brst_l2_extof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms1_epd_eis_brst_l2_extof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms1_epd_eis_brst_l2_extof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms1_epd_eis_brst_l2_extof_oxygen_P3_flux_t5]
      
      
      MMS1 ExTOF-Burst dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_extof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms1_epd_eis_brst_l2_extof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms1_epd_eis_brst_l2_extof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms1_epd_eis_brst_l2_extof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms1_epd_eis_brst_l2_extof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms1_epd_eis_brst_l2_extof_dump_P3_counts_t5]
      
      
      MMS1 ExTOF-Burst dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_extof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms1_epd_eis_brst_l2_extof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms1_epd_eis_brst_l2_extof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms1_epd_eis_brst_l2_extof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms1_epd_eis_brst_l2_extof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms1_epd_eis_brst_l2_extof_dump_P4_counts_t5]
      
      
      MMS1 ExTOF-Burst dump_P5_counts_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_extof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms1_epd_eis_brst_l2_extof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms1_epd_eis_brst_l2_extof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms1_epd_eis_brst_l2_extof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms1_epd_eis_brst_l2_extof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms1_epd_eis_brst_l2_extof_dump_P5_counts_t5]
      
      
      MMS1 ExTOF-Burst dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_extof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms1_epd_eis_brst_l2_extof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms1_epd_eis_brst_l2_extof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms1_epd_eis_brst_l2_extof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms1_epd_eis_brst_l2_extof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms1_epd_eis_brst_l2_extof_dump_P3_cps_t5]
      
      
      MMS1 ExTOF-Burst dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_extof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms1_epd_eis_brst_l2_extof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms1_epd_eis_brst_l2_extof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms1_epd_eis_brst_l2_extof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms1_epd_eis_brst_l2_extof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms1_epd_eis_brst_l2_extof_dump_P4_cps_t5]
      
      
      MMS1 ExTOF-Burst dump_P5_cps_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_extof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms1_epd_eis_brst_l2_extof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms1_epd_eis_brst_l2_extof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms1_epd_eis_brst_l2_extof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms1_epd_eis_brst_l2_extof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms1_epd_eis_brst_l2_extof_dump_P5_cps_t5]
      
      
      MMS1 ExTOF-Burst dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_extof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms1_epd_eis_brst_l2_extof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms1_epd_eis_brst_l2_extof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms1_epd_eis_brst_l2_extof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms1_epd_eis_brst_l2_extof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms1_epd_eis_brst_l2_extof_dump_P3_flux_t5]
      
      
      MMS1 ExTOF-Burst dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_extof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms1_epd_eis_brst_l2_extof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms1_epd_eis_brst_l2_extof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms1_epd_eis_brst_l2_extof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms1_epd_eis_brst_l2_extof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms1_epd_eis_brst_l2_extof_dump_P4_flux_t5]
      
      
      MMS1 ExTOF-Burst dump_P5_flux_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_extof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms1_epd_eis_brst_l2_extof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms1_epd_eis_brst_l2_extof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms1_epd_eis_brst_l2_extof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms1_epd_eis_brst_l2_extof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms1_epd_eis_brst_l2_extof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS1 [mms1_epd_eis_brst_l2_extof_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS1 [mms1_epd_eis_brst_l2_extof_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS1 [mms1_epd_eis_brst_l2_extof_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS1 [mms1_epd_eis_brst_l2_extof_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS1 [mms1_epd_eis_brst_l2_extof_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS1 [mms1_epd_eis_brst_l2_extof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS1 [mms1_epd_eis_brst_l2_extof_look_t0]
      
      
      Look Direction for Telescope 1 MMS1 [mms1_epd_eis_brst_l2_extof_look_t1]
      
      
      Look Direction for Telescope 2 MMS1 [mms1_epd_eis_brst_l2_extof_look_t2]
      
      
      Look Direction for Telescope 3 MMS1 [mms1_epd_eis_brst_l2_extof_look_t3]
      
      
      Look Direction for Telescope 4 MMS1 [mms1_epd_eis_brst_l2_extof_look_t4]
      
      
      Look Direction for Telescope 5 MMS1 [mms1_epd_eis_brst_l2_extof_look_t5]
      
      
      Magnetic Field BCS MMS1 [mms1_epd_eis_brst_l2_extof_b]
      
      
      Spacecraft position GSE MMS1 [mms1_epd_eis_brst_l2_extof_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS1 [mms1_epd_eis_brst_l2_extof_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS1 [mms1_epd_eis_brst_l2_extof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS1 [mms1_epd_eis_brst_l2_extof_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS1 [mms1_epd_eis_brst_l2_extof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS1 [mms1_epd_eis_brst_l2_extof_r]
      
      
      Dipole L-shell MMS1 [mms1_epd_eis_brst_l2_extof_l]
      
      
      Latitude in GSE Frame MMS1 [mms1_epd_eis_brst_l2_extof_gse_lat]
      
      
      Longitude in GSE Frame MMS1 [mms1_epd_eis_brst_l2_extof_gse_lon]
      
      
      Latitude in GSM Frame MMS1 [mms1_epd_eis_brst_l2_extof_gsm_lat]
      
      
      Longitude in GSM Frame MMS1 [mms1_epd_eis_brst_l2_extof_gsm_lon]
      
      
      Latitude in SM Frame MMS1 [mms1_epd_eis_brst_l2_extof_sm_lat]
      
      
      Longitude in SM Frame MMS1 [mms1_epd_eis_brst_l2_extof_sm_lon]
      
      
      Orbit number MMS1 [mms1_epd_eis_brst_l2_extof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS1 [mms1_epd_eis_brst_l2_extof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS1 [mms1_epd_eis_brst_l2_extof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS1 [mms1_epd_eis_brst_l2_extof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS1 [mms1_epd_eis_brst_l2_extof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS1 [mms1_epd_eis_brst_l2_extof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS1 [mms1_epd_eis_brst_l2_extof_ssd5]
      
      
      Valid Events Processed per second MMS1 [mms1_epd_eis_brst_l2_extof_vep]
      
      
      Start 0 Anode Count Rate MMS1 [mms1_epd_eis_brst_l2_extof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS1 [mms1_epd_eis_brst_l2_extof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS1 [mms1_epd_eis_brst_l2_extof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS1 [mms1_epd_eis_brst_l2_extof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS1 [mms1_epd_eis_brst_l2_extof_vtofxphe]
      
      
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MMS1_EPD-EIS_BRST_L2_PHXTOF (spase://NASA/NumericalData/MMS/1/EnergeticParticleDetector/EIS/Burst/Level2/PulseHeightByTimeOfFlight/PT0.605S)
Description
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Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms1_epd_eis_brst_l2_phxtof_duration]
      
      
      ---> Instrument Deadtime [mms1_epd_eis_brst_l2_phxtof_deadtime]
      
      
      ---> Instrument Large Pixel in Use [mms1_epd_eis_brst_l2_phxtof_largepixel]
      
      
      ---> Spin [mms1_epd_eis_brst_l2_phxtof_spin]
      
      
      ---> Sector [mms1_epd_eis_brst_l2_phxtof_sector]
      
      
      ---> Quality Word [mms1_epd_eis_brst_l2_phxtof_quality]
      
      
      MMS1 PhxTOF-Burst proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms1_epd_eis_brst_l2_phxtof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms1_epd_eis_brst_l2_phxtof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms1_epd_eis_brst_l2_phxtof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms1_epd_eis_brst_l2_phxtof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms1_epd_eis_brst_l2_phxtof_proton_P6_counts_t5]
      
      
      MMS1 PhxTOF-Burst proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms1_epd_eis_brst_l2_phxtof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms1_epd_eis_brst_l2_phxtof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms1_epd_eis_brst_l2_phxtof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms1_epd_eis_brst_l2_phxtof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms1_epd_eis_brst_l2_phxtof_proton_P6_cps_t5]
      
      
      MMS1 PhxTOF-Burst proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms1_epd_eis_brst_l2_phxtof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms1_epd_eis_brst_l2_phxtof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms1_epd_eis_brst_l2_phxtof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms1_epd_eis_brst_l2_phxtof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms1_epd_eis_brst_l2_phxtof_proton_P6_flux_t5]
      
      
      MMS1 PhxTOF-Burst oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t5]
      
      
      MMS1 PhxTOF-Burst oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t5]
      
      
      MMS1 PhxTOF-Burst oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms1_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t5]
      
      
      MMS1 PhxTOF-Burst dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms1_epd_eis_brst_l2_phxtof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms1_epd_eis_brst_l2_phxtof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms1_epd_eis_brst_l2_phxtof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms1_epd_eis_brst_l2_phxtof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms1_epd_eis_brst_l2_phxtof_dump_P6_counts_t5]
      
      
      MMS1 PhxTOF-Burst dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms1_epd_eis_brst_l2_phxtof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms1_epd_eis_brst_l2_phxtof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms1_epd_eis_brst_l2_phxtof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms1_epd_eis_brst_l2_phxtof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms1_epd_eis_brst_l2_phxtof_dump_P6_cps_t5]
      
      
      MMS1 PhxTOF-Burst dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms1_epd_eis_brst_l2_phxtof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms1_epd_eis_brst_l2_phxtof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms1_epd_eis_brst_l2_phxtof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms1_epd_eis_brst_l2_phxtof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms1_epd_eis_brst_l2_phxtof_dump_P6_flux_t5]
      
      
      MMS1 PhxTOF-Burst proton_P5_counts_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms1_epd_eis_brst_l2_phxtof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms1_epd_eis_brst_l2_phxtof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms1_epd_eis_brst_l2_phxtof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms1_epd_eis_brst_l2_phxtof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms1_epd_eis_brst_l2_phxtof_proton_P5_counts_t5]
      
      
      MMS1 PhxTOF-Burst proton_P5_cps_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms1_epd_eis_brst_l2_phxtof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms1_epd_eis_brst_l2_phxtof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms1_epd_eis_brst_l2_phxtof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms1_epd_eis_brst_l2_phxtof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms1_epd_eis_brst_l2_phxtof_proton_P5_cps_t5]
      
      
      MMS1 PhxTOF-Burst proton_P5_flux_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms1_epd_eis_brst_l2_phxtof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms1_epd_eis_brst_l2_phxtof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms1_epd_eis_brst_l2_phxtof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms1_epd_eis_brst_l2_phxtof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms1_epd_eis_brst_l2_phxtof_proton_P5_flux_t5]
      
      
      MMS1 PhxTOF-Burst oxygen_P5_counts_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t5]
      
      
      MMS1 PhxTOF-Burst oxygen_P5_cps_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t5]
      
      
      MMS1 PhxTOF-Burst oxygen_P5_flux_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms1_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t5]
      
      
      MMS1 PhxTOF-Burst proton_P4_counts_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_phxtof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms1_epd_eis_brst_l2_phxtof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms1_epd_eis_brst_l2_phxtof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms1_epd_eis_brst_l2_phxtof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms1_epd_eis_brst_l2_phxtof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms1_epd_eis_brst_l2_phxtof_proton_P4_counts_t5]
      
      
      MMS1 PhxTOF-Burst proton_P4_cps_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_phxtof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms1_epd_eis_brst_l2_phxtof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms1_epd_eis_brst_l2_phxtof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms1_epd_eis_brst_l2_phxtof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms1_epd_eis_brst_l2_phxtof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms1_epd_eis_brst_l2_phxtof_proton_P4_cps_t5]
      
      
      MMS1 PhxTOF-Burst proton_P4_flux_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_phxtof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms1_epd_eis_brst_l2_phxtof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms1_epd_eis_brst_l2_phxtof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms1_epd_eis_brst_l2_phxtof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms1_epd_eis_brst_l2_phxtof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms1_epd_eis_brst_l2_phxtof_proton_P4_flux_t5]
      
      
      MMS1 PhxTOF-Burst oxygen_P4_counts_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t5]
      
      
      MMS1 PhxTOF-Burst oxygen_P4_cps_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t5]
      
      
      MMS1 PhxTOF-Burst oxygen_P4_flux_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms1_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t5]
      
      
      MMS1 PhxTOF-Burst proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_phxtof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms1_epd_eis_brst_l2_phxtof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms1_epd_eis_brst_l2_phxtof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms1_epd_eis_brst_l2_phxtof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms1_epd_eis_brst_l2_phxtof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms1_epd_eis_brst_l2_phxtof_proton_P3_counts_t5]
      
      
      MMS1 PhxTOF-Burst proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_phxtof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms1_epd_eis_brst_l2_phxtof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms1_epd_eis_brst_l2_phxtof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms1_epd_eis_brst_l2_phxtof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms1_epd_eis_brst_l2_phxtof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms1_epd_eis_brst_l2_phxtof_proton_P3_cps_t5]
      
      
      MMS1 PhxTOF-Burst proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_phxtof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms1_epd_eis_brst_l2_phxtof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms1_epd_eis_brst_l2_phxtof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms1_epd_eis_brst_l2_phxtof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms1_epd_eis_brst_l2_phxtof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms1_epd_eis_brst_l2_phxtof_proton_P3_flux_t5]
      
      
      MMS1 PhxTOF-Burst oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t5]
      
      
      MMS1 PhxTOF-Burst oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t5]
      
      
      MMS1 PhxTOF-Burst oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms1_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t5]
      
      
      MMS1 PhxTOF-Burst dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_phxtof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms1_epd_eis_brst_l2_phxtof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms1_epd_eis_brst_l2_phxtof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms1_epd_eis_brst_l2_phxtof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms1_epd_eis_brst_l2_phxtof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms1_epd_eis_brst_l2_phxtof_dump_P3_counts_t5]
      
      
      MMS1 PhxTOF-Burst dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_phxtof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms1_epd_eis_brst_l2_phxtof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms1_epd_eis_brst_l2_phxtof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms1_epd_eis_brst_l2_phxtof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms1_epd_eis_brst_l2_phxtof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms1_epd_eis_brst_l2_phxtof_dump_P4_counts_t5]
      
      
      MMS1 PhxTOF-Burst dump_P5_counts_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms1_epd_eis_brst_l2_phxtof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms1_epd_eis_brst_l2_phxtof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms1_epd_eis_brst_l2_phxtof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms1_epd_eis_brst_l2_phxtof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms1_epd_eis_brst_l2_phxtof_dump_P5_counts_t5]
      
      
      MMS1 PhxTOF-Burst dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_phxtof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms1_epd_eis_brst_l2_phxtof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms1_epd_eis_brst_l2_phxtof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms1_epd_eis_brst_l2_phxtof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms1_epd_eis_brst_l2_phxtof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms1_epd_eis_brst_l2_phxtof_dump_P3_cps_t5]
      
      
      MMS1 PhxTOF-Burst dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_phxtof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms1_epd_eis_brst_l2_phxtof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms1_epd_eis_brst_l2_phxtof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms1_epd_eis_brst_l2_phxtof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms1_epd_eis_brst_l2_phxtof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms1_epd_eis_brst_l2_phxtof_dump_P4_cps_t5]
      
      
      MMS1 PhxTOF-Burst dump_P5_cps_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms1_epd_eis_brst_l2_phxtof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms1_epd_eis_brst_l2_phxtof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms1_epd_eis_brst_l2_phxtof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms1_epd_eis_brst_l2_phxtof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms1_epd_eis_brst_l2_phxtof_dump_P5_cps_t5]
      
      
      MMS1 PhxTOF-Burst dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_brst_l2_phxtof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms1_epd_eis_brst_l2_phxtof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms1_epd_eis_brst_l2_phxtof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms1_epd_eis_brst_l2_phxtof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms1_epd_eis_brst_l2_phxtof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms1_epd_eis_brst_l2_phxtof_dump_P3_flux_t5]
      
      
      MMS1 PhxTOF-Burst dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/05] [mms1_epd_eis_brst_l2_phxtof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms1_epd_eis_brst_l2_phxtof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms1_epd_eis_brst_l2_phxtof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms1_epd_eis_brst_l2_phxtof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms1_epd_eis_brst_l2_phxtof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms1_epd_eis_brst_l2_phxtof_dump_P4_flux_t5]
      
      
      MMS1 PhxTOF-Burst dump_P5_flux_t0 [data available from 2019/12/06 to 2025/01/06] [mms1_epd_eis_brst_l2_phxtof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms1_epd_eis_brst_l2_phxtof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms1_epd_eis_brst_l2_phxtof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms1_epd_eis_brst_l2_phxtof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms1_epd_eis_brst_l2_phxtof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms1_epd_eis_brst_l2_phxtof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS1 [mms1_epd_eis_brst_l2_phxtof_pitch_angle_t0]
      
      
      ---> Pitch Angle for Telescope 1 MMS1 [mms1_epd_eis_brst_l2_phxtof_pitch_angle_t1]
      
      
      ---> Pitch Angle for Telescope 2 MMS1 [mms1_epd_eis_brst_l2_phxtof_pitch_angle_t2]
      
      
      ---> Pitch Angle for Telescope 3 MMS1 [mms1_epd_eis_brst_l2_phxtof_pitch_angle_t3]
      
      
      ---> Pitch Angle for Telescope 4 MMS1 [mms1_epd_eis_brst_l2_phxtof_pitch_angle_t4]
      
      
      ---> Pitch Angle for Telescope 5 MMS1 [mms1_epd_eis_brst_l2_phxtof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS1 [mms1_epd_eis_brst_l2_phxtof_look_t0]
      
      
      ---> Look Direction for Telescope 1 MMS1 [mms1_epd_eis_brst_l2_phxtof_look_t1]
      
      
      ---> Look Direction for Telescope 2 MMS1 [mms1_epd_eis_brst_l2_phxtof_look_t2]
      
      
      ---> Look Direction for Telescope 3 MMS1 [mms1_epd_eis_brst_l2_phxtof_look_t3]
      
      
      ---> Look Direction for Telescope 4 MMS1 [mms1_epd_eis_brst_l2_phxtof_look_t4]
      
      
      ---> Look Direction for Telescope 5 MMS1 [mms1_epd_eis_brst_l2_phxtof_look_t5]
      
      
      Magnetic Field BCS MMS1 [mms1_epd_eis_brst_l2_phxtof_b]
      
      
      Spacecraft position GSE MMS1 [mms1_epd_eis_brst_l2_phxtof_position_gse]
      
      
      ---> Spacecraft position in GSM coordinates MMS1 [mms1_epd_eis_brst_l2_phxtof_position_gsm]
      
      
      ---> Spacecraft-Moon vector in GSE coordinates MMS1 [mms1_epd_eis_brst_l2_phxtof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS1 [mms1_epd_eis_brst_l2_phxtof_sc_to_gse]
      
      
      ---> Transformation Matrix GSE to GSM Frame MMS1 [mms1_epd_eis_brst_l2_phxtof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS1 [mms1_epd_eis_brst_l2_phxtof_r]
      
      
      Dipole L-shell MMS1 [mms1_epd_eis_brst_l2_phxtof_l]
      
      
      Latitude in GSE Frame MMS1 [mms1_epd_eis_brst_l2_phxtof_gse_lat]
      
      
      Longitude in GSE Frame MMS1 [mms1_epd_eis_brst_l2_phxtof_gse_lon]
      
      
      Latitude in GSM Frame MMS1 [mms1_epd_eis_brst_l2_phxtof_gsm_lat]
      
      
      Longitude in GSM Frame MMS1 [mms1_epd_eis_brst_l2_phxtof_gsm_lon]
      
      
      Latitude in SM Frame MMS1 [mms1_epd_eis_brst_l2_phxtof_sm_lat]
      
      
      Longitude in SM Frame MMS1 [mms1_epd_eis_brst_l2_phxtof_sm_lon]
      
      
      Orbit number MMS1 [mms1_epd_eis_brst_l2_phxtof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS1 [mms1_epd_eis_brst_l2_phxtof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS1 [mms1_epd_eis_brst_l2_phxtof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS1 [mms1_epd_eis_brst_l2_phxtof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS1 [mms1_epd_eis_brst_l2_phxtof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS1 [mms1_epd_eis_brst_l2_phxtof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS1 [mms1_epd_eis_brst_l2_phxtof_ssd5]
      
      
      Valid Events Processed per second MMS1 [mms1_epd_eis_brst_l2_phxtof_vep]
      
      
      Start 0 Anode Count Rate MMS1 [mms1_epd_eis_brst_l2_phxtof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS1 [mms1_epd_eis_brst_l2_phxtof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS1 [mms1_epd_eis_brst_l2_phxtof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS1 [mms1_epd_eis_brst_l2_phxtof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS1 [mms1_epd_eis_brst_l2_phxtof_vtofxphe]
      
      
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MMS1_EPD-EIS_SRVY_L2_ELECTRONENERGY (spase://NASA/NumericalData/MMS/1/EnergeticParticleDetector/EIS/Survey/Level2/ElectronEnergySpectra/PT2.42S)
Description
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Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms1_epd_eis_srvy_l2_electronenergy_duration]
      
      
      Instrument Deadtime [mms1_epd_eis_srvy_l2_electronenergy_deadtime]
      
      
      Instrument Large Pixel in Use [mms1_epd_eis_srvy_l2_electronenergy_largepixel]
      
      
      Spin [mms1_epd_eis_srvy_l2_electronenergy_spin]
      
      
      Sector [mms1_epd_eis_srvy_l2_electronenergy_sector]
      
      
      Quality Word [mms1_epd_eis_srvy_l2_electronenergy_quality]
      
      
      MMS1 ElectronEnergy-Survey electron_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t0]
      
      
      ---> electron_P6_counts_t1 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t1]
      
      
      ---> electron_P6_counts_t2 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t2]
      
      
      ---> electron_P6_counts_t3 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t3]
      
      
      ---> electron_P6_counts_t4 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t4]
      
      
      ---> electron_P6_counts_t5 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t5]
      
      
      MMS1 ElectronEnergy-Survey electron_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t0]
      
      
      ---> electron_P6_cps_t1 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t1]
      
      
      ---> electron_P6_cps_t2 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t2]
      
      
      ---> electron_P6_cps_t3 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t3]
      
      
      ---> electron_P6_cps_t4 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t4]
      
      
      ---> electron_P6_cps_t5 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t5]
      
      
      MMS1 ElectronEnergy-Survey electron_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t0]
      
      
      ---> electron_P6_flux_t1 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t1]
      
      
      ---> electron_P6_flux_t2 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t2]
      
      
      ---> electron_P6_flux_t3 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t3]
      
      
      ---> electron_P6_flux_t4 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t4]
      
      
      ---> electron_P6_flux_t5 [mms1_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t5]
      
      
      MMS1 ElectronEnergy-Survey dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t5]
      
      
      MMS1 ElectronEnergy-Survey dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t5]
      
      
      MMS1 ElectronEnergy-Survey dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms1_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t5]
      
      
      MMS1 ElectronEnergy-Survey electron_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t0]
      
      
      ---> electron_P5_counts_t1 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t1]
      
      
      ---> electron_P5_counts_t2 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t2]
      
      
      ---> electron_P5_counts_t3 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t3]
      
      
      ---> electron_P5_counts_t4 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t4]
      
      
      ---> electron_P5_counts_t5 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t5]
      
      
      MMS1 ElectronEnergy-Survey electron_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t0]
      
      
      ---> electron_P5_cps_t1 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t1]
      
      
      ---> electron_P5_cps_t2 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t2]
      
      
      ---> electron_P5_cps_t3 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t3]
      
      
      ---> electron_P5_cps_t4 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t4]
      
      
      ---> electron_P5_cps_t5 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t5]
      
      
      MMS1 ElectronEnergy-Survey electron_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t0]
      
      
      ---> electron_P5_flux_t1 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t1]
      
      
      ---> electron_P5_flux_t2 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t2]
      
      
      ---> electron_P5_flux_t3 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t3]
      
      
      ---> electron_P5_flux_t4 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t4]
      
      
      ---> electron_P5_flux_t5 [mms1_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t5]
      
      
      MMS1 ElectronEnergy-Survey electron_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t0]
      
      
      ---> electron_P4_counts_t1 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t1]
      
      
      ---> electron_P4_counts_t2 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t2]
      
      
      ---> electron_P4_counts_t3 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t3]
      
      
      ---> electron_P4_counts_t4 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t4]
      
      
      ---> electron_P4_counts_t5 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t5]
      
      
      MMS1 ElectronEnergy-Survey electron_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t0]
      
      
      ---> electron_P4_cps_t1 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t1]
      
      
      ---> electron_P4_cps_t2 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t2]
      
      
      ---> electron_P4_cps_t3 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t3]
      
      
      ---> electron_P4_cps_t4 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t4]
      
      
      ---> electron_P4_cps_t5 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t5]
      
      
      MMS1 ElectronEnergy-Survey electron_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t0]
      
      
      ---> electron_P4_flux_t1 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t1]
      
      
      ---> electron_P4_flux_t2 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t2]
      
      
      ---> electron_P4_flux_t3 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t3]
      
      
      ---> electron_P4_flux_t4 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t4]
      
      
      ---> electron_P4_flux_t5 [mms1_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t5]
      
      
      MMS1 ElectronEnergy-Survey electron_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t0]
      
      
      ---> electron_P3_counts_t1 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t1]
      
      
      ---> electron_P3_counts_t2 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t2]
      
      
      ---> electron_P3_counts_t3 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t3]
      
      
      ---> electron_P3_counts_t4 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t4]
      
      
      ---> electron_P3_counts_t5 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t5]
      
      
      MMS1 ElectronEnergy-Survey electron_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t0]
      
      
      ---> electron_P3_cps_t1 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t1]
      
      
      ---> electron_P3_cps_t2 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t2]
      
      
      ---> electron_P3_cps_t3 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t3]
      
      
      ---> electron_P3_cps_t4 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t4]
      
      
      ---> electron_P3_cps_t5 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t5]
      
      
      MMS1 ElectronEnergy-Survey electron_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t0]
      
      
      ---> electron_P3_flux_t1 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t1]
      
      
      ---> electron_P3_flux_t2 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t2]
      
      
      ---> electron_P3_flux_t3 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t3]
      
      
      ---> electron_P3_flux_t4 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t4]
      
      
      ---> electron_P3_flux_t5 [mms1_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t5]
      
      
      MMS1 ElectronEnergy-Survey dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t5]
      
      
      MMS1 ElectronEnergy-Survey dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t5]
      
      
      MMS1 ElectronEnergy-Survey dump_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t5]
      
      
      MMS1 ElectronEnergy-Survey dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t5]
      
      
      MMS1 ElectronEnergy-Survey dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t5]
      
      
      MMS1 ElectronEnergy-Survey dump_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t5]
      
      
      MMS1 ElectronEnergy-Survey dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms1_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t5]
      
      
      MMS1 ElectronEnergy-Survey dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms1_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t5]
      
      
      MMS1 ElectronEnergy-Survey dump_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms1_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS1 [mms1_epd_eis_srvy_l2_electronenergy_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS1 [mms1_epd_eis_srvy_l2_electronenergy_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS1 [mms1_epd_eis_srvy_l2_electronenergy_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS1 [mms1_epd_eis_srvy_l2_electronenergy_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS1 [mms1_epd_eis_srvy_l2_electronenergy_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS1 [mms1_epd_eis_srvy_l2_electronenergy_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS1 [mms1_epd_eis_srvy_l2_electronenergy_look_t0]
      
      
      Look Direction for Telescope 1 MMS1 [mms1_epd_eis_srvy_l2_electronenergy_look_t1]
      
      
      Look Direction for Telescope 2 MMS1 [mms1_epd_eis_srvy_l2_electronenergy_look_t2]
      
      
      Look Direction for Telescope 3 MMS1 [mms1_epd_eis_srvy_l2_electronenergy_look_t3]
      
      
      Look Direction for Telescope 4 MMS1 [mms1_epd_eis_srvy_l2_electronenergy_look_t4]
      
      
      Look Direction for Telescope 5 MMS1 [mms1_epd_eis_srvy_l2_electronenergy_look_t5]
      
      
      Magnetic Field BCS MMS1 [mms1_epd_eis_srvy_l2_electronenergy_b]
      
      
      Spacecraft position GSE MMS1 [mms1_epd_eis_srvy_l2_electronenergy_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS1 [mms1_epd_eis_srvy_l2_electronenergy_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS1 [mms1_epd_eis_srvy_l2_electronenergy_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS1 [mms1_epd_eis_srvy_l2_electronenergy_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS1 [mms1_epd_eis_srvy_l2_electronenergy_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS1 [mms1_epd_eis_srvy_l2_electronenergy_r]
      
      
      Dipole L-shell MMS1 [mms1_epd_eis_srvy_l2_electronenergy_l]
      
      
      Latitude in GSE Frame MMS1 [mms1_epd_eis_srvy_l2_electronenergy_gse_lat]
      
      
      Longitude in GSE Frame MMS1 [mms1_epd_eis_srvy_l2_electronenergy_gse_lon]
      
      
      Latitude in GSM Frame MMS1 [mms1_epd_eis_srvy_l2_electronenergy_gsm_lat]
      
      
      Longitude in GSM Frame MMS1 [mms1_epd_eis_srvy_l2_electronenergy_gsm_lon]
      
      
      Latitude in SM Frame MMS1 [mms1_epd_eis_srvy_l2_electronenergy_sm_lat]
      
      
      Longitude in SM Frame MMS1 [mms1_epd_eis_srvy_l2_electronenergy_sm_lon]
      
      
      Orbit number MMS1 [mms1_epd_eis_srvy_l2_electronenergy_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS1 [mms1_epd_eis_srvy_l2_electronenergy_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS1 [mms1_epd_eis_srvy_l2_electronenergy_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS1 [mms1_epd_eis_srvy_l2_electronenergy_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS1 [mms1_epd_eis_srvy_l2_electronenergy_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS1 [mms1_epd_eis_srvy_l2_electronenergy_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS1 [mms1_epd_eis_srvy_l2_electronenergy_ssd5]
      
      
      Valid Events Processed per second MMS1 [mms1_epd_eis_srvy_l2_electronenergy_vep]
      
      
      Valid Electron Events per second MMS1 [mms1_epd_eis_srvy_l2_electronenergy_vee]
      
      
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MMS1_EPD-EIS_SRVY_L2_EXTOF (spase://NASA/NumericalData/MMS/1/EnergeticParticleDetector/EIS/Survey/Level2/EnergyByTimeOfFlight/PT2.42S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms1_epd_eis_srvy_l2_extof_duration]
      
      
      ---> Instrument Deadtime [mms1_epd_eis_srvy_l2_extof_deadtime]
      
      
      ---> Instrument Large Pixel in Use [mms1_epd_eis_srvy_l2_extof_largepixel]
      
      
      ---> Spin [mms1_epd_eis_srvy_l2_extof_spin]
      
      
      ---> Sector [mms1_epd_eis_srvy_l2_extof_sector]
      
      
      ---> Quality Word [mms1_epd_eis_srvy_l2_extof_quality]
      
      
      MMS1 ExTOF-Survey proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_extof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms1_epd_eis_srvy_l2_extof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms1_epd_eis_srvy_l2_extof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms1_epd_eis_srvy_l2_extof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms1_epd_eis_srvy_l2_extof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms1_epd_eis_srvy_l2_extof_proton_P6_counts_t5]
      
      
      MMS1 ExTOF-Survey proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_extof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms1_epd_eis_srvy_l2_extof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms1_epd_eis_srvy_l2_extof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms1_epd_eis_srvy_l2_extof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms1_epd_eis_srvy_l2_extof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms1_epd_eis_srvy_l2_extof_proton_P6_cps_t5]
      
      
      MMS1 ExTOF-Survey proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_extof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms1_epd_eis_srvy_l2_extof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms1_epd_eis_srvy_l2_extof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms1_epd_eis_srvy_l2_extof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms1_epd_eis_srvy_l2_extof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms1_epd_eis_srvy_l2_extof_proton_P6_flux_t5]
      
      
      MMS1 ExTOF-Survey helium_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_extof_helium_P6_counts_t0]
      
      
      ---> helium_P6_counts_t1 [mms1_epd_eis_srvy_l2_extof_helium_P6_counts_t1]
      
      
      ---> helium_P6_counts_t2 [mms1_epd_eis_srvy_l2_extof_helium_P6_counts_t2]
      
      
      ---> helium_P6_counts_t3 [mms1_epd_eis_srvy_l2_extof_helium_P6_counts_t3]
      
      
      ---> helium_P6_counts_t4 [mms1_epd_eis_srvy_l2_extof_helium_P6_counts_t4]
      
      
      ---> helium_P6_counts_t5 [mms1_epd_eis_srvy_l2_extof_helium_P6_counts_t5]
      
      
      MMS1 ExTOF-Survey helium_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_extof_helium_P6_cps_t0]
      
      
      ---> helium_P6_cps_t1 [mms1_epd_eis_srvy_l2_extof_helium_P6_cps_t1]
      
      
      ---> helium_P6_cps_t2 [mms1_epd_eis_srvy_l2_extof_helium_P6_cps_t2]
      
      
      ---> helium_P6_cps_t3 [mms1_epd_eis_srvy_l2_extof_helium_P6_cps_t3]
      
      
      ---> helium_P6_cps_t4 [mms1_epd_eis_srvy_l2_extof_helium_P6_cps_t4]
      
      
      ---> helium_P6_cps_t5 [mms1_epd_eis_srvy_l2_extof_helium_P6_cps_t5]
      
      
      MMS1 ExTOF-Survey helium_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_extof_helium_P6_flux_t0]
      
      
      ---> helium_P6_flux_t1 [mms1_epd_eis_srvy_l2_extof_helium_P6_flux_t1]
      
      
      ---> helium_P6_flux_t2 [mms1_epd_eis_srvy_l2_extof_helium_P6_flux_t2]
      
      
      ---> helium_P6_flux_t3 [mms1_epd_eis_srvy_l2_extof_helium_P6_flux_t3]
      
      
      ---> helium_P6_flux_t4 [mms1_epd_eis_srvy_l2_extof_helium_P6_flux_t4]
      
      
      ---> helium_P6_flux_t5 [mms1_epd_eis_srvy_l2_extof_helium_P6_flux_t5]
      
      
      MMS1 ExTOF-Survey oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_extof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_counts_t5]
      
      
      MMS1 ExTOF-Survey oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_extof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_cps_t5]
      
      
      MMS1 ExTOF-Survey oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_extof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms1_epd_eis_srvy_l2_extof_oxygen_P6_flux_t5]
      
      
      MMS1 ExTOF-Survey dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_extof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms1_epd_eis_srvy_l2_extof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms1_epd_eis_srvy_l2_extof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms1_epd_eis_srvy_l2_extof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms1_epd_eis_srvy_l2_extof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms1_epd_eis_srvy_l2_extof_dump_P6_counts_t5]
      
      
      MMS1 ExTOF-Survey dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_extof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms1_epd_eis_srvy_l2_extof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms1_epd_eis_srvy_l2_extof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms1_epd_eis_srvy_l2_extof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms1_epd_eis_srvy_l2_extof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms1_epd_eis_srvy_l2_extof_dump_P6_cps_t5]
      
      
      MMS1 ExTOF-Survey dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_extof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms1_epd_eis_srvy_l2_extof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms1_epd_eis_srvy_l2_extof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms1_epd_eis_srvy_l2_extof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms1_epd_eis_srvy_l2_extof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms1_epd_eis_srvy_l2_extof_dump_P6_flux_t5]
      
      
      MMS1 ExTOF-Survey proton_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms1_epd_eis_srvy_l2_extof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms1_epd_eis_srvy_l2_extof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms1_epd_eis_srvy_l2_extof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms1_epd_eis_srvy_l2_extof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms1_epd_eis_srvy_l2_extof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms1_epd_eis_srvy_l2_extof_proton_P5_counts_t5]
      
      
      MMS1 ExTOF-Survey proton_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms1_epd_eis_srvy_l2_extof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms1_epd_eis_srvy_l2_extof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms1_epd_eis_srvy_l2_extof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms1_epd_eis_srvy_l2_extof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms1_epd_eis_srvy_l2_extof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms1_epd_eis_srvy_l2_extof_proton_P5_cps_t5]
      
      
      MMS1 ExTOF-Survey proton_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms1_epd_eis_srvy_l2_extof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms1_epd_eis_srvy_l2_extof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms1_epd_eis_srvy_l2_extof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms1_epd_eis_srvy_l2_extof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms1_epd_eis_srvy_l2_extof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms1_epd_eis_srvy_l2_extof_proton_P5_flux_t5]
      
      
      MMS1 ExTOF-Survey oxygen_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms1_epd_eis_srvy_l2_extof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_counts_t5]
      
      
      MMS1 ExTOF-Survey oxygen_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms1_epd_eis_srvy_l2_extof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_cps_t5]
      
      
      MMS1 ExTOF-Survey oxygen_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms1_epd_eis_srvy_l2_extof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms1_epd_eis_srvy_l2_extof_oxygen_P5_flux_t5]
      
      
      MMS1 ExTOF-Survey helium_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms1_epd_eis_srvy_l2_extof_helium_P5_counts_t0]
      
      
      ---> helium_P5_counts_t1 [mms1_epd_eis_srvy_l2_extof_helium_P5_counts_t1]
      
      
      ---> helium_P5_counts_t2 [mms1_epd_eis_srvy_l2_extof_helium_P5_counts_t2]
      
      
      ---> helium_P5_counts_t3 [mms1_epd_eis_srvy_l2_extof_helium_P5_counts_t3]
      
      
      ---> helium_P5_counts_t4 [mms1_epd_eis_srvy_l2_extof_helium_P5_counts_t4]
      
      
      ---> helium_P5_counts_t5 [mms1_epd_eis_srvy_l2_extof_helium_P5_counts_t5]
      
      
      MMS1 ExTOF-Survey helium_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms1_epd_eis_srvy_l2_extof_helium_P5_cps_t0]
      
      
      ---> helium_P5_cps_t1 [mms1_epd_eis_srvy_l2_extof_helium_P5_cps_t1]
      
      
      ---> helium_P5_cps_t2 [mms1_epd_eis_srvy_l2_extof_helium_P5_cps_t2]
      
      
      ---> helium_P5_cps_t3 [mms1_epd_eis_srvy_l2_extof_helium_P5_cps_t3]
      
      
      ---> helium_P5_cps_t4 [mms1_epd_eis_srvy_l2_extof_helium_P5_cps_t4]
      
      
      ---> helium_P5_cps_t5 [mms1_epd_eis_srvy_l2_extof_helium_P5_cps_t5]
      
      
      MMS1 ExTOF-Survey helium_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms1_epd_eis_srvy_l2_extof_helium_P5_flux_t0]
      
      
      ---> helium_P5_flux_t1 [mms1_epd_eis_srvy_l2_extof_helium_P5_flux_t1]
      
      
      ---> helium_P5_flux_t2 [mms1_epd_eis_srvy_l2_extof_helium_P5_flux_t2]
      
      
      ---> helium_P5_flux_t3 [mms1_epd_eis_srvy_l2_extof_helium_P5_flux_t3]
      
      
      ---> helium_P5_flux_t4 [mms1_epd_eis_srvy_l2_extof_helium_P5_flux_t4]
      
      
      ---> helium_P5_flux_t5 [mms1_epd_eis_srvy_l2_extof_helium_P5_flux_t5]
      
      
      MMS1 ExTOF-Survey proton_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms1_epd_eis_srvy_l2_extof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms1_epd_eis_srvy_l2_extof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms1_epd_eis_srvy_l2_extof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms1_epd_eis_srvy_l2_extof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms1_epd_eis_srvy_l2_extof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms1_epd_eis_srvy_l2_extof_proton_P4_counts_t5]
      
      
      MMS1 ExTOF-Survey proton_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms1_epd_eis_srvy_l2_extof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms1_epd_eis_srvy_l2_extof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms1_epd_eis_srvy_l2_extof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms1_epd_eis_srvy_l2_extof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms1_epd_eis_srvy_l2_extof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms1_epd_eis_srvy_l2_extof_proton_P4_cps_t5]
      
      
      MMS1 ExTOF-Survey proton_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms1_epd_eis_srvy_l2_extof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms1_epd_eis_srvy_l2_extof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms1_epd_eis_srvy_l2_extof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms1_epd_eis_srvy_l2_extof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms1_epd_eis_srvy_l2_extof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms1_epd_eis_srvy_l2_extof_proton_P4_flux_t5]
      
      
      MMS1 ExTOF-Survey alpha_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms1_epd_eis_srvy_l2_extof_helium_P4_counts_t0]
      
      
      ---> alpha_P4_counts_t1 [mms1_epd_eis_srvy_l2_extof_helium_P4_counts_t1]
      
      
      ---> alpha_P4_counts_t2 [mms1_epd_eis_srvy_l2_extof_helium_P4_counts_t2]
      
      
      ---> alpha_P4_counts_t3 [mms1_epd_eis_srvy_l2_extof_helium_P4_counts_t3]
      
      
      ---> alpha_P4_counts_t4 [mms1_epd_eis_srvy_l2_extof_helium_P4_counts_t4]
      
      
      ---> alpha_P4_counts_t5 [mms1_epd_eis_srvy_l2_extof_helium_P4_counts_t5]
      
      
      MMS1 ExTOF-Survey alpha_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms1_epd_eis_srvy_l2_extof_helium_P4_cps_t0]
      
      
      ---> alpha_P4_cps_t1 [mms1_epd_eis_srvy_l2_extof_helium_P4_cps_t1]
      
      
      ---> alpha_P4_cps_t2 [mms1_epd_eis_srvy_l2_extof_helium_P4_cps_t2]
      
      
      ---> alpha_P4_cps_t3 [mms1_epd_eis_srvy_l2_extof_helium_P4_cps_t3]
      
      
      ---> alpha_P4_cps_t4 [mms1_epd_eis_srvy_l2_extof_helium_P4_cps_t4]
      
      
      ---> alpha_P4_cps_t5 [mms1_epd_eis_srvy_l2_extof_helium_P4_cps_t5]
      
      
      MMS1 ExTOF-Survey alpha_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms1_epd_eis_srvy_l2_extof_helium_P4_flux_t0]
      
      
      ---> alpha_P4_flux_t1 [mms1_epd_eis_srvy_l2_extof_helium_P4_flux_t1]
      
      
      ---> alpha_P4_flux_t2 [mms1_epd_eis_srvy_l2_extof_helium_P4_flux_t2]
      
      
      ---> alpha_P4_flux_t3 [mms1_epd_eis_srvy_l2_extof_helium_P4_flux_t3]
      
      
      ---> alpha_P4_flux_t4 [mms1_epd_eis_srvy_l2_extof_helium_P4_flux_t4]
      
      
      ---> alpha_P4_flux_t5 [mms1_epd_eis_srvy_l2_extof_helium_P4_flux_t5]
      
      
      MMS1 ExTOF-Survey oxygen_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms1_epd_eis_srvy_l2_extof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_counts_t5]
      
      
      MMS1 ExTOF-Survey oxygen_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms1_epd_eis_srvy_l2_extof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_cps_t5]
      
      
      MMS1 ExTOF-Survey oxygen_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms1_epd_eis_srvy_l2_extof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms1_epd_eis_srvy_l2_extof_oxygen_P4_flux_t5]
      
      
      MMS1 ExTOF-Survey proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_extof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms1_epd_eis_srvy_l2_extof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms1_epd_eis_srvy_l2_extof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms1_epd_eis_srvy_l2_extof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms1_epd_eis_srvy_l2_extof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms1_epd_eis_srvy_l2_extof_proton_P3_counts_t5]
      
      
      MMS1 ExTOF-Survey proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_extof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms1_epd_eis_srvy_l2_extof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms1_epd_eis_srvy_l2_extof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms1_epd_eis_srvy_l2_extof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms1_epd_eis_srvy_l2_extof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms1_epd_eis_srvy_l2_extof_proton_P3_cps_t5]
      
      
      MMS1 ExTOF-Survey proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_extof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms1_epd_eis_srvy_l2_extof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms1_epd_eis_srvy_l2_extof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms1_epd_eis_srvy_l2_extof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms1_epd_eis_srvy_l2_extof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms1_epd_eis_srvy_l2_extof_proton_P3_flux_t5]
      
      
      MMS1 ExTOF-Survey alpha_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_extof_helium_P3_counts_t0]
      
      
      ---> alpha_P3_counts_t1 [mms1_epd_eis_srvy_l2_extof_helium_P3_counts_t1]
      
      
      ---> alpha_P3_counts_t2 [mms1_epd_eis_srvy_l2_extof_helium_P3_counts_t2]
      
      
      ---> alpha_P3_counts_t3 [mms1_epd_eis_srvy_l2_extof_helium_P3_counts_t3]
      
      
      ---> alpha_P3_counts_t4 [mms1_epd_eis_srvy_l2_extof_helium_P3_counts_t4]
      
      
      ---> alpha_P3_counts_t5 [mms1_epd_eis_srvy_l2_extof_helium_P3_counts_t5]
      
      
      MMS1 ExTOF-Survey alpha_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_extof_helium_P3_cps_t0]
      
      
      ---> alpha_P3_cps_t1 [mms1_epd_eis_srvy_l2_extof_helium_P3_cps_t1]
      
      
      ---> alpha_P3_cps_t2 [mms1_epd_eis_srvy_l2_extof_helium_P3_cps_t2]
      
      
      ---> alpha_P3_cps_t3 [mms1_epd_eis_srvy_l2_extof_helium_P3_cps_t3]
      
      
      ---> alpha_P3_cps_t4 [mms1_epd_eis_srvy_l2_extof_helium_P3_cps_t4]
      
      
      ---> alpha_P3_cps_t5 [mms1_epd_eis_srvy_l2_extof_helium_P3_cps_t5]
      
      
      MMS1 ExTOF-Survey alpha_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_extof_helium_P3_flux_t0]
      
      
      ---> alpha_P3_flux_t1 [mms1_epd_eis_srvy_l2_extof_helium_P3_flux_t1]
      
      
      ---> alpha_P3_flux_t2 [mms1_epd_eis_srvy_l2_extof_helium_P3_flux_t2]
      
      
      ---> alpha_P3_flux_t3 [mms1_epd_eis_srvy_l2_extof_helium_P3_flux_t3]
      
      
      ---> alpha_P3_flux_t4 [mms1_epd_eis_srvy_l2_extof_helium_P3_flux_t4]
      
      
      ---> alpha_P3_flux_t5 [mms1_epd_eis_srvy_l2_extof_helium_P3_flux_t5]
      
      
      MMS1 ExTOF-Survey oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_extof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_counts_t5]
      
      
      MMS1 ExTOF-Survey oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_extof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_cps_t5]
      
      
      MMS1 ExTOF-Survey oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_extof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms1_epd_eis_srvy_l2_extof_oxygen_P3_flux_t5]
      
      
      MMS1 ExTOF-Survey dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_extof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms1_epd_eis_srvy_l2_extof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms1_epd_eis_srvy_l2_extof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms1_epd_eis_srvy_l2_extof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms1_epd_eis_srvy_l2_extof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms1_epd_eis_srvy_l2_extof_dump_P3_counts_t5]
      
      
      MMS1 ExTOF-Survey dump_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms1_epd_eis_srvy_l2_extof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms1_epd_eis_srvy_l2_extof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms1_epd_eis_srvy_l2_extof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms1_epd_eis_srvy_l2_extof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms1_epd_eis_srvy_l2_extof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms1_epd_eis_srvy_l2_extof_dump_P4_counts_t5]
      
      
      MMS1 ExTOF-Survey dump_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms1_epd_eis_srvy_l2_extof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms1_epd_eis_srvy_l2_extof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms1_epd_eis_srvy_l2_extof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms1_epd_eis_srvy_l2_extof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms1_epd_eis_srvy_l2_extof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms1_epd_eis_srvy_l2_extof_dump_P5_counts_t5]
      
      
      MMS1 ExTOF-Survey dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_extof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms1_epd_eis_srvy_l2_extof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms1_epd_eis_srvy_l2_extof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms1_epd_eis_srvy_l2_extof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms1_epd_eis_srvy_l2_extof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms1_epd_eis_srvy_l2_extof_dump_P3_cps_t5]
      
      
      MMS1 ExTOF-Survey dump_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms1_epd_eis_srvy_l2_extof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms1_epd_eis_srvy_l2_extof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms1_epd_eis_srvy_l2_extof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms1_epd_eis_srvy_l2_extof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms1_epd_eis_srvy_l2_extof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms1_epd_eis_srvy_l2_extof_dump_P4_cps_t5]
      
      
      MMS1 ExTOF-Survey dump_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms1_epd_eis_srvy_l2_extof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms1_epd_eis_srvy_l2_extof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms1_epd_eis_srvy_l2_extof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms1_epd_eis_srvy_l2_extof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms1_epd_eis_srvy_l2_extof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms1_epd_eis_srvy_l2_extof_dump_P5_cps_t5]
      
      
      MMS1 ExTOF-Survey dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_extof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms1_epd_eis_srvy_l2_extof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms1_epd_eis_srvy_l2_extof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms1_epd_eis_srvy_l2_extof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms1_epd_eis_srvy_l2_extof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms1_epd_eis_srvy_l2_extof_dump_P3_flux_t5]
      
      
      MMS1 ExTOF-Survey dump_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms1_epd_eis_srvy_l2_extof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms1_epd_eis_srvy_l2_extof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms1_epd_eis_srvy_l2_extof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms1_epd_eis_srvy_l2_extof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms1_epd_eis_srvy_l2_extof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms1_epd_eis_srvy_l2_extof_dump_P4_flux_t5]
      
      
      MMS1 ExTOF-Survey dump_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms1_epd_eis_srvy_l2_extof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms1_epd_eis_srvy_l2_extof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms1_epd_eis_srvy_l2_extof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms1_epd_eis_srvy_l2_extof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms1_epd_eis_srvy_l2_extof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms1_epd_eis_srvy_l2_extof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS1 [mms1_epd_eis_srvy_l2_extof_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS1 [mms1_epd_eis_srvy_l2_extof_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS1 [mms1_epd_eis_srvy_l2_extof_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS1 [mms1_epd_eis_srvy_l2_extof_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS1 [mms1_epd_eis_srvy_l2_extof_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS1 [mms1_epd_eis_srvy_l2_extof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS1 [mms1_epd_eis_srvy_l2_extof_look_t0]
      
      
      Look Direction for Telescope 1 MMS1 [mms1_epd_eis_srvy_l2_extof_look_t1]
      
      
      Look Direction for Telescope 2 MMS1 [mms1_epd_eis_srvy_l2_extof_look_t2]
      
      
      Look Direction for Telescope 3 MMS1 [mms1_epd_eis_srvy_l2_extof_look_t3]
      
      
      Look Direction for Telescope 4 MMS1 [mms1_epd_eis_srvy_l2_extof_look_t4]
      
      
      Look Direction for Telescope 5 MMS1 [mms1_epd_eis_srvy_l2_extof_look_t5]
      
      
      Magnetic Field BCS MMS1 [mms1_epd_eis_srvy_l2_extof_b]
      
      
      Spacecraft position GSE MMS1 [mms1_epd_eis_srvy_l2_extof_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS1 [mms1_epd_eis_srvy_l2_extof_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS1 [mms1_epd_eis_srvy_l2_extof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS1 [mms1_epd_eis_srvy_l2_extof_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS1 [mms1_epd_eis_srvy_l2_extof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS1 [mms1_epd_eis_srvy_l2_extof_r]
      
      
      Dipole L-shell MMS1 [mms1_epd_eis_srvy_l2_extof_l]
      
      
      Latitude in GSE Frame MMS1 [mms1_epd_eis_srvy_l2_extof_gse_lat]
      
      
      Longitude in GSE Frame MMS1 [mms1_epd_eis_srvy_l2_extof_gse_lon]
      
      
      Latitude in GSM Frame MMS1 [mms1_epd_eis_srvy_l2_extof_gsm_lat]
      
      
      Longitude in GSM Frame MMS1 [mms1_epd_eis_srvy_l2_extof_gsm_lon]
      
      
      Latitude in SM Frame MMS1 [mms1_epd_eis_srvy_l2_extof_sm_lat]
      
      
      Longitude in SM Frame MMS1 [mms1_epd_eis_srvy_l2_extof_sm_lon]
      
      
      Orbit number MMS1 [mms1_epd_eis_srvy_l2_extof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS1 [mms1_epd_eis_srvy_l2_extof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS1 [mms1_epd_eis_srvy_l2_extof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS1 [mms1_epd_eis_srvy_l2_extof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS1 [mms1_epd_eis_srvy_l2_extof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS1 [mms1_epd_eis_srvy_l2_extof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS1 [mms1_epd_eis_srvy_l2_extof_ssd5]
      
      
      Valid Events Processed per second MMS1 [mms1_epd_eis_srvy_l2_extof_vep]
      
      
      Start 0 Anode Count Rate MMS1 [mms1_epd_eis_srvy_l2_extof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS1 [mms1_epd_eis_srvy_l2_extof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS1 [mms1_epd_eis_srvy_l2_extof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS1 [mms1_epd_eis_srvy_l2_extof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS1 [mms1_epd_eis_srvy_l2_extof_vtofxphe]
      
      
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MMS1_EPD-EIS_SRVY_L2_PHXTOF (spase://NASA/NumericalData/MMS/1/EnergeticParticleDetector/EIS/Survey/Level2/PulseHeightByTimeOfFlight/PT2.42S)
Description
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Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms1_epd_eis_srvy_l2_phxtof_duration]
      
      
      Instrument Deadtime [mms1_epd_eis_srvy_l2_phxtof_deadtime]
      
      
      Instrument Large Pixel in Use [mms1_epd_eis_srvy_l2_phxtof_largepixel]
      
      
      Spin [mms1_epd_eis_srvy_l2_phxtof_spin]
      
      
      Sector [mms1_epd_eis_srvy_l2_phxtof_sector]
      
      
      Quality Word [mms1_epd_eis_srvy_l2_phxtof_quality]
      
      
      MMS1 PhxTOF-Survey proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_counts_t5]
      
      
      MMS1 PhxTOF-Survey proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_cps_t5]
      
      
      MMS1 PhxTOF-Survey proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms1_epd_eis_srvy_l2_phxtof_proton_P6_flux_t5]
      
      
      MMS1 PhxTOF-Survey oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t5]
      
      
      MMS1 PhxTOF-Survey oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t5]
      
      
      MMS1 PhxTOF-Survey oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t5]
      
      
      MMS1 PhxTOF-Survey dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_counts_t5]
      
      
      MMS1 PhxTOF-Survey dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_cps_t5]
      
      
      MMS1 PhxTOF-Survey dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms1_epd_eis_srvy_l2_phxtof_dump_P6_flux_t5]
      
      
      MMS1 PhxTOF-Survey proton_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_counts_t5]
      
      
      MMS1 PhxTOF-Survey proton_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_cps_t5]
      
      
      MMS1 PhxTOF-Survey proton_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms1_epd_eis_srvy_l2_phxtof_proton_P5_flux_t5]
      
      
      MMS1 PhxTOF-Survey oxygen_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t5]
      
      
      MMS1 PhxTOF-Survey oxygen_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t5]
      
      
      MMS1 PhxTOF-Survey oxygen_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t5]
      
      
      MMS1 PhxTOF-Survey proton_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_phxtof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_counts_t5]
      
      
      MMS1 PhxTOF-Survey proton_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_phxtof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_cps_t5]
      
      
      MMS1 PhxTOF-Survey proton_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_phxtof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms1_epd_eis_srvy_l2_phxtof_proton_P4_flux_t5]
      
      
      MMS1 PhxTOF-Survey oxygen_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t5]
      
      
      MMS1 PhxTOF-Survey oxygen_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t5]
      
      
      MMS1 PhxTOF-Survey oxygen_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t5]
      
      
      MMS1 PhxTOF-Survey proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_phxtof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_counts_t5]
      
      
      MMS1 PhxTOF-Survey proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_phxtof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_cps_t5]
      
      
      MMS1 PhxTOF-Survey proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_phxtof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms1_epd_eis_srvy_l2_phxtof_proton_P3_flux_t5]
      
      
      MMS1 PhxTOF-Survey oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t5]
      
      
      MMS1 PhxTOF-Survey oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t5]
      
      
      MMS1 PhxTOF-Survey oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms1_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t5]
      
      
      MMS1 PhxTOF-Survey dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_phxtof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_counts_t5]
      
      
      MMS1 PhxTOF-Survey dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_phxtof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_counts_t5]
      
      
      MMS1 PhxTOF-Survey dump_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_counts_t5]
      
      
      MMS1 PhxTOF-Survey dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_phxtof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_cps_t5]
      
      
      MMS1 PhxTOF-Survey dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_phxtof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_cps_t5]
      
      
      MMS1 PhxTOF-Survey dump_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_cps_t5]
      
      
      MMS1 PhxTOF-Survey dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms1_epd_eis_srvy_l2_phxtof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms1_epd_eis_srvy_l2_phxtof_dump_P3_flux_t5]
      
      
      MMS1 PhxTOF-Survey dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms1_epd_eis_srvy_l2_phxtof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms1_epd_eis_srvy_l2_phxtof_dump_P4_flux_t5]
      
      
      MMS1 PhxTOF-Survey dump_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms1_epd_eis_srvy_l2_phxtof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms1_epd_eis_srvy_l2_phxtof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS1 [mms1_epd_eis_srvy_l2_phxtof_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS1 [mms1_epd_eis_srvy_l2_phxtof_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS1 [mms1_epd_eis_srvy_l2_phxtof_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS1 [mms1_epd_eis_srvy_l2_phxtof_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS1 [mms1_epd_eis_srvy_l2_phxtof_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS1 [mms1_epd_eis_srvy_l2_phxtof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS1 [mms1_epd_eis_srvy_l2_phxtof_look_t0]
      
      
      Look Direction for Telescope 1 MMS1 [mms1_epd_eis_srvy_l2_phxtof_look_t1]
      
      
      Look Direction for Telescope 2 MMS1 [mms1_epd_eis_srvy_l2_phxtof_look_t2]
      
      
      Look Direction for Telescope 3 MMS1 [mms1_epd_eis_srvy_l2_phxtof_look_t3]
      
      
      Look Direction for Telescope 4 MMS1 [mms1_epd_eis_srvy_l2_phxtof_look_t4]
      
      
      Look Direction for Telescope 5 MMS1 [mms1_epd_eis_srvy_l2_phxtof_look_t5]
      
      
      Magnetic Field BCS MMS1 [mms1_epd_eis_srvy_l2_phxtof_b]
      
      
      Spacecraft position GSE MMS1 [mms1_epd_eis_srvy_l2_phxtof_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS1 [mms1_epd_eis_srvy_l2_phxtof_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS1 [mms1_epd_eis_srvy_l2_phxtof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS1 [mms1_epd_eis_srvy_l2_phxtof_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS1 [mms1_epd_eis_srvy_l2_phxtof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS1 [mms1_epd_eis_srvy_l2_phxtof_r]
      
      
      Dipole L-shell MMS1 [mms1_epd_eis_srvy_l2_phxtof_l]
      
      
      Latitude in GSE Frame MMS1 [mms1_epd_eis_srvy_l2_phxtof_gse_lat]
      
      
      Longitude in GSE Frame MMS1 [mms1_epd_eis_srvy_l2_phxtof_gse_lon]
      
      
      Latitude in GSM Frame MMS1 [mms1_epd_eis_srvy_l2_phxtof_gsm_lat]
      
      
      Longitude in GSM Frame MMS1 [mms1_epd_eis_srvy_l2_phxtof_gsm_lon]
      
      
      Latitude in SM Frame MMS1 [mms1_epd_eis_srvy_l2_phxtof_sm_lat]
      
      
      Longitude in SM Frame MMS1 [mms1_epd_eis_srvy_l2_phxtof_sm_lon]
      
      
      Orbit number MMS1 [mms1_epd_eis_srvy_l2_phxtof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS1 [mms1_epd_eis_srvy_l2_phxtof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS1 [mms1_epd_eis_srvy_l2_phxtof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS1 [mms1_epd_eis_srvy_l2_phxtof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS1 [mms1_epd_eis_srvy_l2_phxtof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS1 [mms1_epd_eis_srvy_l2_phxtof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS1 [mms1_epd_eis_srvy_l2_phxtof_ssd5]
      
      
      Valid Events Processed per second MMS1 [mms1_epd_eis_srvy_l2_phxtof_vep]
      
      
      Start 0 Anode Count Rate MMS1 [mms1_epd_eis_srvy_l2_phxtof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS1 [mms1_epd_eis_srvy_l2_phxtof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS1 [mms1_epd_eis_srvy_l2_phxtof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS1 [mms1_epd_eis_srvy_l2_phxtof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS1 [mms1_epd_eis_srvy_l2_phxtof_vtofxphe]
      
      
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MMS1_FEEPS_BRST_L2_ELECTRON (spase://NASA/NumericalData/MMS/1/EnergeticParticleDetector/FEEPS/Burst/Level2/Electron/PT0.3025S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms1_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms1_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms1_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms1_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms1_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms1_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms1_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms1_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms1_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_12]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms1_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms1_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms1_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms1_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms1_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms1_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms1_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms1_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms1_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_12]
      
      
      MMS1 FEEPS top side burst mode electron count rate sensor 1 [mms1_epd_feeps_brst_l2_electron_top_count_rate_sensorid_1]
      
      
      MMS1 FEEPS top side burst mode electron count rate sensor 2 [mms1_epd_feeps_brst_l2_electron_top_count_rate_sensorid_2]
      
      
      MMS1 FEEPS top side burst mode electron count rate sensor 3 [mms1_epd_feeps_brst_l2_electron_top_count_rate_sensorid_3]
      
      
      MMS1 FEEPS top side burst mode electron count rate sensor 4 [mms1_epd_feeps_brst_l2_electron_top_count_rate_sensorid_4]
      
      
      MMS1 FEEPS top side burst mode electron count rate sensor 5 [mms1_epd_feeps_brst_l2_electron_top_count_rate_sensorid_5]
      
      
      MMS1 FEEPS top side burst mode electron count rate sensor 9 [mms1_epd_feeps_brst_l2_electron_top_count_rate_sensorid_9]
      
      
      MMS1 FEEPS top side burst mode electron count rate sensor 10 [mms1_epd_feeps_brst_l2_electron_top_count_rate_sensorid_10]
      
      
      MMS1 FEEPS top side burst mode electron count rate sensor 11 [mms1_epd_feeps_brst_l2_electron_top_count_rate_sensorid_11]
      
      
      MMS1 FEEPS top side burst mode electron count rate sensor 12 [mms1_epd_feeps_brst_l2_electron_top_count_rate_sensorid_12]
      
      
      MMS1 FEEPS bottom side burst mode electron count rate sensor 1 [mms1_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_1]
      
      
      MMS1 FEEPS bottom side burst mode electron count rate sensor 2 [mms1_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_2]
      
      
      MMS1 FEEPS bottom side burst mode electron count rate sensor 3 [mms1_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_3]
      
      
      MMS1 FEEPS bottom side burst mode electron count rate sensor 4 [mms1_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_4]
      
      
      MMS1 FEEPS bottom side burst mode electron count rate sensor 5 [mms1_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_5]
      
      
      MMS1 FEEPS bottom side burst mode electron count rate sensor 9 [mms1_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_9]
      
      
      MMS1 FEEPS bottom side burst mode electron count rate sensor 10 [mms1_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_10]
      
      
      MMS1 FEEPS bottom side burst mode electron count rate sensor 11 [mms1_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_11]
      
      
      MMS1 FEEPS bottom side burst mode electron count rate sensor 12 [mms1_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_12]
      
      
      MMS1 FEEPS top side burst mode electron intensity sensor 1 [mms1_epd_feeps_brst_l2_electron_top_intensity_sensorid_1]
      
      
      MMS1 FEEPS top side burst mode electron intensity sensor 2 [mms1_epd_feeps_brst_l2_electron_top_intensity_sensorid_2]
      
      
      MMS1 FEEPS top side burst mode electron intensity sensor 3 [mms1_epd_feeps_brst_l2_electron_top_intensity_sensorid_3]
      
      
      MMS1 FEEPS top side burst mode electron intensity sensor 4 [mms1_epd_feeps_brst_l2_electron_top_intensity_sensorid_4]
      
      
      MMS1 FEEPS top side burst mode electron intensity sensor 5 [mms1_epd_feeps_brst_l2_electron_top_intensity_sensorid_5]
      
      
      MMS1 FEEPS top side burst mode electron intensity sensor 9 [mms1_epd_feeps_brst_l2_electron_top_intensity_sensorid_9]
      
      
      MMS1 FEEPS top side burst mode electron intensity sensor 10 [mms1_epd_feeps_brst_l2_electron_top_intensity_sensorid_10]
      
      
      MMS1 FEEPS top side burst mode electron intensity sensor 11 [mms1_epd_feeps_brst_l2_electron_top_intensity_sensorid_11]
      
      
      MMS1 FEEPS top side burst mode electron intensity sensor 12 [mms1_epd_feeps_brst_l2_electron_top_intensity_sensorid_12]
      
      
      MMS1 FEEPS bottom side burst mode electron intensity sensor 1 [mms1_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_1]
      
      
      MMS1 FEEPS bottom side burst mode electron intensity sensor 2 [mms1_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_2]
      
      
      MMS1 FEEPS bottom side burst mode electron intensity sensor 3 [mms1_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_3]
      
      
      MMS1 FEEPS bottom side burst mode electron intensity sensor 4 [mms1_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_4]
      
      
      MMS1 FEEPS bottom side burst mode electron intensity sensor 5 [mms1_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_5]
      
      
      MMS1 FEEPS bottom side burst mode electron intensity sensor 9 [mms1_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_9]
      
      
      MMS1 FEEPS bottom side burst mode electron intensity sensor 10 [mms1_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_10]
      
      
      MMS1 FEEPS bottom side burst mode electron intensity sensor 11 [mms1_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_11]
      
      
      MMS1 FEEPS bottom side burst mode electron intensity sensor 12 [mms1_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_12]
      
      
      MMS1 FEEPS top side burst mode electron count error statistics sensor 1 [mms1_epd_feeps_brst_l2_electron_top_percent_error_sensorid_1]
      
      
      MMS1 FEEPS top side burst mode electron count error statistics sensor 2 [mms1_epd_feeps_brst_l2_electron_top_percent_error_sensorid_2]
      
      
      MMS1 FEEPS top side burst mode electron count error statistics sensor 3 [mms1_epd_feeps_brst_l2_electron_top_percent_error_sensorid_3]
      
      
      MMS1 FEEPS top side burst mode electron count error statistics sensor 4 [mms1_epd_feeps_brst_l2_electron_top_percent_error_sensorid_4]
      
      
      MMS1 FEEPS top side burst mode electron count error statistics sensor 5 [mms1_epd_feeps_brst_l2_electron_top_percent_error_sensorid_5]
      
      
      MMS1 FEEPS top side burst mode electron count error statistics sensor 9 [mms1_epd_feeps_brst_l2_electron_top_percent_error_sensorid_9]
      
      
      MMS1 FEEPS top side burst mode electron count error statistics sensor 10 [mms1_epd_feeps_brst_l2_electron_top_percent_error_sensorid_10]
      
      
      MMS1 FEEPS top side burst mode electron count error statistics sensor 11 [mms1_epd_feeps_brst_l2_electron_top_percent_error_sensorid_11]
      
      
      MMS1 FEEPS top side burst mode electron count error statistics sensor 12 [mms1_epd_feeps_brst_l2_electron_top_percent_error_sensorid_12]
      
      
      MMS1 FEEPS bottom side burst mode electron count error statistics sensor 1 [mms1_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_1]
      
      
      MMS1 FEEPS bottom side burst mode electron count error statistics sensor 2 [mms1_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_2]
      
      
      MMS1 FEEPS bottom side burst mode electron count error statistics sensor 3 [mms1_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_3]
      
      
      MMS1 FEEPS bottom side burst mode electron count error statistics sensor 4 [mms1_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_4]
      
      
      MMS1 FEEPS bottom side burst mode electron count error statistics sensor 5 [mms1_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_5]
      
      
      MMS1 FEEPS bottom side burst mode electron count error statistics sensor 9 [mms1_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_9]
      
      
      MMS1 FEEPS bottom side burst mode electron count error statistics sensor 10 [mms1_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_10]
      
      
      MMS1 FEEPS bottom side burst mode electron count error statistics sensor 11 [mms1_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_11]
      
      
      MMS1 FEEPS bottom side burst mode electron count error statistics sensor 12 [mms1_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_12]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms1_epd_feeps_brst_l2_electron_pitch_angle]
      
      
      Latitude [mms1_epd_feeps_brst_l2_electron_lat_gse]
      
      
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MMS1_FEEPS_BRST_L2_ION (spase://NASA/NumericalData/MMS/1/EnergeticParticleDetector/FEEPS/Burst/Level2/Ion/PT0.3025S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms1_epd_feeps_brst_l2_ion_top_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms1_epd_feeps_brst_l2_ion_top_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms1_epd_feeps_brst_l2_ion_top_quality_indicator_sensorid_8]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms1_epd_feeps_brst_l2_ion_bottom_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms1_epd_feeps_brst_l2_ion_bottom_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms1_epd_feeps_brst_l2_ion_bottom_quality_indicator_sensorid_8]
      
      
      MMS1 FEEPS top side burst mode ion count rate sensor 6 [mms1_epd_feeps_brst_l2_ion_top_count_rate_sensorid_6]
      
      
      MMS1 FEEPS top side burst mode ion count rate sensor 7 [mms1_epd_feeps_brst_l2_ion_top_count_rate_sensorid_7]
      
      
      MMS1 FEEPS top side burst mode ion count rate sensor 8 [mms1_epd_feeps_brst_l2_ion_top_count_rate_sensorid_8]
      
      
      MMS1 FEEPS bottom side burst mode ion count rate sensor 6 [mms1_epd_feeps_brst_l2_ion_bottom_count_rate_sensorid_6]
      
      
      MMS1 FEEPS bottom side burst mode ion count rate sensor 7 [mms1_epd_feeps_brst_l2_ion_bottom_count_rate_sensorid_7]
      
      
      MMS1 FEEPS bottom side burst mode ion count rate sensor 8 [mms1_epd_feeps_brst_l2_ion_bottom_count_rate_sensorid_8]
      
      
      MMS1 FEEPS top side burst mode ion intensity sensor 6 [mms1_epd_feeps_brst_l2_ion_top_intensity_sensorid_6]
      
      
      MMS1 FEEPS top side burst mode ion intensity sensor 7 [mms1_epd_feeps_brst_l2_ion_top_intensity_sensorid_7]
      
      
      MMS1 FEEPS top side burst mode ion intensity sensor 8 [mms1_epd_feeps_brst_l2_ion_top_intensity_sensorid_8]
      
      
      MMS1 FEEPS bottom side burst mode ion intensity sensor 6 [mms1_epd_feeps_brst_l2_ion_bottom_intensity_sensorid_6]
      
      
      MMS1 FEEPS bottom side burst mode ion intensity sensor 7 [mms1_epd_feeps_brst_l2_ion_bottom_intensity_sensorid_7]
      
      
      MMS1 FEEPS bottom side burst mode ion intensity sensor 8 [mms1_epd_feeps_brst_l2_ion_bottom_intensity_sensorid_8]
      
      
      MMS1 FEEPS top side burst mode ion count error statistics sensor 6 [mms1_epd_feeps_brst_l2_ion_top_percent_error_sensorid_6]
      
      
      MMS1 FEEPS top side burst mode ion count error statistics sensor 7 [mms1_epd_feeps_brst_l2_ion_top_percent_error_sensorid_7]
      
      
      MMS1 FEEPS top side burst mode ion count error statistics sensor 8 [mms1_epd_feeps_brst_l2_ion_top_percent_error_sensorid_8]
      
      
      MMS1 FEEPS bottom side burst mode ion count error statistics sensor 6 [mms1_epd_feeps_brst_l2_ion_bottom_percent_error_sensorid_6]
      
      
      MMS1 FEEPS bottom side burst mode ion count error statistics sensor 7 [mms1_epd_feeps_brst_l2_ion_bottom_percent_error_sensorid_7]
      
      
      MMS1 FEEPS bottom side burst mode ion count error statistics sensor 8 [mms1_epd_feeps_brst_l2_ion_bottom_percent_error_sensorid_8]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms1_epd_feeps_brst_l2_ion_pitch_angle]
      
      
      Latitude [mms1_epd_feeps_brst_l2_ion_lat_gse]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS1_FEEPS_SRVY_L2_ELECTRON (spase://NASA/NumericalData/MMS/1/EnergeticParticleDetector/FEEPS/Survey/Level2/Electron/PT2.42S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms1_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms1_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms1_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms1_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms1_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms1_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms1_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms1_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms1_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_12]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms1_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms1_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms1_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms1_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms1_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms1_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms1_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms1_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms1_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_12]
      
      
      MMS1 FEEPS top side survey mode electron count rate sensor 1 [mms1_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_1]
      
      
      MMS1 FEEPS top side survey mode electron count rate sensor 2 [mms1_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_2]
      
      
      MMS1 FEEPS top side survey mode electron count rate sensor 3 [mms1_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_3]
      
      
      MMS1 FEEPS top side survey mode electron count rate sensor 4 [mms1_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_4]
      
      
      MMS1 FEEPS top side survey mode electron count rate sensor 5 [mms1_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_5]
      
      
      MMS1 FEEPS top side survey mode electron count rate sensor 9 [mms1_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_9]
      
      
      MMS1 FEEPS top side survey mode electron count rate sensor 10 [mms1_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_10]
      
      
      MMS1 FEEPS top side survey mode electron count rate sensor 11 [mms1_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_11]
      
      
      MMS1 FEEPS top side survey mode electron count rate sensor 12 [mms1_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_12]
      
      
      MMS1 FEEPS bottom side survey mode electron count rate sensor 1 [mms1_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_1]
      
      
      MMS1 FEEPS bottom side survey mode electron count rate sensor 2 [mms1_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_2]
      
      
      MMS1 FEEPS bottom side survey mode electron count rate sensor 3 [mms1_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_3]
      
      
      MMS1 FEEPS bottom side survey mode electron count rate sensor 4 [mms1_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_4]
      
      
      MMS1 FEEPS bottom side survey mode electron count rate sensor 5 [mms1_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_5]
      
      
      MMS1 FEEPS bottom side survey mode electron count rate sensor 9 [mms1_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_9]
      
      
      MMS1 FEEPS bottom side survey mode electron count rate sensor 10 [mms1_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_10]
      
      
      MMS1 FEEPS bottom side survey mode electron count rate sensor 11 [mms1_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_11]
      
      
      MMS1 FEEPS bottom side survey mode electron count rate sensor 12 [mms1_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_12]
      
      
      MMS1 FEEPS top side survey mode electron intensity sensor 1 [mms1_epd_feeps_srvy_l2_electron_top_intensity_sensorid_1]
      
      
      MMS1 FEEPS top side survey mode electron intensity sensor 2 [mms1_epd_feeps_srvy_l2_electron_top_intensity_sensorid_2]
      
      
      MMS1 FEEPS top side survey mode electron intensity sensor 3 [mms1_epd_feeps_srvy_l2_electron_top_intensity_sensorid_3]
      
      
      MMS1 FEEPS top side survey mode electron intensity sensor 4 [mms1_epd_feeps_srvy_l2_electron_top_intensity_sensorid_4]
      
      
      MMS1 FEEPS top side survey mode electron intensity sensor 5 [mms1_epd_feeps_srvy_l2_electron_top_intensity_sensorid_5]
      
      
      MMS1 FEEPS top side survey mode electron intensity sensor 9 [mms1_epd_feeps_srvy_l2_electron_top_intensity_sensorid_9]
      
      
      MMS1 FEEPS top side survey mode electron intensity sensor 10 [mms1_epd_feeps_srvy_l2_electron_top_intensity_sensorid_10]
      
      
      MMS1 FEEPS top side survey mode electron intensity sensor 11 [mms1_epd_feeps_srvy_l2_electron_top_intensity_sensorid_11]
      
      
      MMS1 FEEPS top side survey mode electron intensity sensor 12 [mms1_epd_feeps_srvy_l2_electron_top_intensity_sensorid_12]
      
      
      MMS1 FEEPS bottom side survey mode electron intensity sensor 1 [mms1_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_1]
      
      
      MMS1 FEEPS bottom side survey mode electron intensity sensor 2 [mms1_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_2]
      
      
      MMS1 FEEPS bottom side survey mode electron intensity sensor 3 [mms1_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_3]
      
      
      MMS1 FEEPS bottom side survey mode electron intensity sensor 4 [mms1_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_4]
      
      
      MMS1 FEEPS bottom side survey mode electron intensity sensor 5 [mms1_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_5]
      
      
      MMS1 FEEPS bottom side survey mode electron intensity sensor 9 [mms1_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_9]
      
      
      MMS1 FEEPS bottom side survey mode electron intensity sensor 10 [mms1_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_10]
      
      
      MMS1 FEEPS bottom side survey mode electron intensity sensor 11 [mms1_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_11]
      
      
      MMS1 FEEPS bottom side survey mode electron intensity sensor 12 [mms1_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_12]
      
      
      MMS1 FEEPS top side survey mode electron count error statistics sensor 1 [mms1_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_1]
      
      
      MMS1 FEEPS top side survey mode electron count error statistics sensor 2 [mms1_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_2]
      
      
      MMS1 FEEPS top side survey mode electron count error statistics sensor 3 [mms1_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_3]
      
      
      MMS1 FEEPS top side survey mode electron count error statistics sensor 4 [mms1_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_4]
      
      
      MMS1 FEEPS top side survey mode electron count error statistics sensor 5 [mms1_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_5]
      
      
      MMS1 FEEPS top side survey mode electron count error statistics sensor 9 [mms1_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_9]
      
      
      MMS1 FEEPS top side survey mode electron count error statistics sensor 10 [mms1_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_10]
      
      
      MMS1 FEEPS top side survey mode electron count error statistics sensor 11 [mms1_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_11]
      
      
      MMS1 FEEPS top side survey mode electron count error statistics sensor 12 [mms1_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_12]
      
      
      MMS1 FEEPS bottom side survey mode electron count error statistics sensor 1 [mms1_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_1]
      
      
      MMS1 FEEPS bottom side survey mode electron count error statistics sensor 2 [mms1_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_2]
      
      
      MMS1 FEEPS bottom side survey mode electron count error statistics sensor 3 [mms1_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_3]
      
      
      MMS1 FEEPS bottom side survey mode electron count error statistics sensor 4 [mms1_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_4]
      
      
      MMS1 FEEPS bottom side survey mode electron count error statistics sensor 5 [mms1_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_5]
      
      
      MMS1 FEEPS bottom side survey mode electron count error statistics sensor 9 [mms1_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_9]
      
      
      MMS1 FEEPS bottom side survey mode electron count error statistics sensor 10 [mms1_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_10]
      
      
      MMS1 FEEPS bottom side survey mode electron count error statistics sensor 11 [mms1_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_11]
      
      
      MMS1 FEEPS bottom side survey mode electron count error statistics sensor 12 [mms1_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_12]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms1_epd_feeps_srvy_l2_electron_pitch_angle]
      
      
      Latitude [mms1_epd_feeps_srvy_l2_electron_lat_gse]
      
      
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MMS1_FEEPS_SRVY_L2_ION (spase://NASA/NumericalData/MMS/1/EnergeticParticleDetector/FEEPS/Survey/Level2/Ion/PT2.42S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms1_epd_feeps_srvy_l2_ion_top_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms1_epd_feeps_srvy_l2_ion_top_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms1_epd_feeps_srvy_l2_ion_top_quality_indicator_sensorid_8]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms1_epd_feeps_srvy_l2_ion_bottom_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms1_epd_feeps_srvy_l2_ion_bottom_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms1_epd_feeps_srvy_l2_ion_bottom_quality_indicator_sensorid_8]
      
      
      MMS1 FEEPS top side survey mode ion count rate sensor 6 [mms1_epd_feeps_srvy_l2_ion_top_count_rate_sensorid_6]
      
      
      MMS1 FEEPS top side survey mode ion count rate sensor 7 [mms1_epd_feeps_srvy_l2_ion_top_count_rate_sensorid_7]
      
      
      MMS1 FEEPS top side survey mode ion count rate sensor 8 [mms1_epd_feeps_srvy_l2_ion_top_count_rate_sensorid_8]
      
      
      MMS1 FEEPS bottom side survey mode ion count rate sensor 6 [mms1_epd_feeps_srvy_l2_ion_bottom_count_rate_sensorid_6]
      
      
      MMS1 FEEPS bottom side survey mode ion count rate sensor 7 [mms1_epd_feeps_srvy_l2_ion_bottom_count_rate_sensorid_7]
      
      
      MMS1 FEEPS bottom side survey mode ion count rate sensor 8 [mms1_epd_feeps_srvy_l2_ion_bottom_count_rate_sensorid_8]
      
      
      MMS1 FEEPS top side survey mode ion intensity sensor 6 [mms1_epd_feeps_srvy_l2_ion_top_intensity_sensorid_6]
      
      
      MMS1 FEEPS top side survey mode ion intensity sensor 7 [mms1_epd_feeps_srvy_l2_ion_top_intensity_sensorid_7]
      
      
      MMS1 FEEPS top side survey mode ion intensity sensor 8 [mms1_epd_feeps_srvy_l2_ion_top_intensity_sensorid_8]
      
      
      MMS1 FEEPS bottom side survey mode ion intensity sensor 6 [mms1_epd_feeps_srvy_l2_ion_bottom_intensity_sensorid_6]
      
      
      MMS1 FEEPS bottom side survey mode ion intensity sensor 7 [mms1_epd_feeps_srvy_l2_ion_bottom_intensity_sensorid_7]
      
      
      MMS1 FEEPS bottom side survey mode ion intensity sensor 8 [mms1_epd_feeps_srvy_l2_ion_bottom_intensity_sensorid_8]
      
      
      MMS1 FEEPS top side survey mode ion count error statistics sensor 6 [mms1_epd_feeps_srvy_l2_ion_top_percent_error_sensorid_6]
      
      
      MMS1 FEEPS top side survey mode ion count error statistics sensor 7 [mms1_epd_feeps_srvy_l2_ion_top_percent_error_sensorid_7]
      
      
      MMS1 FEEPS top side survey mode ion count error statistics sensor 8 [mms1_epd_feeps_srvy_l2_ion_top_percent_error_sensorid_8]
      
      
      MMS1 FEEPS bottom side survey mode ion count error statistics sensor 6 [mms1_epd_feeps_srvy_l2_ion_bottom_percent_error_sensorid_6]
      
      
      MMS1 FEEPS bottom side survey mode ion count error statistics sensor 7 [mms1_epd_feeps_srvy_l2_ion_bottom_percent_error_sensorid_7]
      
      
      MMS1 FEEPS bottom side survey mode ion count error statistics sensor 8 [mms1_epd_feeps_srvy_l2_ion_bottom_percent_error_sensorid_8]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms1_epd_feeps_srvy_l2_ion_pitch_angle]
      
      
      Latitude [mms1_epd_feeps_srvy_l2_ion_lat_gse]
      
      
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MMS1_FGM_BRST_L2 (spase://NASA/NumericalData/MMS/1/FIELDS/FGM/Burst/Level2/PT0.0078125S)
Description
The Fluxgate Magnetometers (FGM) on Magnetospheric Multiscale consist of a
traditional Analog Fluxgate Magnetometer (AFG), and a Digital Fluxgate
magnetometer (DFG). The dual magnetometers are operated as a single instrument
providing a single intercalibrated data product. Range changes occur at
different times on the two instruments so the gains checked each periapsis can
be carried out unambiguously to apoapsis. Cross correlation of calibration
parameters can separate causes of the any apparent calibration changes. Use of
Electron Drift Instrument (EDI) to determine the field along the rotation axis
allows accurate monitoring of the zero levels along the rotation axis.  Prior to
launch the magnetometers were calibrated at the Technical University,
Braunschweig, except for the AFG magnetometers on MMS3 and MMS4, which were
calibrated at UCLA.  Both sets of sensors are operated for the entire MMS orbit,
with slow survey (8 samples per second) outside of the Region of Interest (ROI),
and fast survey (16 samples per second) inside the ROI. Within the ROI burst
mode data (128 samples per second) are also acquired.  A detailed description of
the MMS fluxgate magnetometers, including science objectives, instrument
description, calibration, magnetic cleanliness program, and data flow can be
found at http://link.springer.com/article/10.1007%2Fs11214-014-0057-3 (DOI 
10.1007/s11214-014-0057-3).Additional information can also be found at
http://www-spc.igpp.ucla.edu/ssc/mms (UCLA),and http://www.iwf.oeaw.ac.at (IWF,
Graz).
For the purpose of creating a unified FGM Level2 data product, burst mode data
is taken from DFG and survey mode data is taken from AFG.  Because AFG and DFG
are cross-calibrated on an orbit-averaged basis, small differences in offset may
be observed between Level2 burst and survey mode data.  Consequently, any
differences are within the error of the measurement. Based on preliminary
analysis of the data, the absolute error within the Region of Interest (ROI) is
estimated to be no more than 0.1 nT in the spin-plane, 0.15 nT along the
spin-axis and 0.2 nT in total magnitude.
Modification History
version X=5:  * Y-version number comes from cal file entries. 
              *
Ensures there are 2 ephemeris points before/after data to enable proper spline. 

              * Fix to depend_0 of rdeltahalf:  fixes bug when reading position
data.
              * L-vector for DMPA2GSE transformation is smoothed with a
gaussian filter, instead 
                of using a single average value for
the day.  This short-term filter avoids  
                introduding artificial
jumps at 00:00 UTC and removes 7-minute 'wobble' after  
               
maneuvers in the GSE result.   
              * Fixes error with DEFATT file
selection found when choosing the 
                daily DEFATT files to be used
in Phase 2.
              * Fixed bug where reference Etemp was used for high
range gain.  Now uses measured Etemp.
version X=4:  First version for public
release of L2.
              Renamed variables to conform with new MMS variable
name guidelines 
              (obs_instr_paramName[_coordSys]_mode_level):  
  
             Mag field parameters include 'b' for paramName.  
               
Use 'r' instead of 'pos' for S/C position paramName.  
               
Eliminated 'rate', replaced with 'bdeltahalf'.  Added 'rdeltahalf'.
            
   l1a_mode is now just 'mode'.
version X=3:  fixed removal of overlap between
modes.
              fixed a bug that caused stemp and etemp to be
empty.
version X=2:  flag parameter name corrected: was 'status'
               
        added bits 4, 5, 6 to flag saturation on B1, B2, and B3, respectively
  
                     added bit 7 to flag bad data at range changes
             
Added etemp and l1a_mode parameters.  
              rate, hirange, and stemp
parameters now comply with MMS CDF Guidlelines, e.g.
              FILLVAL now
defined for stemp and etemp, and is set to !values.f_nan
              No longer
use Var_Parents attribute in stemp -- see Parents instead
              In this
version, temperature-corrected gains are applied.  Reference temperatures are
used when 
              stemp or etemp are set to FILLVAL. 
             
Non-linearity correction is applied to high rage DFG data.
version X=1:  added
'flag', rate and hirange parameters (but 'flag' is actually called 'status')
 
  • Data Variable Descriptions
      Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (128 S/s) [mms1_fgm_b_gse_brst_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms1_fgm_b_gse_brst_l2]
      
      
      Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (128 S/s) [mms1_fgm_b_gsm_brst_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms1_fgm_b_gsm_brst_l2]
      
      
      Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (128 S/s) [mms1_fgm_b_dmpa_brst_l2_clean]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      ---> Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (128 S/s), including flagged data [mms1_fgm_b_dmpa_brst_l2]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (128 S/s) [mms1_fgm_b_bcs_brst_l2_clean]
      
      
      ---> Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (128 S/s), including flagged data [mms1_fgm_b_bcs_brst_l2]
      
      
      Quality Flag: 0 = No identified problems, non-zero = blank out the data [mms1_fgm_flag_brst_l2]
      bit definitions: .    0: TBD, 1: TBD, 2: user flagged, 3: TBD, .    4: B1
      saturated, 5: B2 saturated, 6: B3 saturated, 7: range-change glitch, .    8-31:
      TBD
      
      Definitive Position in GSE coordinates, 30 second [mms1_fgm_r_gse_brst_l2]
      
      
      Definitive Position in GSM coordinates, 30 second [mms1_fgm_r_gsm_brst_l2]
      
      
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MMS1_FGM_SRVY_L2 (spase://NASA/NumericalData/MMS/1/FIELDS/FGM/Survey/Level2/PT0.125S)
Description
The Fluxgate Magnetometers (FGM) on Magnetospheric Multiscale consist of a
traditional Analog Fluxgate Magnetometer (AFG), and a Digital Fluxgate
magnetometer (DFG). The dual magnetometers are operated as a single instrument
providing a single intercalibrated data product. Range changes occur at
different times on the two instruments so the gains checked each periapsis can
be carried out unambiguously to apoapsis. Cross correlation of calibration
parameters can separate causes of the any apparent calibration changes. Use of
Electron Drift Instrument (EDI) to determine the field along the rotation axis
allows accurate monitoring of the zero levels along the rotation axis.  Prior to
launch the magnetometers were calibrated at the Technical University,
Braunschweig, except for the AFG magnetometers on MMS3 and MMS4, which were
calibrated at UCLA.  Both sets of sensors are operated for the entire MMS orbit,
with slow survey (8 samples per second) outside of the Region of Interest (ROI),
and fast survey (16 samples per second) inside the ROI. Within the ROI burst
mode data (128 samples per second) are also acquired.  A detailed description of
the MMS fluxgate magnetometers, including science objectives, instrument
description, calibration, magnetic cleanliness program, and data flow can be
found at http://link.springer.com/article/10.1007%2Fs11214-014-0057-3 (DOI 
10.1007/s11214-014-0057-3).Additional information can also be found at
http://www-spc.igpp.ucla.edu/ssc/mms (UCLA),and http://www.iwf.oeaw.ac.at (IWF,
Graz).
For the purpose of creating a unified FGM Level2 data product, burst mode data
is taken from DFG and survey mode data is taken from AFG.  Because AFG and DFG
are cross-calibrated on an orbit-averaged basis, small differences in offset may
be observed between Level2 burst and survey mode data.  Consequently, any
differences are within the error of the measurement. Based on preliminary
analysis of the data, the absolute error within the Region of Interest (ROI) is
estimated to be no more than 0.1 nT in the spin-plane, 0.15 nT along the
spin-axis and 0.2 nT in total magnitude.
Modification History
version X=5:  * Y-version number comes from cal file entries. 
              *
Ensures there are 2 ephemeris points before/after data to enable proper spline. 

              * Fix to depend_0 of rdeltahalf:  fixes bug when reading position
data.
              * L-vector for DMPA2GSE transformation is smoothed with a
gaussian filter, instead 
                of using a single average value for
the day.  This short-term filter avoids  
                introduding artificial
jumps at 00:00 UTC and removes 7-minute 'wobble' after  
               
maneuvers in the GSE result.   
              * Fixes error with DEFATT file
selection found when choosing the 
                daily DEFATT files to be used
in Phase 2.
              * Fixed bug where reference Etemp was used for high
range gain.  Now uses measured Etemp.
version X=4:  First version for public
release of L2.
              Renamed variables to conform with new MMS variable
name guidelines 
              (obs_instr_paramName[_coordSys]_mode_level):  
  
             Mag field parameters include 'b' for paramName.  
               
Use 'r' instead of 'pos' for S/C position paramName.  
               
Eliminated 'rate', replaced with 'bdeltahalf'.  Added 'rdeltahalf'.
            
   l1a_mode is now just 'mode'.
version X=3:  fixed removal of overlap between
modes.
              fixed a bug that caused stemp and etemp to be
empty.
version X=2:  flag parameter name corrected: was 'status'
               
        added bits 4, 5, 6 to flag saturation on B1, B2, and B3, respectively
  
                     added bit 7 to flag bad data at range changes
             
Added etemp and l1a_mode parameters.  
              rate, hirange, and stemp
parameters now comply with MMS CDF Guidlelines, e.g.
              FILLVAL now
defined for stemp and etemp, and is set to !values.f_nan
              No longer
use Var_Parents attribute in stemp -- see Parents instead
              In this
version, temperature-corrected gains are applied.  Reference temperatures are
used when 
              stemp or etemp are set to FILLVAL. 
             
Non-linearity correction is applied to high rage DFG data.
version X=1:  added
'flag', rate and hirange parameters (but 'flag' is actually called 'status')
 
  • Data Variable Descriptions
      Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (8 or 16 S/s) [mms1_fgm_b_gse_srvy_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms1_fgm_b_gse_srvy_l2]
      
      
      Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (8 or 16 S/s) [mms1_fgm_b_gsm_srvy_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms1_fgm_b_gsm_srvy_l2]
      
      
      Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (8 or 16 S/s) [mms1_fgm_b_dmpa_srvy_l2_clean]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      ---> Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms1_fgm_b_dmpa_srvy_l2]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (8 or 16 S/s) [mms1_fgm_b_bcs_srvy_l2_clean]
      
      
      ---> Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms1_fgm_b_bcs_srvy_l2]
      
      
      Quality Flag: 0 = No identified problems, non-zero = blank out the data [mms1_fgm_flag_srvy_l2]
      bit definitions: .    0: TBD, 1: TBD, 2: user flagged, 3: TBD, .    4: B1
      saturated, 5: B2 saturated, 6: B3 saturated, 7: range-change glitch, .    8-31:
      TBD
      
      Definitive Position in GSE coordinates, 30 second [mms1_fgm_r_gse_srvy_l2]
      
      
      Definitive Position in GSM coordinates, 30 second [mms1_fgm_r_gsm_srvy_l2]
      
      
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MMS1_FPI_BRST_L2_DES-DIST (spase://NASA/NumericalData/MMS/1/FastPlasmaInvestigation/DES/Burst/Level2/Distribution/PT0.03S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data are taken at burst (30/150 ms for DES/DIS)
resolution in this mode.  Data are also made available at survey (4.5 s, etc)
resolution; these form a separate product from this.  Per mission design, not
all burst-resolution data are downlinked.  This product contains phase-space
distribution maps of those burst-resolution data selected for downlink.  In
particular, the (highest possible quality at the time of release)
corrected/converted "Burst SkyMap" distributions are reported with time-stamps
and other annotation characterizing the state of the instrument system at the
indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      [CDAWeb List/Download/Create ONLY] MMS1 FPI/DES burst sky-map instrument distribution [mms1_des_dist_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 10.9 eV (E1/even) [mms1_des_dist_brst1_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 12.4 eV (E1/odd) [mms1_des_dist_brst1_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~11.6 eV (E1 even-odd) [mms1_des_dist_brst1_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 10.9 eV (E1/even) [mms1_des_dist_brst1_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 12.4 eV (E1/odd) [mms1_des_dist_brst1_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 37.9 eV (E6/even) [mms1_des_dist_brst6_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 42.9 eV (E6/odd) [mms1_des_dist_brst6_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~40.4 eV (E6 even-odd) [mms1_des_dist_brst6_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 37.9 eV (E6/even) [mms1_des_dist_brst6_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 42.9 eV (E6/odd) [mms1_des_dist_brst6_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 80.0 eV (E9/even) [mms1_des_dist_brst9_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 90.6 eV (E9/odd) [mms1_des_dist_brst9_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~85 eV (E9 even-odd) [mms1_des_dist_brst9_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 80.0 eV (E9/even) [mms1_des_dist_brst9_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 90.6 eV (E9/odd) [mms1_des_dist_brst9_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 169 eV (E12/even) [mms1_des_dist_brst12_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 191 eV (E12/odd) [mms1_des_dist_brst12_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~180 eV (E12 even-odd) [mms1_des_dist_brst12_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 169 eV (E12/even) [mms1_des_dist_brst12_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 191 eV (E12/odd) [mms1_des_dist_brst12_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 277 eV (E14/even) [mms1_des_dist_brst14_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 314 eV (E14/odd) [mms1_des_dist_brst14_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~295 eV (E14 even-odd) [mms1_des_dist_brst14_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 277 eV (E14/even) [mms1_des_dist_brst14_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 314 eV (E14/odd) [mms1_des_dist_brst14_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 456 eV (E16/even) [mms1_des_dist_brst16_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 517 eV (E16/odd) [mms1_des_dist_brst16_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~485 eV (E16 even-odd) [mms1_des_dist_brst16_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 456 eV (E16/even) [mms1_des_dist_brst16_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 517 eV (E16/odd) [mms1_des_dist_brst16_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 750 eV (E18/even) [mms1_des_dist_brst18_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 850 eV (E18/odd) [mms1_des_dist_brst18_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~800 eV (E18 even-odd) [mms1_des_dist_brst18_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 750 eV (E18/even) [mms1_des_dist_brst18_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 850 eV (E18/odd) [mms1_des_dist_brst18_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 1230 eV (E20/even) [mms1_des_dist_brst20_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 1400 eV (E20/odd) [mms1_des_dist_brst20_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~1310 eV (E20 even-odd) [mms1_des_dist_brst20_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1230 eV (E20/even) [mms1_des_dist_brst20_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1400 eV (E20/odd) [mms1_des_dist_brst20_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 2600 eV (E23/even) [mms1_des_dist_brst23_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 2950 eV (E23/odd) [mms1_des_dist_brst23_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~2770 eV (E23 even-odd) [mms1_des_dist_brst23_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2600 eV (E23/even) [mms1_des_dist_brst23_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2950 eV (E23/odd) [mms1_des_dist_brst23_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 5490 eV (E26/even) [mms1_des_dist_brst26_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 6210 eV (E26/odd) [mms1_des_dist_brst26_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~5840 eV (E26 even-odd) [mms1_des_dist_brst26_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5490 eV (E26/even) [mms1_des_dist_brst26_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 6210 eV (E26/odd) [mms1_des_dist_brst26_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 24400 eV (E32/even) [mms1_des_dist_brst32_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst sky-map instrument distribution - 27600 eV (E32/odd) [mms1_des_dist_brst32_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~26000 eV (E32 even-odd) [mms1_des_dist_brst32_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 24400 eV (E32/even) [mms1_des_dist_brst32_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 27600 eV (E32/odd) [mms1_des_dist_brst32_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [List/Create only in CDAWeb] 1-sigma error: MMS1 FPI/DES burst sky-map instrument distribution [mms1_des_disterr_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES burst average f1 count values [mms1_des_avgf1counts_brst]
      Average f1-count level as a function of energy
      
      MMS1 FPI/DES burst sky-map microsecond offsets from Epoch [mms1_des_steptimeoffsets_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order. Offsets reflect 128 steps over the 30 msec sweep
      period. See FPI docs for details.
      
      MMS1 FPI/DES vector of data-quality indicators at burst-start time [mms1_des_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS1 FPI/DES compression lossless/lossy indicator at survey-start time [mms1_des_compressionloss_brst]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS1 FPI/DES step table parity, this burst [mms1_des_steptable_parity_brst]
      FPI/DES alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS1 FPI/DES Del-Phi (obs spin-phase) count at burst-start time [mms1_des_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS1 FPI/DES Del-Phi (obs spin-phase) angle at burst-start time [mms1_des_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      ---> MMS1 FPI/DES sector de-Spin P value, this burst [mms1_des_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS1 FPI/DES burst sky-map instrument azimuthal angles [mms1_des_phi_brst]
      see FPI docs for details
      
      MMS FPI/DES burst sky-map parity 0/1 energies [mms1_des_energy_brst]
      Energies (parity 0/1) in the 64-step FPI energy table
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS1_FPI_BRST_L2_DES-MOMS (spase://NASA/NumericalData/MMS/1/FastPlasmaInvestigation/DES/Burst/Level2/Moments/PT0.03S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode.  Data are also made available at survey (4.5
s, etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked.  Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available.  This product contains results from
integrating the standard moments of phase-space distributions formed from the
indicated data type (DES/DIS burst, FS or SS).  For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DES 32-bit vector of data-quality indicators at burst-start time [mms1_des_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>25%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied
      
      ---> MMS1 FPI/DES compression lossless/lossy indicator at survey-start time [mms1_des_compressionloss_brst]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS1 FPI/DES step table parity, this burst [mms1_des_steptable_parity_brst]
      FPI/DES alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS1 FPI/DES Del-Phi (obs spin-phase) count at burst-start time [mms1_des_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS1 FPI/DES Del-Phi (obs spin-phase) angle at burst-start time [mms1_des_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      ---> MMS1 FPI/DES sector de-Spin P value, this burst [mms1_des_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS1 FPI/DES electron pitch-angle distribution for "low" energies during this burst [mms1_des_pitchangdist_lowen_brst]
      low energy bin: 0 eV - 200 eV.  pitch-angle bin size: 6 deg.
      
      ---> MMS1 FPI/DES electron pitch-angle distribution for "mid" energies during this burst [mms1_des_pitchangdist_miden_brst]
      mid energy bin: 200 eV - 2 keV.  pitch-angle bin size: 6 deg.
      
      ---> MMS1 FPI/DES electron pitch-angle distribution for "high" energies during this burst [mms1_des_pitchangdist_highen_brst]
      high energy bin: 2 keV - 30 keV.  pitch-angle bin size: 6 deg.
      
      MMS1 FPI/DES electron energy spectrum "near" +X_DSC during this burst [mms1_des_energyspectr_px_brst]
      Counts, summed over DSC velocity-dirs closest to +X_DSC, by energy bin.
      
      ---> MMS1 FPI/DES electron energy spectrum "near" -X_DSC during this burst [mms1_des_energyspectr_mx_brst]
      Counts, summed over DSC velocity-dirs closest to -X_DSC, by energy bin.
      
      ---> MMS1 FPI/DES electron energy spectrum "near" +Y_DSC during this burst [mms1_des_energyspectr_py_brst]
      Counts, summed over DSC velocity-dirs closest to +Y_DSC, by energy bin.
      
      ---> MMS1 FPI/DES electron energy spectrum "near" -Y_DSC during this burst [mms1_des_energyspectr_my_brst]
      Counts, summed over DSC velocity-dirs closest to -Y_DSC, by energy bin.
      
      ---> MMS1 FPI/DES electron energy spectrum "near" +Z_DSC during this burst [mms1_des_energyspectr_pz_brst]
      Counts, summed over DSC velocity-dirs closest to +Z_DSC, by energy bin.
      
      ---> MMS1 FPI/DES electron energy spectrum "near" -Z_DSC during this burst [mms1_des_energyspectr_mz_brst]
      Counts, summed over DSC velocity-dirs closest to -Z_DSC, by energy bin.
      
      MMS1 FPI/DES electron energy parallel spectrum 30 degrees parallel to B during this burst [mms1_des_energyspectr_par_brst]
      Counts, summed within 30 degrees parallel bentPipe magnetic field.
      
      ---> MMS1 FPI/DES electron energy anti-parallel spectrum 30 degrees anti-parallel to B during this burst [mms1_des_energyspectr_anti_brst]
      Counts, summed within 30 degrees antiparallel to bentPipe magnetic field.
      
      ---> MMS1 FPI/DES electron energy perpendicular spectrum 60 degrees perpendicular to B during this burst [mms1_des_energyspectr_perp_brst]
      Counts, summed within 60 degrees perpendicular to bentPipe magnetic field.
      
      MMS1 FPI/DES omni-directional electron energy spectrum during this burst [mms1_des_energyspectr_omni_brst]
      Differential energy flux, averaged (weighted by solid angle) over all look
      directions, by energy bin.
      
      MMS1 FPI/DES electron number density during this burst [mms1_des_numberdensity_brst]
      
      
      ---> (no error bars displayed) MMS1 FPI/DES electron number density during this burst [mms1_des_numberdensity_brst_noerr]
      
      
      ---> MMS1 FPI/DES electron number density error during this burst [mms1_des_numberdensity_err_brst]
      
      
      MMS1 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms1_des_densityextrapolation_low_brst]
      
      
      MMS1 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms1_des_densityextrapolation_high_brst]
      
      
      MMS1 FPI/DES electron bulk-velocity DBCS vector during this burst [mms1_des_bulkv_dbcs_brst]
      
      
      MMS1 FPI/DES electron bulk-velocity estimated spintone vector in DBCS during this burst [mms1_des_bulkv_spintone_dbcs_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS1 FPI/DES electron bulk-velocity DBCS vector during this burst [mms1_des_bulkv_dbcs_brst_noerr]
      
      
      MMS1 FPI/DES electron bulk-velocity GSE vector during this burst [mms1_des_bulkv_gse_brst]
      
      
      MMS1 FPI/DES electron bulk-velocity estimated spintone vector in GSE during this burst [mms1_des_bulkv_spintone_gse_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS1 FPI/DES electron bulk-velocity GSE vector during this burst [mms1_des_bulkv_gse_brst_noerr]
      
      
      MMS1 FPI/DES electron bulk-velocity spintone vector in DBCS during this burst [mms1_des_bulkv_spin_dbcs_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS1 FPI/DES electron bulk-velocity spintone vector in GSE during this burst [mms1_des_bulkv_spin_gse_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS1 FPI/DES electron pressure tensor DBCS matrix during this burst [mms1_des_prestensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES electron pressure tensor GSE matrix during this burst [mms1_des_prestensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES electron temperature tensor DBCS matrix during this burst [mms1_des_temptensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES electron temperature tensor GSE matrix during this burst [mms1_des_temptensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES electron heat-flux DBCS vector during this burst [mms1_des_heatq_dbcs_brst]
      
      
      MMS1 FPI/DES electron heat-flux GSE vector during this burst [mms1_des_heatq_gse_brst]
      
      
      MMS1 FPI/DES electron parallel temperature during this BP [mms1_des_temppara_brst]
      
      
      MMS1 FPI/DES electron perpendicular temperature during this BP [mms1_des_tempperp_brst]
      
      
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MMS1_FPI_BRST_L2_DES-PARTMOMS (spase://NASA/NumericalData/MMS/1/FastPlasmaInvestigation/DES/Burst/Level2/PartialMoments/PT0.03S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s,
etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked. Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available. This product contains partial moments that
come from performing the standard moment integrals over a limited portion of
velocity space. The resulting quantities are named similarly to their
corresponding standard moments, but are decorated with 'part' to differentiate.
For example, density_part is the density moment integrated from a particular
energy step to infinity. These partial moments are formed from the indicated
data type (DES/DIS burst, FS or SS). For convenience, some additional parameters
are included to augment those most commonly found in a moments product of this
sort, plus time-stamps and other annotation characterizing the state of the
instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DES vector of data-quality indicators at burst-start time [mms1_des_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only)
      
      MMS1 FPI/DES partial electron number density during this burst [mms1_des_numberdensity_part_brst]
      
      
      MMS1 FPI/DES partial electron bulk-velocity vector in DBCS during this burst [mms1_des_bulkv_part_dbcs_brst]
      
      
      MMS1 FPI/DES partial electron bulk-velocity vector in GSE during this burst [mms1_des_bulkv_part_gse_brst]
      
      
      MMS1 FPI/DES partial electron pressure tensor in DBCS during this burst [mms1_des_prestensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES partial electron pressure tensor in GSE during this burst [mms1_des_prestensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES partial electron temperature tensor in DBCS during this burst [mms1_des_temptensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES partial electron temperature tensor in GSE during this burst [mms1_des_temptensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES partial electron parallel temperature during this burst [mms1_des_temppara_part_brst]
      
      
      MMS1 FPI/DES partial electron perpendicular temperature during this burst [mms1_des_tempperp_part_brst]
      
      
      MMS1 FPI/DES recommended energy index during this burst [mms1_des_part_index_brst]
      Recommended energy index during this burst
      
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MMS1_FPI_BRST_L2_DIS-DIST (spase://NASA/NumericalData/MMS/1/FastPlasmaInvestigation/DIS/Burst/Level2/Distribution/PT0.15S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data are taken at burst (30/150 ms for DES/DIS)
resolution in this mode.  Data are also made available at survey (4.5 s, etc)
resolution; these form a separate product from this.  Per mission design, not
all burst-resolution data are downlinked.  This product contains phase-space
distribution maps of those burst-resolution data selected for downlink.  In
particular, the (highest possible quality at the time of release)
corrected/converted "Burst SkyMap" distributions are reported with time-stamps
and other annotation characterizing the state of the instrument system at the
indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      [CDAWeb List/Download/Create ONLY] MMS1 FPI/DIS burst sky-map instrument distribution [mms1_dis_dist_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 10.6 eV (E1/even) [mms1_dis_dist_brst1_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 12.0 eV (E1/odd) [mms1_dis_dist_brst1_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~11.3 eV (E1 even-odd) [mms1_dis_dist_brst1_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 10.6 eV (E1/even) [mms1_dis_dist_brst1_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 12.0 eV (E1/odd) [mms1_dis_dist_brst1_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 37.2 eV (E6/even) [mms1_dis_dist_brst6_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 42.1 eV (E6/odd) [mms1_dis_dist_brst6_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~39.6 eV (E6 even-odd) [mms1_dis_dist_brst6_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 37.2 eV (E6/even) [mms1_dis_dist_brst6_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 42.1 eV (E6/odd) [mms1_dis_dist_brst6_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 78.8 eV (E9/even) [mms1_dis_dist_brst9_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 89.3 eV (E9/odd) [mms1_dis_dist_brst9_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~83.9 eV (E9 even-odd) [mms1_dis_dist_brst9_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 78.8 eV (E9/even) [mms1_dis_dist_brst9_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 89.3 eV (E9/odd) [mms1_dis_dist_brst9_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 167 eV (E12/even) [mms1_dis_dist_brst12_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 189 eV (E12/odd) [mms1_dis_dist_brst12_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~178 eV (E12 even-odd) [mms1_dis_dist_brst12_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 167 eV (E12/even) [mms1_dis_dist_brst12_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 189 eV (E12/odd) [mms1_dis_dist_brst12_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 275 eV (E14/even) [mms1_dis_dist_brst14_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 312 eV (E14/odd) [mms1_dis_dist_brst14_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~293 eV (E14 even-odd) [mms1_dis_dist_brst14_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 275 eV (E14/even) [mms1_dis_dist_brst14_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 312 eV (E14/odd) [mms1_dis_dist_brst14_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 455 eV (E16/even) [mms1_dis_dist_brst16_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 515 eV (E16/odd) [mms1_dis_dist_brst16_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~484 eV (E16 even-odd) [mms1_dis_dist_brst16_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 455 eV (E16/even) [mms1_dis_dist_brst16_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 515 eV (E16/odd) [mms1_dis_dist_brst16_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 750 eV (E18/even) [mms1_dis_dist_brst18_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 850 eV (E18/odd) [mms1_dis_dist_brst18_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~800 eV (E18 even-odd) [mms1_dis_dist_brst18_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 750 eV (E18/even) [mms1_dis_dist_brst18_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 850 eV (E18/odd) [mms1_dis_dist_brst18_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 1240 eV (E20/even) [mms1_dis_dist_brst20_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 1400 eV (E20/odd) [mms1_dis_dist_brst20_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~1320 eV (E20 even-odd) [mms1_dis_dist_brst20_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1240 eV (E20/even) [mms1_dis_dist_brst20_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1400 eV (E20/odd) [mms1_dis_dist_brst20_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 2620 eV (E23/even) [mms1_dis_dist_brst23_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 2970 eV (E23/odd) [mms1_dis_dist_brst23_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~2800 eV (E23 even-odd) [mms1_dis_dist_brst23_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2620 eV (E23/even) [mms1_dis_dist_brst23_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2970 eV (E23/odd) [mms1_dis_dist_brst23_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 5560 eV (E26/even) [mms1_dis_dist_brst26_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 6300 eV (E26/odd) [mms1_dis_dist_brst26_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~5920 eV (E26 even-odd) [mms1_dis_dist_brst26_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5560 eV (E26/even) [mms1_dis_dist_brst26_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 6300 eV (E26/odd) [mms1_dis_dist_brst26_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 25000 eV (E32/even) [mms1_dis_dist_brst32_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS burst sky-map instrument distribution - 28300 eV (E32/odd) [mms1_dis_dist_brst32_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~26600 eV (E32 even-odd) [mms1_dis_dist_brst32_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 25000 eV (E32/even) [mms1_dis_dist_brst32_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 28300 eV (E32/odd) [mms1_dis_dist_brst32_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [List/Create only in CDAWeb] 1-sigma error: MMS1 FPI/DIS burst sky-map instrument distribution [mms1_dis_disterr_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS vector of data-quality indicators at burst-start time [mms1_dis_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS1 FPI/DIS compression lossless/lossy indicator at survey-start time [mms1_dis_compressionloss_brst]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS1 FPI/DIS step table parity, this burst [mms1_dis_steptable_parity_brst]
      FPI/DIS alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS1 FPI/DIS Del-Phi (obs spin-phase) count at burst-start time [mms1_dis_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS1 FPI/DIS Del-Phi (obs spin-phase) angle at burst-start time [mms1_dis_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS1 FPI/DIS burst average f1 count values [mms1_dis_avgf1counts_brst]
      Average f1-count level as a function of energy
      
      MMS1 FPI/DIS burst sky-map microsecond offsets from Epoch [mms1_dis_steptimeoffsets_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order. Offsets reflect 128 steps over the 150 msec sweep
      period. See FPI docs for details.
      
      ---> MMS1 FPI/DIS sector de-Spin P value, this burst [mms1_dis_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS1 FPI/DIS burst sky-map instrument azimuthal angles [mms1_dis_phi_brst]
      see FPI docs for details
      
      MMS FPI/DIS burst sky-map parity 0/1 energies [mms1_dis_energy_brst]
      Energies (parity 0/1) in the 64-step FPI energy table
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS1_FPI_BRST_L2_DIS-MOMS (spase://NASA/NumericalData/MMS/1/FastPlasmaInvestigation/DIS/Burst/Level2/Moments/PT0.15S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode.  Data are also made available at survey (4.5
s, etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked.  Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available.  This product contains results from
integrating the standard moments of phase-space distributions formed from the
indicated data type (DES/DIS burst, FS or SS).  For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DIS 32-bit vector of data-quality indicators at burst-start time [mms1_dis_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>25%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied
      
      ---> MMS1 FPI/DIS compression lossless/lossy indicator at survey-start time [mms1_dis_compressionloss_brst]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS1 FPI/DIS step table parity, this burst [mms1_dis_steptable_parity_brst]
      FPI/DIS alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS1 FPI/DIS Del-Phi (obs spin-phase) count at burst-start time [mms1_dis_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS1 FPI/DIS Del-Phi (obs spin-phase) angle at burst-start time [mms1_dis_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      ---> MMS1 FPI/DIS sector de-Spin P value, this burst [mms1_dis_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS1 FPI/DIS ion energy spectrum "near" +X_DSC during this burst [mms1_dis_energyspectr_px_brst]
      Counts, summed over DSC velocity-dirs closest to +X_DSC, by energy bin.
      
      ---> MMS1 FPI/DIS ion energy spectrum "near" -X_DSC during this burst [mms1_dis_energyspectr_mx_brst]
      Counts, summed over DSC velocity-dirs closest to -X_DSC, by energy bin.
      
      ---> MMS1 FPI/DIS ion energy spectrum "near" +Y_DSC during this burst [mms1_dis_energyspectr_py_brst]
      Counts, summed over DSC velocity-dirs closest to +Y_DSC, by energy bin.
      
      ---> MMS1 FPI/DIS ion energy spectrum "near" -Y_DSC during this burst [mms1_dis_energyspectr_my_brst]
      Counts, summed over DSC velocity-dirs closest to -Y_DSC, by energy bin.
      
      ---> MMS1 FPI/DIS ion energy spectrum "near" +Z_DSC during this burst [mms1_dis_energyspectr_pz_brst]
      Counts, summed over DSC velocity-dirs closest to +Z_DSC, by energy bin.
      
      ---> MMS1 FPI/DIS ion energy spectrum "near" -Z_DSC during this burst [mms1_dis_energyspectr_mz_brst]
      Counts, summed over DSC velocity-dirs closest to -Z_DSC, by energy bin.
      
      MMS1 FPI/DIS omni-directional ion energy spectrum during this burst [mms1_dis_energyspectr_omni_brst]
      Differential energy flux, averaged (weighted by solid angle) over all look
      directions, by energy bin.
      
      MMS1 FPI/DIS ion background energy during this burst [mms1_dis_spectr_bg_brst]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look) background level.
      
      MMS1 FPI/DIS ion background number density during this burst [mms1_dis_numberdensity_bg_brst]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS1 FPI/DIS ion number density during this burst [mms1_dis_numberdensity_brst]
      
      
      ---> (no error bars displayed) MMS1 FPI/DIS ion number density during this burst [mms1_dis_numberdensity_brst_noerr]
      
      
      ---> MMS1 FPI/DIS ion number density error during this burst [mms1_dis_numberdensity_err_brst]
      
      
      MMS1 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms1_dis_densityextrapolation_low_brst]
      
      
      MMS1 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms1_dis_densityextrapolation_high_brst]
      
      
      MMS1 FPI/DIS ion bulk-velocity DBCS vector during this burst [mms1_dis_bulkv_dbcs_brst]
      
      
      MMS1 FPI/DIS ion bulk-velocity estimated spintone vector in DBCS during this burst [mms1_dis_bulkv_spintone_dbcs_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS1 FPI/DIS ion bulk-velocity DBCS vector during this burst [mms1_dis_bulkv_dbcs_brst_noerr]
      
      
      MMS1 FPI/DIS ion bulk-velocity GSE vector during this burst [mms1_dis_bulkv_gse_brst]
      
      
      MMS1 FPI/DIS ion bulk-velocity estimated spintone vector in GSE during this burst [mms1_dis_bulkv_spintone_gse_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS1 FPI/DIS ion bulk-velocity GSE vector during this burst [mms1_dis_bulkv_gse_brst_noerr]
      
      
      MMS1 FPI/DIS ion bulk-velocity spintone vector in DBCS during this burst [mms1_dis_bulkv_spin_dbcs_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS1 FPI/DIS ion bulk-velocity spintone vector in GSE during this burst [mms1_dis_bulkv_spin_gse_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS1 FPI/DIS ion pressure tensor DBCS matrix during this burst [mms1_dis_prestensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS ion pressure tensor GSE matrix during this burst [mms1_dis_prestensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS ion background pressure during this survey [mms1_dis_pres_bg_brst]
      
      
      MMS1 FPI/DIS ion temperature tensor DBCS matrix during this burst [mms1_dis_temptensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS ion temperature tensor GSE matrix during this burst [mms1_dis_temptensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS ion heat-flux DBCS vector during this burst [mms1_dis_heatq_dbcs_brst]
      
      
      MMS1 FPI/DIS ion heat-flux GSE vector during this burst [mms1_dis_heatq_gse_brst]
      
      
      MMS1 FPI/DIS ion parallel temperature during this BP [mms1_dis_temppara_brst]
      
      
      MMS1 FPI/DIS ion perpendicular temperature during this BP [mms1_dis_tempperp_brst]
      
      
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MMS1_FPI_BRST_L2_DIS-PARTMOMS (spase://NASA/NumericalData/MMS/1/FastPlasmaInvestigation/DIS/Burst/Level2/PartialMoments/PT0.15S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s,
etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked. Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available. This product contains partial moments that
come from performing the standard moment integrals over a limited portion of
velocity space. The resulting quantities are named similarly to their
corresponding standard moments, but are decorated with 'part' to differentiate.
For example, density_part is the density moment integrated from a particular
energy step to infinity. These partial moments are formed from the indicated
data type (DES/DIS burst, FS or SS). For convenience, some additional parameters
are included to augment those most commonly found in a moments product of this
sort, plus time-stamps and other annotation characterizing the state of the
instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DIS vector of data-quality indicators at burst-start time [mms1_dis_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation
      
      MMS1 FPI/DIS partial ion number density during this burst [mms1_dis_numberdensity_part_brst]
      
      
      MMS1 FPI/DIS partial ion bulk-velocity vector in DBCS during this burst [mms1_dis_bulkv_part_dbcs_brst]
      
      
      MMS1 FPI/DIS partial ion bulk-velocity vector in GSE during this burst [mms1_dis_bulkv_part_gse_brst]
      
      
      MMS1 FPI/DIS partial ion pressure tensor in DBCS during this burst [mms1_dis_prestensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS partial ion pressure tensor in GSE during this burst [mms1_dis_prestensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS partial ion temperature tensor in DBCS during this burst [mms1_dis_temptensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS partial ion temperature tensor in GSE during this burst [mms1_dis_temptensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS partial ion parallel temperature during this burst [mms1_dis_temppara_part_brst]
      
      
      MMS1 FPI/DIS partial ion perpendicular temperature during this burst [mms1_dis_tempperp_part_brst]
      
      
      MMS1 FPI/DIS recommended energy index during this burst [mms1_dis_part_index_brst]
      Recommended energy index during this burst
      
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MMS1_FPI_FAST_L2_DES-DIST (spase://NASA/NumericalData/MMS/1/FastPlasmaInvestigation/DES/Fast/Level2/Distribution/PT4.5S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data taken at burst (30/150 ms for DES/DIS)
resolution are aggregated on board and made available at survey (4.5 s)
resolution in this mode.  This product contains phase-space distribution maps of
results from surveying the high-resolution observations during each 4.5 s
period.  In particular, the (highest possible quality at the time of release)
corrected/converted "Fast Survey SkyMap" distributions are reported with
time-stamps and other annotation characterizing the state of the instrument
system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DES fast sky-map instrument distribution - 11.6 eV (E1) using averaged even/odd steps [mms1_des_dist_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 11.6 eV [mms1_des_dist_fast1_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES fast sky-map instrument distribution - 40.4 eV (E6) using averaged even/odd steps [mms1_des_dist_fast6]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 40.4 eV [mms1_des_dist_fast6_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES fast sky-map instrument distribution - 85.1 eV (E9) using averaged even/odd steps [mms1_des_dist_fast9]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 85.1 eV [mms1_des_dist_fast9_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES fast sky-map instrument distribution - 179 eV (E12) using averaged even/odd steps [mms1_des_dist_fast12]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 179 eV [mms1_des_dist_fast12_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES fast sky-map instrument distribution - 295 eV (E14) using averaged even/odd steps [mms1_des_dist_fast14]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 295 eV [mms1_des_dist_fast14_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES fast sky-map instrument distribution - 485 eV (E16) using averaged even/odd steps [mms1_des_dist_fast16]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 485 eV [mms1_des_dist_fast16_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES fast sky-map instrument distribution - 798 eV (E18) using averaged even/odd steps [mms1_des_dist_fast18]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 798 eV [mms1_des_dist_fast18_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES fast sky-map instrument distribution - 1310 eV (E20) using averaged even/odd steps [mms1_des_dist_fast20]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1310 eV [mms1_des_dist_fast20_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES fast sky-map instrument distribution - 2770 eV (E23) using averaged even/odd steps [mms1_des_dist_fast23]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2770 eV [mms1_des_dist_fast23_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES fast sky-map instrument distribution - 5840 eV (E26) using averaged even/odd steps [mms1_des_dist_fast26]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5840 eV [mms1_des_dist_fast26_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES fast sky-map instrument distribution - 26000 eV (E32) using averaged even/odd steps [mms1_des_dist_fast32]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 26000 eV [mms1_des_dist_fast32_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [Only List/Create in CDAWeb] MMS1 FPI/DES fast sky-map instrument distribution 1-sigma error [mms1_des_disterr_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES vector of data-quality indicators at fast survey-start time - 32-bit error flags [mms1_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS1 FPI/DES compression lossless/lossy indicator at survey-start time [mms1_des_compressionloss_fast]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS1 FPI/DES Del-Phi (obs spin-phase) count at fast survey-start time [mms1_des_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS1 FPI/DES Del-Phi (obs spin-phase) angle at fast survey-start time [mms1_des_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS1 FPI/DES fast survey average f1 count values [mms1_des_avgf1counts_fast]
      Average f1-count level as a function of energy
      
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MMS1_FPI_FAST_L2_DES-MOMS (spase://NASA/NumericalData/MMS/1/FastPlasmaInvestigation/DES/Fast/Level2/Moments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution.  Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This moments product
contains results from integrating the standard moments of phase-space
distributions formed from the indicated data type (DES/DIS burst, FS or SS). For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotation characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DES 32-bit vector of data-quality indicators at survey-start time [mms1_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>25%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied
      
      ---> MMS1 FPI/DES compression lossless/lossy indicator at survey-start time [mms1_des_compressionloss_fast]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS1 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms1_des_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS1 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms1_des_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS1 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms1_des_pitchangdist_lowen_fast]
      low energy bin: 0 eV - 200 eV.  pitch-angle bin size: 6 deg.
      
      ---> MMS1 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms1_des_pitchangdist_miden_fast]
      mid energy bin: 200 eV - 2 keV.  pitch-angle bin size: 6 deg.
      
      ---> MMS1 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms1_des_pitchangdist_highen_fast]
      high energy bin: 2 keV - 30 keV.  pitch-angle bin size: 6 deg.
      
      MMS1 FPI/DES electron energy spectrum "near" +X_DSC during this survey [mms1_des_energyspectr_px_fast]
      Counts, summed over DSC velocity-dirs closest to +X_DSC, by energy bin.
      
      ---> MMS1 FPI/DES electron energy spectrum "near" -X_DSC during this survey [mms1_des_energyspectr_mx_fast]
      Counts, summed over DSC velocity-dirs closest to -X_DSC, by energy bin.
      
      ---> MMS1 FPI/DES electron energy spectrum "near" +Y_DSC during this survey [mms1_des_energyspectr_py_fast]
      Counts, summed over DSC velocity-dirs closest to +Y_DSC, by energy bin.
      
      ---> MMS1 FPI/DES electron energy spectrum "near" -Y_DSC during this survey [mms1_des_energyspectr_my_fast]
      Counts, summed over DSC velocity-dirs closest to -Y_DSC, by energy bin.
      
      ---> MMS1 FPI/DES electron energy spectrum "near" +Z_DSC during this survey [mms1_des_energyspectr_pz_fast]
      Counts, summed over DSC velocity-dirs closest to +Z_DSC, by energy bin.
      
      ---> MMS1 FPI/DES electron energy spectrum "near" -Z_DSC during this survey [mms1_des_energyspectr_mz_fast]
      Counts, summed over DSC velocity-dirs closest to -Z_DSC, by energy bin.
      
      MMS1 FPI/DES electron energy parallel spectrum 30 degrees parallel to B during this survey [mms1_des_energyspectr_par_fast]
      Counts, summed within 30 degrees parallel bentPipe magnetic field.
      
      ---> MMS1 FPI/DES electron energy anti-parallel spectrum 30 degrees anti-parallel to B during this survey [mms1_des_energyspectr_anti_fast]
      Counts, summed within 30 degrees antiparallel to bentPipe magnetic field.
      
      ---> MMS1 FPI/DES electron energy perpendicular spectrum 60 degrees perpendicular to B during this survey [mms1_des_energyspectr_perp_fast]
      Counts, summed within 60 degrees perpendicular to bentPipe magnetic field.
      
      MMS1 FPI/DES omni-directional electron energy spectrum during this survey [mms1_des_energyspectr_omni_fast]
      Differential energy flux, averaged (weighted by solid angle) over all look
      directions, by energy bin.
      
      MMS1 FPI/DES electron number density during this survey [mms1_des_numberdensity_fast]
      
      
      ---> (no error bars displayed) MMS1 FPI/DES electron number density during this survey [mms1_des_numberdensity_fast_noerr]
      
      
      ---> MMS1 FPI/DES electron number density error during this survey [mms1_des_numberdensity_err_fast]
      
      
      MMS1 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms1_des_densityextrapolation_low_fast]
      
      
      MMS1 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms1_des_densityextrapolation_high_fast]
      
      
      MMS1 FPI/DES electron bulk-velocity DBCS vector during this survey [mms1_des_bulkv_dbcs_fast]
      
      
      MMS1 FPI/DES electron bulk-velocity estimated spintone vector in DBCS during this survey [mms1_des_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS1 FPI/DES electron bulk-velocity DBCS vector during this survey [mms1_des_bulkv_dbcs_fast_noerr]
      
      
      MMS1 FPI/DES electron bulk-velocity GSE vector during this survey [mms1_des_bulkv_gse_fast]
      
      
      MMS1 FPI/DES electron bulk-velocity estimated spintone vector in GSE during this survey [mms1_des_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS1 FPI/DES electron bulk-velocity GSE vector during this survey [mms1_des_bulkv_gse_fast_noerr]
      
      
      MMS1 FPI/DES electron bulk-velocity spintone vector in DBCS during this survey [mms1_des_bulkv_spin_dbcs_fast]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS1 FPI/DES electron bulk-velocity spintone vector in GSE during this survey [mms1_des_bulkv_spin_gse_fast]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS1 FPI/DES electron pressure tensor DBCS matrix during this survey [mms1_des_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES electron pressure tensor GSE matrix during this survey [mms1_des_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES electron temperature tensor DBCS matrix during this survey [mms1_des_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES electron temperature tensor GSE matrix during this survey [mms1_des_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES electron heat-flux DBCS vector during this survey [mms1_des_heatq_dbcs_fast]
      
      
      MMS1 FPI/DES electron heat-flux GSE vector during this survey [mms1_des_heatq_gse_fast]
      
      
      MMS1 FPI/DES electron parallel temperature during this BP [mms1_des_temppara_fast]
      
      
      MMS1 FPI/DES electron perpendicular temperature during this BP [mms1_des_tempperp_fast]
      
      
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MMS1_FPI_FAST_L2_DES-MOMSAUX
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DES vector of data-quality indicators at survey-start time [mms1_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only)
      
      MMS1 FPI/DES partial electron number density during this survey [mms1_des_numberdensity_part_fast]
      
      
      MMS1 FPI/DES partial electron bulk-velocity vector in DBCS during this survey [mms1_des_bulkv_part_dbcs_fast]
      
      
      MMS1 FPI/DES partial electron bulk-velocity vector in GSE during this survey [mms1_des_bulkv_part_gse_fast]
      
      
      MMS1 FPI/DES partial electron pressure tensor in DBCS during this survey [mms1_des_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES partial electron pressure tensor in GSE during this survey [mms1_des_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES partial electron temperature tensor in DBCS during this survey [mms1_des_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES partial electron temperature tensor in GSE during this survey [mms1_des_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES partial electron parallel temperature during this survey [mms1_des_temppara_part_fast]
      
      
      MMS1 FPI/DES partial electron perpendicular temperature during this survey [mms1_des_tempperp_part_fast]
      
      
      MMS1 FPI/DES recommended energy index for partial moments during this survey [mms1_des_part_index_fast]
      Recommended energy index during this survey
      
      MMS1 FPI/DES compression lossless/lossy indicator at survey-start time [mms1_des_compressionloss_fast]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS1 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms1_des_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS1 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms1_des_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS1 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms1_des_pitchangdist_lowen_fast]
      Low energy bin: energy steps 0-10 (of total steps 0-31). Pitch-angle bin size: 6
      deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS1 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms1_des_pitchangdist_miden_fast]
      Mid energy bin: energy steps 11-20 (of total steps 0-31). Pitch-angle bin size:
      6 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS1 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms1_des_pitchangdist_highen_fast]
      High energy bin: energy steps 21-31 (of total steps 0-31). Pitch-angle bin size:
      6 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS1 FPI/DES electron energy spectrum "near" +X_DBCS during this survey [mms1_des_energyspectr_px_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS1 FPI/DES electron energy spectrum "near" -X_DBCS during this survey [mms1_des_energyspectr_mx_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS1 FPI/DES electron energy spectrum "near" +Y_DBCS during this survey [mms1_des_energyspectr_py_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS1 FPI/DES electron energy spectrum "near" -Y_DBCS during this survey [mms1_des_energyspectr_my_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS1 FPI/DES electron energy spectrum "near" +Z_DBCS during this survey [mms1_des_energyspectr_pz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS1 FPI/DES electron energy spectrum "near" -Z_DBCS during this survey [mms1_des_energyspectr_mz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS1 FPI/DES electron energy parallel to the magnetic field direction during this survey [mms1_des_energyspectr_par_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within 30
      degrees of the magnetic field direction.
      
      MMS1 FPI/DES electron energy anti-parallel to the magnetic field direction during this survey [mms1_des_energyspectr_anti_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      150 degrees of the magnetic field direction.
      
      MMS1 FPI/DES electron energy perpendicular to the magnetic field direction during this survey [mms1_des_energyspectr_perp_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      60-120 degrees of the magnetic field direction.
      
      MMS1 FPI/DES omni-directional electron energy spectrum during this survey [mms1_des_energyspectr_omni_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS1 FPI/DES electron number density during this survey [mms1_des_numberdensity_fast]
      
      
      MMS1 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms1_des_densityextrapolation_low_fast]
      
      
      MMS1 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms1_des_densityextrapolation_high_fast]
      
      
      MMS1 FPI/DES electron bulk-velocity vector in DBCS during this survey [mms1_des_bulkv_dbcs_fast]
      
      
      MMS1 FPI/DES electron bulk-velocity estimated spintone vector in DBCS during this survey [mms1_des_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS1 FPI/DES electron bulk-velocity vector in GSE during this survey [mms1_des_bulkv_gse_fast]
      
      
      MMS1 FPI/DES electron bulk-velocity estimated spintone vector in GSE during this survey [mms1_des_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS1 FPI/DES electron pressure tensor in DBCS during this survey [mms1_des_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES electron pressure tensor in GSE during this survey [mms1_des_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES electron temperature tensor in DBCS during this survey [mms1_des_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES electron temperature tensor in GSE during this survey [mms1_des_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES electron heat-flux vector in DBCS during this survey [mms1_des_heatq_dbcs_fast]
      
      
      MMS1 FPI/DES electron heat-flux vector in GSE during this survey [mms1_des_heatq_gse_fast]
      
      
      MMS1 FPI/DES electron parallel temperature during this BP [mms1_des_temppara_fast]
      
      
      MMS1 FPI/DES electron perpendicular temperature during this BP [mms1_des_tempperp_fast]
      
      
      MMS1 FPI/DES S/C potential mean [mms1_des_scpot_mean_fast]
      Average spacecraft potential during this FP used to shift the measure energies.
      
      MMS1 FPI/DES S/C potential max [mms1_des_scpot_max_fast]
      Maximum spacecraft potential during this FP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      MMS1 FPI/DES Mag data X,Y,Z,Norm DSC components [nT] at survey-start time [mms1_des_fpibentpipe_dsc_fast]
      X, Y, Z are unit vector components.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms1_des_fpib_gse_srvy_fast]
      Averaged survey magnetic field data during this FP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms1_des_fpib_dmpa_srvy_fast]
      Averaged survey magnetic field data during this FP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms1_des_pos_gse_fast]
      
      
      Position in GSM coordinates, 30 second [mms1_des_pos_gsm_fast]
      
      
      MMS1 number density integrands [mms1_des_numberdensity_int_fast]
      Integrand terms used in normalized energy integration for number density
      
      number flux [mms1_des_numberflux_int_dbcs_fast]
      Integrand terms used in normalized energy integration for number flux
      
      MMS1 pressure tensor integrands [mms1_des_prestensor_int_dbcs_fast]
      Integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms1_des_ugrid_int_fast]
      
      
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MMS1_FPI_FAST_L2_DES-PARTMOMS (spase://NASA/NumericalData/MMS/1/FastPlasmaInvestigation/DES/Fast/Level2/PartialMoments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DES vector of data-quality indicators at survey-start time [mms1_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only)
      
      MMS1 FPI/DES partial electron number density during this survey [mms1_des_numberdensity_part_fast]
      
      
      MMS1 FPI/DES partial electron bulk-velocity vector in DBCS during this survey [mms1_des_bulkv_part_dbcs_fast]
      
      
      MMS1 FPI/DES partial electron bulk-velocity vector in GSE during this survey [mms1_des_bulkv_part_gse_fast]
      
      
      MMS1 FPI/DES partial electron pressure tensor in DBCS during this survey [mms1_des_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES partial electron pressure tensor in GSE during this survey [mms1_des_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES partial electron temperature tensor in DBCS during this survey [mms1_des_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES partial electron temperature tensor in GSE during this survey [mms1_des_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES partial electron parallel temperature during this survey [mms1_des_temppara_part_fast]
      
      
      MMS1 FPI/DES partial electron perpendicular temperature during this survey [mms1_des_tempperp_part_fast]
      
      
      MMS1 FPI/DES recommended energy index during this survey [mms1_des_part_index_fast]
      Recommended energy index during this survey
      
Dataset in CDAWeb
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MMS1_FPI_FAST_L2_DIS-DIST (spase://NASA/NumericalData/MMS/1/FastPlasmaInvestigation/DIS/Fast/Level2/Distribution/PT4.5S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data taken at burst (30/150 ms for DES/DIS)
resolution are aggregated on board and made available at survey (4.5 s)
resolution in this mode.  This product contains phase-space distribution maps of
results from surveying the high-resolution observations during each 4.5 s
period.  In particular, the (highest possible quality at the time of release)
corrected/converted "Fast Survey SkyMap" distributions are reported with
time-stamps and other annotation characterizing the state of the instrument
system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DIS fast sky-map instrument distribution - 11.3 eV (E1) using averaged even/odd steps [mms1_dis_dist_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 11.3 eV [mms1_dis_dist_fast1_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS fast sky-map instrument distribution - 39.6 eV (E6) using averaged even/odd steps [mms1_dis_dist_fast6]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 39.6 eV [mms1_dis_dist_fast6_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS fast sky-map instrument distribution - 83.9 eV (E9 using averaged even/odd steps) [mms1_dis_dist_fast9]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 83.9 eV [mms1_dis_dist_fast9_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS fast sky-map instrument distribution - 178 eV (E12) using averaged even/odd steps [mms1_dis_dist_fast12]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 178 eV [mms1_dis_dist_fast12_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS fast sky-map instrument distribution - 293 eV (E14) using averaged even/odd steps [mms1_dis_dist_fast14]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 293 eV [mms1_dis_dist_fast14_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS fast sky-map instrument distribution - 484 eV (E16) using averaged even/odd steps [mms1_dis_dist_fast16]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 484 eV [mms1_dis_dist_fast16_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS fast sky-map instrument distribution - 799 eV (E18) using averaged even/odd steps [mms1_dis_dist_fast18]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 799 eV [mms1_dis_dist_fast18_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS fast sky-map instrument distribution - 1320 eV (E20) using averaged even/odd steps [mms1_dis_dist_fast20]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1320 eV [mms1_dis_dist_fast20_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS fast sky-map instrument distribution - 2800 eV (E23) using averaged even/odd steps [mms1_dis_dist_fast23]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2800 eV [mms1_dis_dist_fast23_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS fast sky-map instrument distribution - 5920 eV (E26) using averaged even/odd steps [mms1_dis_dist_fast26]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5920 eV [mms1_dis_dist_fast26_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS fast sky-map instrument distribution - 26600 eV (E32) using averaged even/odd steps [mms1_dis_dist_fast32]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 26600 eV [mms1_dis_dist_fast32_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [Only List/Create in CDAWeb] MMS1 FPI/DIS fast sky-map instrument distribution 1-sigma error [mms1_dis_disterr_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS vector of data-quality indicators at fast survey-start time - 32-bit error flags [mms1_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS1 FPI/DIS compression lossless/lossy indicator at survey-start time [mms1_dis_compressionloss_fast]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS1 FPI/DIS Del-Phi (obs spin-phase) count at fast survey-start time [mms1_dis_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS1 FPI/DIS Del-Phi (obs spin-phase) angle at fast survey-start time [mms1_dis_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS1 FPI/DIS fast survey average f1 count values [mms1_dis_avgf1counts_fast]
      Average f1-count level as a function of energy
      
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MMS1_FPI_FAST_L2_DIS-MOMS (spase://NASA/NumericalData/MMS/1/FastPlasmaInvestigation/DIS/Fast/Level2/Moments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution.  Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This moments product
contains results from integrating the standard moments of phase-space
distributions formed from the indicated data type (DES/DIS burst, FS or SS). For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotation characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DIS vector of data-quality indicators at survey-start time [mms1_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation, Bit-14 =
      high MMS3 spintone due to DIS008 anomaly
      
      ---> MMS1 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms1_dis_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      ---> MMS1 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms1_dis_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS1 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms1_dis_energyspectr_px_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      ---> MMS1 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms1_dis_energyspectr_mx_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      ---> MMS1 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms1_dis_energyspectr_py_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      ---> MMS1 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms1_dis_energyspectr_my_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      ---> MMS1 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms1_dis_energyspectr_pz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      ---> MMS1 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms1_dis_energyspectr_mz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS1 FPI/DIS omni-directional ion energy spectrum during this survey [mms1_dis_energyspectr_omni_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS1 FPI/DIS ion background energy during this survey [mms1_dis_spectr_bg_fast]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS1 FPI/DIS ion background number density during this survey [mms1_dis_numberdensity_bg_fast]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS1 FPI/DIS ion number density during this survey [mms1_dis_numberdensity_fast]
      
      
      ---> (no error bars displayed) MMS1 FPI/DIS ion number density during this survey [mms1_dis_numberdensity_fast_noerr]
      
      
      MMS1 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms1_dis_densityextrapolation_low_fast]
      
      
      MMS1 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms1_dis_densityextrapolation_high_fast]
      
      
      MMS1 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms1_dis_bulkv_dbcs_fast]
      
      
      ---> (no error bars displayed) MMS1 FPI/DIS ion bulk-velocity DBCS vector during this survey [mms1_dis_bulkv_dbcs_fast_noerr]
      
      
      MMS1 FPI/DIS ion bulk-velocity estimated spintone vector in DBCS during this survey [mms1_dis_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS1 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms1_dis_bulkv_gse_fast]
      
      
      MMS1 FPI/DIS ion bulk-velocity estimated spintone vector in GSE during this survey [mms1_dis_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS1 FPI/DIS ion bulk-velocity GSE vector during this survey [mms1_dis_bulkv_gse_fast_noerr]
      
      
      MMS1 FPI/DIS ion pressure tensor in DBCS during this survey [mms1_dis_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS ion pressure tensor in GSE during this survey [mms1_dis_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS ion background pressure during this survey [mms1_dis_pres_bg_fast]
      
      
      MMS1 FPI/DIS ion temperature tensor in DBCS during this survey [mms1_dis_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS ion temperature tensor in GSE during this survey [mms1_dis_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS ion heat-flux vector in DBCS during this survey [mms1_dis_heatq_dbcs_fast]
      
      
      MMS1 FPI/DIS ion heat-flux vector in GSE during this survey [mms1_dis_heatq_gse_fast]
      
      
      MMS1 FPI/DIS ion parallel temperature during this BP [mms1_dis_temppara_fast]
      
      
      MMS1 FPI/DIS ion perpendicular temperature during this BP [mms1_dis_tempperp_fast]
      
      
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MMS1_FPI_FAST_L2_DIS-MOMSAUX
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DIS vector of data-quality indicators at survey-start time [mms1_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation
      
      MMS1 FPI/DIS partial ion number density during this survey [mms1_dis_numberdensity_part_fast]
      
      
      MMS1 FPI/DIS partial ion bulk-velocity vector in DBCS during this survey [mms1_dis_bulkv_part_dbcs_fast]
      
      
      MMS1 FPI/DIS partial ion bulk-velocity vector in GSE during this survey [mms1_dis_bulkv_part_gse_fast]
      
      
      MMS1 FPI/DIS partial ion pressure tensor in DBCS during this survey [mms1_dis_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS partial ion pressure tensor in GSE during this survey [mms1_dis_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS partial ion temperature tensor in DBCS during this survey [mms1_dis_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS partial ion temperature tensor in GSE during this survey [mms1_dis_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS partial ion parallel temperature during this survey [mms1_dis_temppara_part_fast]
      
      
      MMS1 FPI/DIS partial ion perpendicular temperature during this survey [mms1_dis_tempperp_part_fast]
      
      
      MMS1 FPI/DIS recommended energy index for partial moments during this survey [mms1_dis_part_index_fast]
      Recommended energy index during this survey
      
      MMS1 FPI/DIS compression lossless/lossy indicator at survey-start time [mms1_dis_compressionloss_fast]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS1 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms1_dis_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS1 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms1_dis_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS1 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms1_dis_energyspectr_px_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms1_dis_energyspectr_mx_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms1_dis_energyspectr_py_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms1_dis_energyspectr_my_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms1_dis_energyspectr_pz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms1_dis_energyspectr_mz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS1 FPI/DIS omni-directional ion energy spectrum during this survey [mms1_dis_energyspectr_omni_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS1 FPI/DIS ion background energy during this survey [mms1_dis_spectr_bg_fast]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS1 FPI/DIS ion background number density during this survey [mms1_dis_numberdensity_bg_fast]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS1 FPI/DIS ion number density during this survey [mms1_dis_numberdensity_fast]
      
      
      MMS1 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms1_dis_densityextrapolation_low_fast]
      
      
      MMS1 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms1_dis_densityextrapolation_high_fast]
      
      
      MMS1 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms1_dis_bulkv_dbcs_fast]
      
      
      MMS1 FPI/DIS ion bulk-velocity estimated spintone vector in DBCS during this survey [mms1_dis_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS1 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms1_dis_bulkv_gse_fast]
      
      
      MMS1 FPI/DIS ion bulk-velocity estimated spintone vector in GSE during this survey [mms1_dis_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS1 FPI/DIS ion pressure tensor in DBCS during this survey [mms1_dis_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS ion pressure tensor in GSE during this survey [mms1_dis_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS ion background pressure during this survey [mms1_dis_pres_bg_fast]
      
      
      MMS1 FPI/DIS ion temperature tensor in DBCS during this survey [mms1_dis_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS ion temperature tensor in GSE during this survey [mms1_dis_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS ion heat-flux vector in DBCS during this survey [mms1_dis_heatq_dbcs_fast]
      
      
      MMS1 FPI/DIS ion heat-flux vector in GSE during this survey [mms1_dis_heatq_gse_fast]
      
      
      MMS1 FPI/DIS ion parallel temperature during this BP [mms1_dis_temppara_fast]
      
      
      MMS1 FPI/DIS ion perpendicular temperature during this BP [mms1_dis_tempperp_fast]
      
      
      MMS1 FPI/DIS S/C potential mean [mms1_dis_scpot_mean_fast]
      Average spacecraft potential during this FP used to shift the measure energies.
      
      MMS1 FPI/DIS S/C potential max [mms1_dis_scpot_max_fast]
      Maximum spacecraft potential during this FP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      MMS1 FPI/DIS Mag data X,Y,Z,Norm DSC components [nT] at survey-start time [mms1_dis_fpibentpipe_dsc_fast]
      X, Y, Z are unit vector components.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms1_dis_fpib_gse_srvy_fast]
      Averaged survey magnetic field data during this FP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms1_dis_fpib_dmpa_srvy_fast]
      Averaged survey magnetic field data during this FP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms1_dis_pos_gse_fast]
      
      
      Position in GSM coordinates, 30 second [mms1_dis_pos_gsm_fast]
      
      
      MMS1 number density integrands [mms1_dis_numberdensity_int_fast]
      integrand terms used in normalized energy integration for number density
      
      number flux [mms1_dis_numberflux_int_dbcs_fast]
      integrand terms used in normalized energy integration for number flux
      
      MMS1 pressure tensor integrands [mms1_dis_prestensor_int_dbcs_fast]
      integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms1_dis_ugrid_int_fast]
      
      
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MMS1_FPI_FAST_L2_DIS-PARTMOMS (spase://NASA/NumericalData/MMS/1/FastPlasmaInvestigation/DIS/Fast/Level2/PartialMoments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DIS vector of data-quality indicators at survey-start time [mms1_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation
      
      MMS1 FPI/DIS partial ion number density during this survey [mms1_dis_numberdensity_part_fast]
      
      
      MMS1 FPI/DIS partial ion bulk-velocity vector in DBCS during this survey [mms1_dis_bulkv_part_dbcs_fast]
      
      
      MMS1 FPI/DIS partial ion bulk-velocity vector in GSE during this survey [mms1_dis_bulkv_part_gse_fast]
      
      
      MMS1 FPI/DIS partial ion pressure tensor in DBCS during this survey [mms1_dis_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS partial ion pressure tensor in GSE during this survey [mms1_dis_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS partial ion temperature tensor in DBCS during this survey [mms1_dis_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS partial ion temperature tensor in GSE during this survey [mms1_dis_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS partial ion parallel temperature during this survey [mms1_dis_temppara_part_fast]
      
      
      MMS1 FPI/DIS partial ion perpendicular temperature during this survey [mms1_dis_tempperp_part_fast]
      
      
      MMS1 FPI/DIS recommended energy index during this survey [mms1_dis_part_index_fast]
      Recommended energy index during this survey
      
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MMS1_FPI_SLOW_L2_DES-DIST
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode.  This product contains phase-space distribution maps of those
survey-resolution data from Slow Mode.  In particular, the (highest possible
quality at the time of release) corrected/converted "Slow Survey SkyMap"
distributions are reported with time-stamps and other annotation characterizing
the state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DES vector of data-quality indicators at survey-start time [mms1_des_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = compression pipeline error
      
      MMS1 FPI/DES compression lossless/lossy indicator at survey-start time [mms1_des_compressionloss_slow]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS1 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms1_des_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS1 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms1_des_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS1 FPI/DES Slow Survey sky-map instrument distribution [mms1_des_dist_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES Slow Survey sky-map instrument distribution 1-sigma error [mms1_des_disterr_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DES slow survey average f1 count values [mms1_des_avgf1counts_slow]
      Average f1-count level as a function of energy
      
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MMS1_FPI_SLOW_L2_DES-MOMS
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DES vector of data-quality indicators at survey-start time [mms1_des_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only)
      
      MMS1 FPI/DES compression lossless/lossy indicator at survey-start time [mms1_des_compressionloss_slow]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS1 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms1_des_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS1 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms1_des_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS1 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms1_des_pitchangdist_lowen_slow]
      Low energy bin: energy steps 0-10 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS1 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms1_des_pitchangdist_miden_slow]
      Mid energy bin: energy steps 11-20 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS1 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms1_des_pitchangdist_highen_slow]
      High energy bin: energy steps 21-31 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS1 FPI/DES electron energy spectrum "near" +X_DBCS during this survey [mms1_des_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS1 FPI/DES electron energy spectrum "near" -X_DBCS during this survey [mms1_des_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS1 FPI/DES electron energy spectrum "near" +Y_DBCS during this survey [mms1_des_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS1 FPI/DES electron energy spectrum "near" -Y_DBCS during this survey [mms1_des_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS1 FPI/DES electron energy spectrum "near" +Z_DBCS during this survey [mms1_des_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS1 FPI/DES electron energy spectrum "near" -Z_DBCS during this survey [mms1_des_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS1 FPI/DES electron energy parallel to the magnetic field direction during this survey [mms1_des_energyspectr_par_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within 30
      degrees of the magnetic field direction.
      
      MMS1 FPI/DES electron energy anti-parallel to the magnetic field direction during this survey [mms1_des_energyspectr_anti_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      150 degrees of the magnetic field direction.
      
      MMS1 FPI/DES electron energy perpendicular to the magnetic field direction during this survey [mms1_des_energyspectr_perp_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      60-120 degrees of the magnetic field direction.
      
      MMS1 FPI/DES omni-directional electron energy spectrum during this survey [mms1_des_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS1 FPI/DES electron number density during this survey [mms1_des_numberdensity_slow]
      
      
      MMS1 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms1_des_densityextrapolation_low_slow]
      
      
      MMS1 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms1_des_densityextrapolation_high_slow]
      
      
      MMS1 FPI/DES electron bulk-velocity vector in DBCS during this survey [mms1_des_bulkv_dbcs_slow]
      
      
      MMS1 FPI/DES electron bulk-velocity vector in GSE during this survey [mms1_des_bulkv_gse_slow]
      
      
      MMS1 FPI/DES electron pressure tensor in DBCS during this survey [mms1_des_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES electron pressure tensor in GSE during this survey [mms1_des_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES electron temperature tensor in DBCS during this survey [mms1_des_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES electron temperature tensor in GSE during this survey [mms1_des_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES electron heat-flux vector in DBCS during this survey [mms1_des_heatq_dbcs_slow]
      
      
      MMS1 FPI/DES electron heat-flux vector in GSE during this survey [mms1_des_heatq_gse_slow]
      
      
      MMS1 FPI/DES electron parallel temperature during this BP [mms1_des_temppara_slow]
      
      
      MMS1 FPI/DES electron perpendicular temperature during this BP [mms1_des_tempperp_slow]
      
      
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MMS1_FPI_SLOW_L2_DES-MOMSAUX
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DES vector of data-quality indicators at survey-start time [mms1_des_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only)
      
      MMS1 FPI/DES partial electron number density during this survey [mms1_des_numberdensity_part_slow]
      
      
      MMS1 FPI/DES partial electron bulk-velocity vector in DBCS during this survey [mms1_des_bulkv_part_dbcs_slow]
      
      
      MMS1 FPI/DES partial electron bulk-velocity vector in GSE during this survey [mms1_des_bulkv_part_gse_slow]
      
      
      MMS1 FPI/DES partial electron pressure tensor in DBCS during this survey [mms1_des_prestensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES partial electron pressure tensor in GSE during this survey [mms1_des_prestensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES partial electron temperature tensor in DBCS during this survey [mms1_des_temptensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES partial electron temperature tensor in GSE during this survey [mms1_des_temptensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES partial electron parallel temperature during this survey [mms1_des_temppara_part_slow]
      
      
      MMS1 FPI/DES partial electron perpendicular temperature during this survey [mms1_des_tempperp_part_slow]
      
      
      MMS1 FPI/DES recommended energy index for partial moments during this survey [mms1_des_part_index_slow]
      Recommended energy index during this survey
      
      MMS1 FPI/DES compression lossless/lossy indicator at survey-start time [mms1_des_compressionloss_slow]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS1 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms1_des_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS1 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms1_des_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS1 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms1_des_pitchangdist_lowen_slow]
      Low energy bin: energy steps 0-10 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS1 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms1_des_pitchangdist_miden_slow]
      Mid energy bin: energy steps 11-20 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS1 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms1_des_pitchangdist_highen_slow]
      High energy bin: energy steps 21-31 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS1 FPI/DES electron energy spectrum "near" +X_DBCS during this survey [mms1_des_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS1 FPI/DES electron energy spectrum "near" -X_DBCS during this survey [mms1_des_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS1 FPI/DES electron energy spectrum "near" +Y_DBCS during this survey [mms1_des_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS1 FPI/DES electron energy spectrum "near" -Y_DBCS during this survey [mms1_des_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS1 FPI/DES electron energy spectrum "near" +Z_DBCS during this survey [mms1_des_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS1 FPI/DES electron energy spectrum "near" -Z_DBCS during this survey [mms1_des_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS1 FPI/DES electron energy parallel to the magnetic field direction during this survey [mms1_des_energyspectr_par_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within 30
      degrees of the magnetic field direction.
      
      MMS1 FPI/DES electron energy anti-parallel to the magnetic field direction during this survey [mms1_des_energyspectr_anti_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      150 degrees of the magnetic field direction.
      
      MMS1 FPI/DES electron energy perpendicular to the magnetic field direction during this survey [mms1_des_energyspectr_perp_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      60-120 degrees of the magnetic field direction.
      
      MMS1 FPI/DES omni-directional electron energy spectrum during this survey [mms1_des_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS1 FPI/DES electron number density during this survey [mms1_des_numberdensity_slow]
      
      
      MMS1 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms1_des_densityextrapolation_low_slow]
      
      
      MMS1 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms1_des_densityextrapolation_high_slow]
      
      
      MMS1 FPI/DES electron bulk-velocity vector in DBCS during this survey [mms1_des_bulkv_dbcs_slow]
      
      
      MMS1 FPI/DES electron bulk-velocity vector in GSE during this survey [mms1_des_bulkv_gse_slow]
      
      
      MMS1 FPI/DES electron pressure tensor in DBCS during this survey [mms1_des_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES electron pressure tensor in GSE during this survey [mms1_des_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DES electron temperature tensor in DBCS during this survey [mms1_des_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES electron temperature tensor in GSE during this survey [mms1_des_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DES electron heat-flux vector in DBCS during this survey [mms1_des_heatq_dbcs_slow]
      
      
      MMS1 FPI/DES electron heat-flux vector in GSE during this survey [mms1_des_heatq_gse_slow]
      
      
      MMS1 FPI/DES electron parallel temperature during this BP [mms1_des_temppara_slow]
      
      
      MMS1 FPI/DES electron perpendicular temperature during this BP [mms1_des_tempperp_slow]
      
      
      MMS1 FPI/DES S/C potential mean [mms1_des_scpot_mean_slow]
      Average spacecraft potential during this SP used to shift the measure energies.
      
      MMS1 FPI/DES S/C potential max [mms1_des_scpot_max_slow]
      Maximum spacecraft potential during this SP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms1_des_fpib_gse_srvy_slow]
      Averaged survey magnetic field data during this SP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms1_des_fpib_dmpa_srvy_slow]
      Averaged survey magnetic field data during this SP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms1_des_pos_gse_slow]
      
      
      Position in GSM coordinates, 30 second [mms1_des_pos_gsm_slow]
      
      
      MMS1 number density integrands [mms1_des_numberdensity_int_slow]
      integrand terms used in normalized energy integration for number density
      
      number flux [mms1_des_numberflux_int_dbcs_slow]
      integrand terms used in normalized energy integration for number flux
      
      MMS1 pressure tensor integrands [mms1_des_prestensor_int_dbcs_slow]
      integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms1_des_ugrid_int_slow]
      
      
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MMS1_FPI_SLOW_L2_DIS-DIST
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode.  This product contains phase-space distribution maps of those
survey-resolution data from Slow Mode.  In particular, the (highest possible
quality at the time of release) corrected/converted "Slow Survey SkyMap"
distributions are reported with time-stamps and other annotation characterizing
the state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DIS vector of data-quality indicators at survey-start time [mms1_dis_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = compression pipeline error
      
      MMS1 FPI/DIS compression lossless/lossy indicator at survey-start time [mms1_dis_compressionloss_slow]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS1 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms1_dis_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS1 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms1_dis_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS1 FPI/DIS Slow Survey sky-map instrument distribution [mms1_dis_dist_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS Slow Survey sky-map instrument distribution 1-sigma error [mms1_dis_disterr_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS1 FPI/DIS slow survey average f1 count values [mms1_dis_avgf1counts_slow]
      Average f1-count level as a function of energy
      
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MMS1_FPI_SLOW_L2_DIS-MOMS
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DIS vector of data-quality indicators at survey-start time [mms1_dis_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only), Bit-13 =
      significant (>=20%) penetrating radiation, Bit-14 = high MMS3 spintone due to
      DIS008 anomaly
      
      MMS1 FPI/DIS compression lossless/lossy indicator at survey-start time [mms1_dis_compressionloss_slow]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS1 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms1_dis_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS1 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms1_dis_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS1 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms1_dis_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms1_dis_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms1_dis_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms1_dis_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms1_dis_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms1_dis_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS1 FPI/DIS omni-directional ion energy spectrum during this survey [mms1_dis_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS1 FPI/DIS ion background energy during this survey [mms1_dis_spectr_bg_slow]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS1 FPI/DIS ion background number density during this survey [mms1_dis_numberdensity_bg_slow]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS1 FPI/DIS ion number density during this survey [mms1_dis_numberdensity_slow]
      
      
      MMS1 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms1_dis_densityextrapolation_low_slow]
      
      
      MMS1 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms1_dis_densityextrapolation_high_slow]
      
      
      MMS1 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms1_dis_bulkv_dbcs_slow]
      
      
      MMS1 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms1_dis_bulkv_gse_slow]
      
      
      MMS1 FPI/DIS ion pressure tensor in DBCS during this survey [mms1_dis_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS ion pressure tensor in GSE during this survey [mms1_dis_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS ion background pressure during this survey [mms1_dis_pres_bg_slow]
      
      
      MMS1 FPI/DIS ion temperature tensor in DBCS during this survey [mms1_dis_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS ion temperature tensor in GSE during this survey [mms1_dis_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS ion heat-flux vector in DBCS during this survey [mms1_dis_heatq_dbcs_slow]
      
      
      MMS1 FPI/DIS ion heat-flux vector in GSE during this survey [mms1_dis_heatq_gse_slow]
      
      
      MMS1 FPI/DIS ion parallel temperature during this BP [mms1_dis_temppara_slow]
      
      
      MMS1 FPI/DIS ion perpendicular temperature during this BP [mms1_dis_tempperp_slow]
      
      
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MMS1_FPI_SLOW_L2_DIS-MOMSAUX
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS1 FPI/DIS vector of data-quality indicators at survey-start time [mms1_dis_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only), Bit-13 =
      significant (>=20%) penetrating radiation, Bit-14 = high MMS3 spintone due to
      DIS008 anomaly
      
      MMS1 FPI/DIS partial ion number density during this survey [mms1_dis_numberdensity_part_slow]
      
      
      MMS1 FPI/DIS partial ion bulk-velocity vector in DBCS during this survey [mms1_dis_bulkv_part_dbcs_slow]
      
      
      MMS1 FPI/DIS partial ion bulk-velocity vector in GSE during this survey [mms1_dis_bulkv_part_gse_slow]
      
      
      MMS1 FPI/DIS partial ion pressure tensor in DBCS during this survey [mms1_dis_prestensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS partial ion pressure tensor in GSE during this survey [mms1_dis_prestensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS partial ion temperature tensor in DBCS during this survey [mms1_dis_temptensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS partial ion temperature tensor in GSE during this survey [mms1_dis_temptensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS partial ion parallel temperature during this survey [mms1_dis_temppara_part_slow]
      
      
      MMS1 FPI/DIS partial ion perpendicular temperature during this survey [mms1_dis_tempperp_part_slow]
      
      
      MMS1 FPI/DIS recommended energy index for partial moments during this survey [mms1_dis_part_index_slow]
      Recommended energy index during this survey
      
      MMS1 FPI/DIS compression lossless/lossy indicator at survey-start time [mms1_dis_compressionloss_slow]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS1 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms1_dis_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS1 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms1_dis_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS1 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms1_dis_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms1_dis_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms1_dis_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms1_dis_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms1_dis_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS1 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms1_dis_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS1 FPI/DIS omni-directional ion energy spectrum during this survey [mms1_dis_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS1 FPI/DIS ion background energy during this survey [mms1_dis_spectr_bg_slow]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS1 FPI/DIS ion background number density during this survey [mms1_dis_numberdensity_bg_slow]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS1 FPI/DIS ion number density during this survey [mms1_dis_numberdensity_slow]
      
      
      MMS1 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms1_dis_densityextrapolation_low_slow]
      
      
      MMS1 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms1_dis_densityextrapolation_high_slow]
      
      
      MMS1 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms1_dis_bulkv_dbcs_slow]
      
      
      MMS1 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms1_dis_bulkv_gse_slow]
      
      
      MMS1 FPI/DIS ion pressure tensor in DBCS during this survey [mms1_dis_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS ion pressure tensor in GSE during this survey [mms1_dis_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS1 FPI/DIS ion background pressure during this survey [mms1_dis_pres_bg_slow]
      
      
      MMS1 FPI/DIS ion temperature tensor in DBCS during this survey [mms1_dis_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS ion temperature tensor in GSE during this survey [mms1_dis_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS1 FPI/DIS ion heat-flux vector in DBCS during this survey [mms1_dis_heatq_dbcs_slow]
      
      
      MMS1 FPI/DIS ion heat-flux vector in GSE during this survey [mms1_dis_heatq_gse_slow]
      
      
      MMS1 FPI/DIS ion parallel temperature during this BP [mms1_dis_temppara_slow]
      
      
      MMS1 FPI/DIS ion perpendicular temperature during this BP [mms1_dis_tempperp_slow]
      
      
      MMS1 FPI/DIS S/C potential mean [mms1_dis_scpot_mean_slow]
      Average spacecraft potential during this SP used to shift the measure energies.
      
      MMS1 FPI/DIS S/C potential max [mms1_dis_scpot_max_slow]
      Maximum spacecraft potential during this SP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms1_dis_fpib_gse_srvy_slow]
      Averaged survey magnetic field data during this SP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms1_dis_fpib_dmpa_srvy_slow]
      Averaged survey magnetic field data during this SP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms1_dis_pos_gse_slow]
      
      
      Position in GSM coordinates, 30 second [mms1_dis_pos_gsm_slow]
      
      
      MMS1 number density integrands [mms1_dis_numberdensity_int_slow]
      integrand terms used in normalized energy integration for number density
      
      number flux [mms1_dis_numberflux_int_dbcs_slow]
      integrand terms used in normalized energy integration for number flux
      
      MMS1 pressure tensor integrands [mms1_dis_prestensor_int_dbcs_slow]
      integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms1_dis_ugrid_int_slow]
      
      
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MMS1_HPCA_BRST_L2_ION (spase://NASA/NumericalData/MMS/1/HotPlasmaCompositionAnalyzer/Burst/Level2/Ion/PT0.625S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Start Azimuth [mms1_hpca_start_azimuth]
      
      
      Science Mode Value as defined in the HPCA Science Algorithm Document [mms1_hpca_science_mode]
      
      
      H+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms1_hpca_hplus_data_quality]
      
      
      Hydrogen+ Flux for all Elevation Anodes across all energies [mms1_hpca_hplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_hplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_hplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_hplus_flux_byAnode_atE]
      
      
      Hydrogen+ Phase Space Density for all Elevation Anodes across all energies [mms1_hpca_hplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_hplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anodes [mms1_hpca_hplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_hplus_phase_space_density_byAnode_atE]
      
      
      He+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms1_hpca_heplus_data_quality]
      
      
      Helium+ Flux for all Elevation Anodes across all energies [mms1_hpca_heplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_heplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_heplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_heplus_flux_byAnode_atE]
      
      
      Helium+ Phase Space Density for all Elevation Anodes across all energies [mms1_hpca_heplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_heplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_heplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_heplus_phase_space_density_byAnode_atE]
      
      
      He++ per sweep status (0=bad): see Data_Quality_Key global attribute [mms1_hpca_heplusplus_data_quality]
      
      
      Helium++ Flux for all Elevation Anodes across all energies [mms1_hpca_heplusplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_heplusplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_heplusplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_heplusplus_flux_byAnode_atE]
      
      
      Helium++ Phase Space Density for all Elevation Anodes across all energies [mms1_hpca_heplusplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_heplusplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_heplusplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_heplusplus_phase_space_density_byAnode_atE]
      
      
      O+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms1_hpca_oplus_data_quality]
      
      
      Oxygen+ Flux for all Elevation Anodes across all energies [mms1_hpca_oplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_oplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_oplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_oplus_flux_byAnode_atE]
      
      
      Oxygen+ Phase Space Density for all Elevation Anodes across all energies [mms1_hpca_oplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_oplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_oplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_oplus_phase_space_density_byAnode_atE]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s), Despun MPA-aligned cartesian coordinates [mms1_hpca_B_GSE_sweep_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s), Geocentric Solar Magnetospheric (GSM) cartesian coordinates [mms1_hpca_B_GSM_sweep_avg]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms1_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms1_hpca_TOF_VMON_MIN_converted]
      
      
      Decimation Factor Index from mode config file [mms1_hpca_decimation_factor_index]
      
      
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MMS1_HPCA_BRST_L2_MOMENTS (spase://NASA/NumericalData/MMS/1/HotPlasmaCompositionAnalyzer/Burst/Level2/Moments/PT10S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Number Density Hydrogen+ for each HPCA half-spin [mms1_hpca_hplus_number_density]
      
      
      ---> Ion Bulk Velocity Hydrogen+ for each HPCA half-spin (x, y, z) [mms1_hpca_hplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Hydrogen+ for each HPCA half-spin [mms1_hpca_hplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_hplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_hplus_temperature_tensor]
      
      
      Number Density Helium+ for each HPCA half-spin [mms1_hpca_heplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium+ for each HPCA half-spin (x, y, z) [mms1_hpca_heplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium+ for each HPCA half-spin [mms1_hpca_heplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_heplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_heplus_temperature_tensor]
      
      
      Number Density Helium++ for each HPCA half-spin [mms1_hpca_heplusplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium++ for each HPCA half-spin (x, y, z) [mms1_hpca_heplusplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium++ for each HPCA half-spin [mms1_hpca_heplusplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_heplusplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_heplusplus_temperature_tensor]
      
      
      Number Density Oxygen+ for each HPCA half-spin [mms1_hpca_oplus_number_density]
      
      
      ---> Ion Bulk Velocity Oxygen+ for each HPCA half-spin (x, y, z) [mms1_hpca_oplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Oxygen+ for each HPCA half-spin [mms1_hpca_oplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_oplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_oplus_temperature_tensor]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms1_hpca_B_GSE_spin_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms1_hpca_B_GSM_spin_avg]
      
      
      Bulk Velocity in GSM for H+ for each HPCA half-spin (x, y, z) [mms1_hpca_hplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp H+ for each HPCA half-spin [mms1_hpca_hplus_tperp]
      
      
      ---> Tparallel H+ for each HPCA half-spin [mms1_hpca_hplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_hplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_hplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_hplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_hplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He+ for each HPCA half-spin (x, y, z) [mms1_hpca_heplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He+ for each HPCA half-spin [mms1_hpca_heplus_tperp]
      
      
      ---> Tparallel He+ for each HPCA half-spin [mms1_hpca_heplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He++ for each HPCA half-spin (x, y, z) [mms1_hpca_heplusplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He++ for each HPCA half-spin [mms1_hpca_heplusplus_tperp]
      
      
      ---> Tparallel He++ for each HPCA half-spin [mms1_hpca_heplusplus_tparallel]
      
      
      Vperp vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplusplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplusplus_vparallel]
      
      
      Vperp vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplusplus_vperp_GSM]
      
      
      Vparallel vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplusplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for O+ for each HPCA half-spin (x, y, z) [mms1_hpca_oplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp O+ for each HPCA half-spin [mms1_hpca_oplus_tperp]
      
      
      ---> Tparallel O+ for each HPCA half-spin [mms1_hpca_oplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_oplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_oplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_oplus_vperp_GSM]
      
      
      --->Vparallel vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_oplus_vparallel_GSM]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms1_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms1_hpca_TOF_VMON_MIN_converted]
      
      
Dataset in CDAWeb
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MMS1_HPCA_SRVY_L2_ION (spase://NASA/NumericalData/MMS/1/HotPlasmaCompositionAnalyzer/Survey/Level2/Ion/PT0.625S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Start Azimuth [mms1_hpca_start_azimuth]
      
      
      Science Mode Value as defined in the HPCA Science Algorithm Document [mms1_hpca_science_mode]
      
      
      H+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms1_hpca_hplus_data_quality]
      
      
      Hydrogen+ Flux for all Elevation Anodes across all energies [mms1_hpca_hplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_hplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_hplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_hplus_flux_byAnode_atE]
      
      
      Hydrogen+ Phase Space Density for all Elevation Anodes across all energies [mms1_hpca_hplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_hplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anodes [mms1_hpca_hplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_hplus_phase_space_density_byAnode_atE]
      
      
      He+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms1_hpca_heplus_data_quality]
      
      
      Helium+ Flux for all Elevation Anodes across all energies [mms1_hpca_heplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_heplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_heplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_heplus_flux_byAnode_atE]
      
      
      Helium+ Phase Space Density for all Elevation Anodes across all energies [mms1_hpca_heplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_heplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_heplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_heplus_phase_space_density_byAnode_atE]
      
      
      He++ per sweep status (0=bad): see Data_Quality_Key global attribute [mms1_hpca_heplusplus_data_quality]
      
      
      Helium++ Flux for all Elevation Anodes across all energies [mms1_hpca_heplusplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_heplusplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_heplusplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_heplusplus_flux_byAnode_atE]
      
      
      Helium++ Phase Space Density for all Elevation Anodes across all energies [mms1_hpca_heplusplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_heplusplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_heplusplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_heplusplus_phase_space_density_byAnode_atE]
      
      
      O+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms1_hpca_oplus_data_quality]
      
      
      Oxygen+ Flux for all Elevation Anodes across all energies [mms1_hpca_oplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_oplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_oplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_oplus_flux_byAnode_atE]
      
      
      Oxygen+ Phase Space Density for all Elevation Anodes across all energies [mms1_hpca_oplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms1_hpca_oplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms1_hpca_oplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms1_hpca_oplus_phase_space_density_byAnode_atE]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s), Despun MPA-aligned cartesian coordinates [mms1_hpca_B_GSE_sweep_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s), Geocentric Solar Magnetospheric (GSM) cartesian coordinates [mms1_hpca_B_GSM_sweep_avg]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms1_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms1_hpca_TOF_VMON_MIN_converted]
      
      
      Decimation Factor Index from mode config file [mms1_hpca_decimation_factor_index]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS1_HPCA_SRVY_L2_MOMENTS (spase://NASA/NumericalData/MMS/1/HotPlasmaCompositionAnalyzer/Survey/Level2/Moments/PT10S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Number Density Hydrogen+ for each HPCA half-spin [mms1_hpca_hplus_number_density]
      
      
      ---> Ion Bulk Velocity Hydrogen+ for each HPCA half-spin (x, y, z) [mms1_hpca_hplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Hydrogen+ for each HPCA half-spin [mms1_hpca_hplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_hplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_hplus_temperature_tensor]
      
      
      Number Density Helium+ for each HPCA half-spin [mms1_hpca_heplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium+ for each HPCA half-spin (x, y, z) [mms1_hpca_heplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium+ for each HPCA half-spin [mms1_hpca_heplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_heplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_heplus_temperature_tensor]
      
      
      Number Density Helium++ for each HPCA half-spin [mms1_hpca_heplusplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium++ for each HPCA half-spin (x, y, z) [mms1_hpca_heplusplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium++ for each HPCA half-spin [mms1_hpca_heplusplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_heplusplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_heplusplus_temperature_tensor]
      
      
      Number Density Oxygen+ for each HPCA half-spin [mms1_hpca_oplus_number_density]
      
      
      ---> Ion Bulk Velocity Oxygen+ for each HPCA half-spin (x, y, z) [mms1_hpca_oplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Oxygen+ for each HPCA half-spin [mms1_hpca_oplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_oplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms1_hpca_oplus_temperature_tensor]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms1_hpca_B_GSE_spin_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms1_hpca_B_GSM_spin_avg]
      
      
      Bulk Velocity in GSM for H+ for each HPCA half-spin (x, y, z) [mms1_hpca_hplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp H+ for each HPCA half-spin [mms1_hpca_hplus_tperp]
      
      
      ---> Tparallel H+ for each HPCA half-spin [mms1_hpca_hplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_hplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_hplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_hplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_hplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He+ for each HPCA half-spin (x, y, z) [mms1_hpca_heplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He+ for each HPCA half-spin [mms1_hpca_heplus_tperp]
      
      
      ---> Tparallel He+ for each HPCA half-spin [mms1_hpca_heplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He++ for each HPCA half-spin (x, y, z) [mms1_hpca_heplusplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He++ for each HPCA half-spin [mms1_hpca_heplusplus_tperp]
      
      
      ---> Tparallel He++ for each HPCA half-spin [mms1_hpca_heplusplus_tparallel]
      
      
      Vperp vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplusplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplusplus_vparallel]
      
      
      Vperp vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplusplus_vperp_GSM]
      
      
      Vparallel vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms1_hpca_heplusplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for O+ for each HPCA half-spin (x, y, z) [mms1_hpca_oplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp O+ for each HPCA half-spin [mms1_hpca_oplus_tperp]
      
      
      ---> Tparallel O+ for each HPCA half-spin [mms1_hpca_oplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_oplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_oplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_oplus_vperp_GSM]
      
      
      --->Vparallel vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms1_hpca_oplus_vparallel_GSM]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms1_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms1_hpca_TOF_VMON_MIN_converted]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS1_HPCA_SRVY_L2_TOF-COUNTS (spase://NASA/NumericalData/MMS/1/HotPlasmaCompositionAnalyzer/Survey/Level2/TimeOfFlight/Counts/PT0.625S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      TOF Counts for all angles, across all energies [mms1_hpca_tof_counts]
      
      
      ---> Spectrograms all angles, at selected energies [mms1_hpca_tof_counts_allA_atE]
      
      
      ---> Spectrograms at select angles, for all energies [mms1_hpca_tof_counts_allE_atA]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS1_MEC_BRST_L2_EPHT89D (spase://NASA/NumericalData/MMS/1/Ephemeris/Burst/Level2/Tsyganenko_89_Dynamic/PT0.030S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms1_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms1_mec_gmst]
      
      
      Magnetic Latitude. [mms1_mec_mlat]
      
      
      Magnetic Local Time. [mms1_mec_mlt]
      
      
      Dipole L-shell value. [mms1_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms1_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms1_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms1_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms1_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms1_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms1_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms1_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms1_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms1_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms1_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms1 (km) [mms1_mec_r_eci]
      
      
      Velocity of mms1 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms1_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms1 (km) [mms1_mec_r_gsm]
      
      
      Velocity of mms1 spacecraft in GSM coordinates (km/s) [mms1_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms1 (km) [mms1_mec_r_geo]
      
      
      Velocity of mms1 spacecraft in GEO coordinates (km/s) [mms1_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms1 (km) [mms1_mec_r_sm]
      
      
      Velocity of mms1 spacecraft in SM coordinates (km/s) [mms1_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms1 (km) [mms1_mec_r_gse]
      
      
      Velocity of mms1 spacecraft in GSE coordinates (km/s) [mms1_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms1 (km) [mms1_mec_r_gse2000]
      
      
      Velocity of mms1 spacecraft in GSE2000 coordinates (km/s) [mms1_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms1 spacecraft [mms1_mec_geod_lat]
      
      
      Geodetic longitude of mms1 spacecraft [mms1_mec_geod_lon]
      
      
      Geodetic height of mms1 spacecraft. (Height above WGS84 Spheroid.) [mms1_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms1_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms1_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms1_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms1 spacecraft [mms1_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms1_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms1_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms1 spacecraft [mms1_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms1 spacecraft [mms1_mec_bmin_gsm]
      
      
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MMS1_MEC_BRST_L2_EPHT89Q (spase://NASA/NumericalData/MMS/1/Ephemeris/Burst/Level2/Tsyganenko_89_Quiet/PT0.030S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms1_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms1_mec_gmst]
      
      
      Magnetic Latitude. [mms1_mec_mlat]
      
      
      Magnetic Local Time. [mms1_mec_mlt]
      
      
      Dipole L-shell value. [mms1_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms1_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms1_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms1_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms1_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms1_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms1_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms1_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms1_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms1_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms1_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms1 (km) [mms1_mec_r_eci]
      
      
      Velocity of mms1 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms1_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms1 (km) [mms1_mec_r_gsm]
      
      
      Velocity of mms1 spacecraft in GSM coordinates (km/s) [mms1_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms1 (km) [mms1_mec_r_geo]
      
      
      Velocity of mms1 spacecraft in GEO coordinates (km/s) [mms1_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms1 (km) [mms1_mec_r_sm]
      
      
      Velocity of mms1 spacecraft in SM coordinates (km/s) [mms1_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms1 (km) [mms1_mec_r_gse]
      
      
      Velocity of mms1 spacecraft in GSE coordinates (km/s) [mms1_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms1 (km) [mms1_mec_r_gse2000]
      
      
      Velocity of mms1 spacecraft in GSE2000 coordinates (km/s) [mms1_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms1 spacecraft [mms1_mec_geod_lat]
      
      
      Geodetic longitude of mms1 spacecraft [mms1_mec_geod_lon]
      
      
      Geodetic height of mms1 spacecraft. (Height above WGS84 Spheroid.) [mms1_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms1_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms1_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms1_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms1 spacecraft [mms1_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms1_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms1_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms1 spacecraft [mms1_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms1 spacecraft [mms1_mec_bmin_gsm]
      
      
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MMS1_MEC_BRST_L2_EPHTS04D (spase://NASA/NumericalData/MMS/1/Ephemeris/Burst/Level2/Tsyganenko_04_Dynamic/PT0.030S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms1_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms1_mec_gmst]
      
      
      Magnetic Latitude. [mms1_mec_mlat]
      
      
      Magnetic Local Time. [mms1_mec_mlt]
      
      
      Dipole L-shell value. [mms1_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms1_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms1_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms1_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms1_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms1_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms1_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms1_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms1_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms1_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms1_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms1 (km) [mms1_mec_r_eci]
      
      
      Velocity of mms1 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms1_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms1 (km) [mms1_mec_r_gsm]
      
      
      Velocity of mms1 spacecraft in GSM coordinates (km/s) [mms1_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms1 (km) [mms1_mec_r_geo]
      
      
      Velocity of mms1 spacecraft in GEO coordinates (km/s) [mms1_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms1 (km) [mms1_mec_r_sm]
      
      
      Velocity of mms1 spacecraft in SM coordinates (km/s) [mms1_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms1 (km) [mms1_mec_r_gse]
      
      
      Velocity of mms1 spacecraft in GSE coordinates (km/s) [mms1_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms1 (km) [mms1_mec_r_gse2000]
      
      
      Velocity of mms1 spacecraft in GSE2000 coordinates (km/s) [mms1_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms1 spacecraft [mms1_mec_geod_lat]
      
      
      Geodetic longitude of mms1 spacecraft [mms1_mec_geod_lon]
      
      
      Geodetic height of mms1 spacecraft. (Height above WGS84 Spheroid.) [mms1_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms1_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms1_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms1_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms1 spacecraft [mms1_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms1_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms1_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms1 spacecraft [mms1_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms1 spacecraft [mms1_mec_bmin_gsm]
      
      
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MMS1_MEC_SRVY_L2_EPHT89D (spase://NASA/NumericalData/MMS/1/Ephemeris/Survey/Level2/Tsyganenko_89_Dynamic/PT30S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms1_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms1_mec_gmst]
      
      
      Magnetic Latitude. [mms1_mec_mlat]
      
      
      Magnetic Local Time. [mms1_mec_mlt]
      
      
      Dipole L-shell value. [mms1_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms1_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms1_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms1_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms1_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms1_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms1_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms1_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms1_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms1_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms1_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms1 (km) [mms1_mec_r_eci]
      
      
      Velocity of mms1 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms1_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms1 (km) [mms1_mec_r_gsm]
      
      
      Velocity of mms1 spacecraft in GSM coordinates (km/s) [mms1_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms1 (km) [mms1_mec_r_geo]
      
      
      Velocity of mms1 spacecraft in GEO coordinates (km/s) [mms1_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms1 (km) [mms1_mec_r_sm]
      
      
      Velocity of mms1 spacecraft in SM coordinates (km/s) [mms1_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms1 (km) [mms1_mec_r_gse]
      
      
      Velocity of mms1 spacecraft in GSE coordinates (km/s) [mms1_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms1 (km) [mms1_mec_r_gse2000]
      
      
      Velocity of mms1 spacecraft in GSE2000 coordinates (km/s) [mms1_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms1 spacecraft [mms1_mec_geod_lat]
      
      
      Geodetic longitude of mms1 spacecraft [mms1_mec_geod_lon]
      
      
      Geodetic height of mms1 spacecraft. (Height above WGS84 Spheroid.) [mms1_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms1_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms1_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms1_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms1 spacecraft [mms1_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms1_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms1_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms1 spacecraft [mms1_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms1 spacecraft [mms1_mec_bmin_gsm]
      
      
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MMS1_MEC_SRVY_L2_EPHT89Q (spase://NASA/NumericalData/MMS/1/Ephemeris/Survey/Level2/Tsyganenko_89_Quiet/PT30S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms1_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms1_mec_gmst]
      
      
      Magnetic Latitude. [mms1_mec_mlat]
      
      
      Magnetic Local Time. [mms1_mec_mlt]
      
      
      Dipole L-shell value. [mms1_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms1_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms1_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms1_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms1_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms1_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms1_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms1_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms1_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms1_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms1_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms1 (km) [mms1_mec_r_eci]
      
      
      Velocity of mms1 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms1_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms1 (km) [mms1_mec_r_gsm]
      
      
      Velocity of mms1 spacecraft in GSM coordinates (km/s) [mms1_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms1 (km) [mms1_mec_r_geo]
      
      
      Velocity of mms1 spacecraft in GEO coordinates (km/s) [mms1_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms1 (km) [mms1_mec_r_sm]
      
      
      Velocity of mms1 spacecraft in SM coordinates (km/s) [mms1_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms1 (km) [mms1_mec_r_gse]
      
      
      Velocity of mms1 spacecraft in GSE coordinates (km/s) [mms1_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms1 (km) [mms1_mec_r_gse2000]
      
      
      Velocity of mms1 spacecraft in GSE2000 coordinates (km/s) [mms1_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms1 spacecraft [mms1_mec_geod_lat]
      
      
      Geodetic longitude of mms1 spacecraft [mms1_mec_geod_lon]
      
      
      Geodetic height of mms1 spacecraft. (Height above WGS84 Spheroid.) [mms1_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms1_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms1_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms1_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms1 spacecraft [mms1_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms1_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms1_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms1 spacecraft [mms1_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms1 spacecraft [mms1_mec_bmin_gsm]
      
      
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MMS1_MEC_SRVY_L2_EPHTS04D (spase://NASA/NumericalData/MMS/1/Ephemeris/Survey/Level2/Tsyganenko_04_Dynamic/PT30S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms1_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms1_mec_gmst]
      
      
      Magnetic Latitude. [mms1_mec_mlat]
      
      
      Magnetic Local Time. [mms1_mec_mlt]
      
      
      Dipole L-shell value. [mms1_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms1_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms1_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms1_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms1_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms1_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms1_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms1_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms1_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms1_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms1_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms1 (km) [mms1_mec_r_eci]
      
      
      Velocity of mms1 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms1_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms1 (km) [mms1_mec_r_gsm]
      
      
      Velocity of mms1 spacecraft in GSM coordinates (km/s) [mms1_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms1 (km) [mms1_mec_r_geo]
      
      
      Velocity of mms1 spacecraft in GEO coordinates (km/s) [mms1_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms1 (km) [mms1_mec_r_sm]
      
      
      Velocity of mms1 spacecraft in SM coordinates (km/s) [mms1_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms1 (km) [mms1_mec_r_gse]
      
      
      Velocity of mms1 spacecraft in GSE coordinates (km/s) [mms1_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms1 (km) [mms1_mec_r_gse2000]
      
      
      Velocity of mms1 spacecraft in GSE2000 coordinates (km/s) [mms1_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms1_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms1 spacecraft [mms1_mec_geod_lat]
      
      
      Geodetic longitude of mms1 spacecraft [mms1_mec_geod_lon]
      
      
      Geodetic height of mms1 spacecraft. (Height above WGS84 Spheroid.) [mms1_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms1_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms1_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms1_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms1 spacecraft [mms1_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms1_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms1_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms1 spacecraft [mms1_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms1 spacecraft [mms1_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms1 spacecraft [mms1_mec_bmin_gsm]
      
      
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MMS1_R0_SUMMARY
Description
Pre-generated MMS Quicklook Summary Plots
File location: https://cdaweb.gsfc.nasa.gov/pub/data/mms/ql_plots/al1_mms4_summ 
 
  • Data Variable Descriptions
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MMS1_SCM_BRST_L2_SCB (spase://NASA/NumericalData/MMS/1/FIELDS/SCM/Burst/Level2/PT0.0001220703125S)
Description
The tri-axial search-coil magnetometer (SCM) with its associated preamplifier
provides the three-dimensional measurement of the magnetic field fluctuations.
The analog magnetic waveforms measured by the SCM are digitized and processed
inside the digital signal processor (DSP), collected and stored by the central
instrument data processor (CIDP) via the Fields central electronics box (CEB).
Prior to launch, all SCM Flight models were calibrated by LPP at the National
Magnetic Observatory at Chambon-la-Foret (Orleans). Once per orbit, each SCM
transfer function is checked thanks to the onboard calibration signal provided
by DSP. SCM is operated for the entire MMS orbit in survey mode. Within the ROI,
burst mode data are also acquired as well as high burst mode data. 
SCM data set corresponds to the AC magnetic field waveforms in nanoTesla and in
the GSE frame.
The instrument paper for SCM can be found at
https://urldefense.proofpoint.com/v2/url?u=http-3A__link.springer.com_article_10
.1007_s11214-2D014-2D0096-2D9&d=DwIFAg&c=c6MrceVCY5m5A_KAUkrdoA&r=bjziExGTRYoZgE
2xb_dDSm9NxNIo0lG6Q-rB0Y6rHS4&m=CMzo0Vv9zPtWSdbdY1Wq9-jIkYS2cOMV9JYZsMV10y0&s=Xb
P9PiEAswHGl5lqgsDVI6zs8ivJx7yek9i2undKl10&e= 
Modification History
unpack telemetry, assign sample times
2026-07-10T20:12:20.00006318092028Z - [L1A->L1B (step 1/1)] Calibration
(TMcounts->nT). See CALIBRATION_PARAMETERS for details.
2026-07-16T12:36:26.00005209445941Z - [L1B->L2 (step 1/2)] Coordinate transform
(SCM123->GSE). See COORD_TRANS_PARAMETERS for details.
2026-07-16T12:36:32.00005978345859Z - [L1B->L2 (step 2/2)] Frequency filtering.
See FREQUENCY_FILTER for details.
 
  • Data Variable Descriptions
      L2 AC magnetic field in GSE frame [mms1_scm_acb_gse_scb_brst_l2]
      These calibrated (nT) AC magnetic field waveform data are sampled at 8192S/s.
      They are high-pass filtered above 1.00Hz but not low-pass filtered. See global
      attributes for details. For more information, please have a look at the SCM Data
      Products Guide.
      
      (List/Create Only) Quality Factor (one letter per antenna, G=good) [mms1_scm_qf_scm123_scb_brst_l2]
      Each letter refers to one SCM physical antenna in the SCM123 order. 'G' stands
      for good data, 'Z' for data that are affected or set to zero by convolution
      boundary effect, 'S' for saturated data, 'X' for out of range data, 'B' for
      fillvalue/bad data.
      
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MMS1_SCM_BRST_L2_SCHB (spase://NASA/NumericalData/MMS/1/FIELDS/SCM/Burst/Level2/PT0.00006101515625S)
Description
The tri-axial search-coil magnetometer (SCM) with its associated preamplifier
provides the three-dimensional measurement of the magnetic field fluctuations.
The analog magnetic waveforms measured by the SCM are digitized and processed
inside the digital signal processor (DSP), collected and stored by the central
instrument data processor (CIDP) via the Fields central electronics box (CEB).
Prior to launch, all SCM Flight models were calibrated by LPP at the National
Magnetic Observatory at Chambon-la-Foret (Orleans). Once per orbit, each SCM
transfer function is checked thanks to the onboard calibration signal provided
by DSP. SCM is operated for the entire MMS orbit in survey mode. Within the ROI,
burst mode data are also acquired as well as high burst mode data. 
SCM data set corresponds to the AC magnetic field waveforms in nanoTesla and in
the GSE frame.
The instrument paper for SCM can be found at
http://link.springer.com/article/10.1007/s11214-014-0096-9
Modification History
unpack telemetry, assign sample times
2026-07-10T20:12:49.0000668168036Z - [L1A->L1B (step 1/1)] Calibration
(TMcounts->nT). See CALIBRATION_PARAMETERS for details.
2026-07-16T12:41:02.00004369020467Z - [L1B->L2 (step 1/2)] Coordinate transform
(SCM123->GSE). See COORD_TRANS_PARAMETERS for details.
2026-07-16T12:41:07.00005680322652Z - [L1B->L2 (step 2/2)] Frequency filtering.
See FREQUENCY_FILTER for details.
 
  • Data Variable Descriptions
      L2 AC magnetic field in GSE frame [mms1_scm_acb_gse_schb_brst_l2]
      These calibrated (nT) AC magnetic field waveform data are sampled at 16384S/s.
      They are high-pass filtered above 32.00Hz but not low-pass filtered. See global
      attributes for details. For more information, please have a look at the SCM Data
      Products Guide
      (https://lasp.colorado.edu/mms/sdc/public/datasets/fields/Science_Data_Products_ 
      Guide_vol2_SCM_v11_20160301.pdf).
      
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MMS1_SCM_SRVY_L2_SCSRVY (spase://NASA/NumericalData/MMS/1/FIELDS/SCM/Survey/Level2/PT0.03125S)
Description
The tri-axial search-coil magnetometer (SCM) with its associated preamplifier
provides the three-dimensional measurement of the magnetic field fluctuations.
The analog magnetic waveforms measured by the SCM are digitized and processed
inside the digital signal processor (DSP), collected and stored by the central
instrument data processor (CIDP) via the Fields central electronics box (CEB).
Prior to launch, all SCM Flight models were calibrated by LPP at the National
Magnetic Observatory at Chambon-la-Foret (Orleans). Once per orbit, each SCM
transfer function is checked thanks to the onboard calibration signal provided
by DSP. SCM is operated for the entire MMS orbit in survey mode. Within the ROI,
burst mode data are also acquired as well as high burst mode data. 
SCM data set corresponds to the AC magnetic field waveforms in nanoTesla and in
the GSE frame.
The instrument paper for SCM can be found at
https://urldefense.proofpoint.com/v2/url?u=http-3A__link.springer.com_article_10
.1007_s11214-2D014-2D0096-2D9&d=DwIFAg&c=c6MrceVCY5m5A_KAUkrdoA&r=bjziExGTRYoZgE
2xb_dDSm9NxNIo0lG6Q-rB0Y6rHS4&m=CMzo0Vv9zPtWSdbdY1Wq9-jIkYS2cOMV9JYZsMV10y0&s=Xb
P9PiEAswHGl5lqgsDVI6zs8ivJx7yek9i2undKl10&e= 
Modification History
unpack telemetry, assign sample times
2026-07-02T23:55:03.00004184245717Z - [L1A->L1B (step 1/1)] Calibration
(TMcounts->nT). See CALIBRATION_PARAMETERS for details.
2026-07-15T23:54:12.00003683566739Z - [L1B->L2 (step 1/2)] Coordinate transform
(SCM123->GSE). See COORD_TRANS_PARAMETERS for details.
2026-07-15T23:54:59.00006353854825Z - [L1B->L2 (step 2/2)] Frequency filtering.
See FREQUENCY_FILTER for details.
 
  • Data Variable Descriptions
      L2 AC magnetic field in GSE frame [mms1_scm_acb_gse_scsrvy_srvy_l2]
      These calibrated (nT) AC magnetic field waveform data are sampled at 32S/s. They
      are high-pass filtered above 0.50Hz but not low-pass filtered. See global
      attributes for details. For more information, please have a look at the SCM Data
      Products Guide.
      
      (List/Create Only) Quality Factor (one letter per antenna, G=good) [mms1_scm_qf_scm123_scsrvy_srvy_l2]
      Each letter refers to one SCM physical antenna in the SCM123 order. 'G' stands
      for good data, 'Z' for data that are affected or set to zero by convolution
      boundary effect, 'S' for saturated data, 'X' for out of range data, 'B' for
      fillvalue/bad data.
      
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MMS2_ASPOC_SRVY_L2 (spase://NASA/NumericalData/MMS/2/ASPOC/Survey/Level2/PT1S)
Description
K. Torkar et al, Active Spacecraft Potential Control Investigation
Space Science Reviews, 2014, DOI: 10.1007/s11214-014-0049-3
Further information:
- http://www.iwf.oeaw.ac.at/en/research/near-earth-space/mms/ 
- http://mms.space.swri.edu/ 
Modification History
150224 Initial version
150831 Minor updates and fixes
160205 CDF file format guide compliant
 
  • Data Variable Descriptions
      ASPOC Ion Emission Current Sum, 1s resolution [mms2_aspoc_ionc]
      
      
      ASPOC Unit 1 Ion Emission Current, 1s resolution [mms2_asp1_ionc]
      
      
      ASPOC Unit 2 Ion Emission Current, 1s resolution [mms2_asp2_ionc]
      
      
      ASPOC Unit 1 Emitted Beam Energy, 1s resolution [mms2_asp1_energy]
      
      
      ASPOC Unit 2 Emitted Beam Energy, 1s resolution [mms2_asp2_energy]
      
      
      ASPOC Data Quality and Instrument Status, 1s resolution [mms2_aspoc_status]
      
      
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MMS2_DSP_FAST_L2_BPSD (spase://NASA/NumericalData/MMS/2/FIELDS/DSP/Fast/Level2/MagneticFieldPowerSpectralDensity/PT2S)
Description
BPSD is the low frequency B spectral density covering the frequency range of .2
to 6000 Hz.
 
  • Data Variable Descriptions
      SCM Axis 1 (X) component magnetic power spectral density [mms2_dsp_bpsd_scm1_fast_l2]
      
      
      SCM Axis 2 (Y, ~direction of S/C Z) component magnetic power spectral density [mms2_dsp_bpsd_scm2_fast_l2]
      
      
      SCM Axis 3 (Z) component magnetic power spectral density [mms2_dsp_bpsd_scm3_fast_l2]
      
      
      Omni-directional magnetic power spectral density: square root of the sum of the squares of 3 components [mms2_dsp_bpsd_omni_fast_l2]
      
      
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MMS2_DSP_FAST_L2_EPSD (spase://NASA/NumericalData/MMS/2/FIELDS/DSP/Fast/Level2/ElectricFieldPowerSpectralDensity/PT2S)
Description
EPSD combines the low frequency E spectral density covering the frequency range
of 1 to 8000 Hz and the  medium frequency E spectral density covering the
frequency range of .25 to 100 kHz.
 
  • Data Variable Descriptions
      null [mms2_dsp_epsd_x]
      
      
      null [mms2_dsp_epsd_y]
      
      
      null [mms2_dsp_epsd_z]
      
      
      null [mms2_dsp_epsd_omni]
      
      
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MMS2_DSP_SLOW_L2_BPSD (spase://NASA/NumericalData/MMS/2/FIELDS/DSP/Slow/Level2/MagneticFieldPowerSpectralDensity/PT16S)
Description
search coil magnetometer spectral density
 
  • Data Variable Descriptions
      SCM1 component magnetic power spectral density [mms2_dsp_bpsd_scm1_slow_l2]
      
      
      SCM2 component magnetic power spectral density - NO DATA in Slow Survey [mms2_dsp_bpsd_scm2_slow_l2]
      
      
      SCM3 component magnetic power spectral density [mms2_dsp_bpsd_scm3_slow_l2]
      
      
      Omni-directional magnetic power spectral density: square root of the sum of the squares of 2 components [mms2_dsp_bpsd_omni_slow_l2]
      
      
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MMS2_DSP_SLOW_L2_EPSD (spase://NASA/NumericalData/MMS/2/FIELDS/DSP/Slow/Level2/ElectricFieldPowerSpectralDensity/PT16S)
Description
electric spectral density
 
  • Data Variable Descriptions
      null [mms2_dsp_epsd_x]
      
      
      null [mms2_dsp_epsd_y]
      
      
      null [mms2_dsp_epsd_z]
      
      
      null [mms2_dsp_epsd_omni]
      
      
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MMS2_EDI_BRST_L2_AMB (spase://NASA/NumericalData/MMS/2/FIELDS/EDI/Burst/Level2/ElectronFluxAmbient/ProjectionMethod1/PT0.0009765625S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - Original version.
v1.0.0 - Include trajectory vectors and optics state.
v1.1.0 - Update metadata: counts -> flux.
v1.2.0 - Added flux error.
v1.3.0 - Trajectory vector errors are now deltas.
v1.4.0 - Fixed dead-time correction and error values.
v1.5.0 - Factor of 2 for accumulation time & 2 for abscal factor in srvy mode.
v1.6.0 - No factor of 2 for accumulation time in srvy mode.
v2.0.0 - Reduced file size with scalar errors. Update metadata.
v2.1.0 - Correct fill value for fluxes.
v3.0.0 - Omni-directional error for trajectories. Y-Version linked to cal file.
Single epoch for counts.
v4.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
 
  • Data Variable Descriptions
      Optics state [mms2_edi_optics_state_brst_l2]
      
      
      ---> GDU1 energy [mms2_edi_energy_gdu1_brst_l2]
      
      
      ---> GDU2 energy [mms2_edi_energy_gdu2_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-1 0PA [mms2_edi_flux1_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-1 0PA [mms2_edi_flux1_0_brst_l2_noerr]
      
      
      ---> Error for flux1 0-degree pitch angle electron flux. [mms2_edi_flux1_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-2 0PA [mms2_edi_flux2_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-2 0PA [mms2_edi_flux2_0_brst_l2_noerr]
      
      
      ---> Error for flux2 0-degree pitch angle electron flux. [mms2_edi_flux2_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-3 0PA [mms2_edi_flux3_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-3 0PA [mms2_edi_flux3_0_brst_l2_noerr]
      
      
      ---> Error for flux3 0-degree pitch angle electron flux. [mms2_edi_flux3_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-4 0PA [mms2_edi_flux4_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-4 0PA [mms2_edi_flux4_0_brst_l2_noerr]
      
      
      ---> Error for flux4 0-degree pitch angle electron flux. [mms2_edi_flux4_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-1 180PA [mms2_edi_flux1_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-1 180PA [mms2_edi_flux1_180_brst_l2_noerr]
      
      
      ---> Error for flux1 180-degree pitch angle electron flux. [mms2_edi_flux1_180_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by traj2 180PA [mms2_edi_flux2_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-2 180PA [mms2_edi_flux2_180_brst_l2_noerr]
      
      
      ---> Error for flux2 180-degree pitch angle electron flux. [mms2_edi_flux2_180_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by traj3 180PA [mms2_edi_flux3_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-3 180PA [mms2_edi_flux3_180_brst_l2_noerr]
      
      
      ---> Error for flux3 180-degree pitch angle electron flux. [mms2_edi_flux3_180_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by traj4 180PA [mms2_edi_flux4_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-4 180PA [mms2_edi_flux4_180_brst_l2_noerr]
      
      
      ---> Error for flux4 180-degree pitch angle electron flux. [mms2_edi_flux4_180_delta_brst_l2]
      
      
      Trajectory of flux1 0-degree pitch angle electrons in GSE coordinates. [mms2_edi_traj1_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 0-degree pitch angle electrons in GSE coordinates. [mms2_edi_traj2_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 0-degree pitch angle electrons in GSE coordinates. [mms2_edi_traj3_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 0-degree pitch angle electrons in GSE coordinates. [mms2_edi_traj4_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of flux1 180-degree pitch angle electrons in GSE coordinates. [mms2_edi_traj1_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 180-degree pitch angle electrons in GSE coordinates. [mms2_edi_traj2_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 180-degree pitch angle electrons in GSE coordinates. [mms2_edi_traj3_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 180-degree pitch angle electrons in GSE coordinates. [mms2_edi_traj4_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj1_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 0-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj2_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 0-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj3_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 0-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj4_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj1_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 180-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj2_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 180-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj3_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 180-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj4_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms2_edi_traj1_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms2_edi_traj2_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms2_edi_traj3_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms2_edi_traj4_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms2_edi_traj1_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms2_edi_traj2_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms2_edi_traj3_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms2_edi_traj4_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS2_EDI_BRST_L2_AMB-PM2 (spase://NASA/NumericalData/MMS/2/FIELDS/EDI/Burst/Level2/AmbientElectronFlux/ProjectionMethod2/PT0.0009765625S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v1.0.0 - Original version.
v1.1.0 - Correct fill value for fluxes.
v2.0.0 - Omni-directional error for trajectories. Y-Version linked to cal file.
Single epoch for counts.
v3.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
v4.0.0 - Each trajectory has its own LABL_PTR_1 variable.
 
  • Data Variable Descriptions
      Optics state [mms2_edi_optics_state_brst_l2]
      
      
      ---> GDU1 energy [mms2_edi_energy_gdu1_brst_l2]
      
      
      ---> GDU2 energy [mms2_edi_energy_gdu2_brst_l2]
      
      
      Field-aligned electron flux from channel 1 of both GDUs [mms2_edi_flux1_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 1 of both GDUs [mms2_edi_flux1_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 1 of both GDUs. [mms2_edi_flux1_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 1 of both GDUs [mms2_edi_flux1_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 1 of both GDUs [mms2_edi_flux1_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 1 of both GDUs. [mms2_edi_flux1_180_delta_brst_l2]
      
      
      Field-aligned electron flux from channel 2 of both GDUs [mms2_edi_flux2_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 2 of both GDUs [mms2_edi_flux2_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 2 of both GDUs. [mms2_edi_flux2_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 2 of both GDUs [mms2_edi_flux2_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 2 of both GDUs [mms2_edi_flux2_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 2 of both GDUs. [mms2_edi_flux2_180_delta_brst_l2]
      
      
      Field-aligned electron flux from channel 3 of both GDUs [mms2_edi_flux3_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 3 of both GDUs [mms2_edi_flux3_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 3 of both GDUs. [mms2_edi_flux3_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 3 of both GDUs [mms2_edi_flux3_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 3 of both GDUs [mms2_edi_flux3_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 3 of both GDUs. [mms2_edi_flux3_180_delta_brst_l2]
      
      
      Field-aligned electron flux from channel 4 of both GDUs [mms2_edi_flux4_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 4 of both GDUs [mms2_edi_flux4_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 4 of both GDUs. [mms2_edi_flux4_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 4 of both GDUs [mms2_edi_flux4_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 4 of both GDUs [mms2_edi_flux4_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 4 of both GDUs. [mms2_edi_flux4_180_delta_brst_l2]
      
      
      Trajectory of field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms2_edi_traj1_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms2_edi_traj1_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 1 of both GDUs in GSE coordinates. [mms2_edi_traj1_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 1 of both GDUs, in GSE coordinates. [mms2_edi_traj1_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms2_edi_traj2_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms2_edi_traj2_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 2 of both GDUs in GSE coordinates. [mms2_edi_traj2_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 2 of both GDUs, in GSE coordinates. [mms2_edi_traj2_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms2_edi_traj3_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms2_edi_traj3_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 3 of both GDUs in GSE coordinates. [mms2_edi_traj3_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 3 of both GDUs, in GSE coordinates. [mms2_edi_traj3_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms2_edi_traj4_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms2_edi_traj4_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 4 of both GDUs in GSE coordinates. [mms2_edi_traj4_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 4 of both GDUs, in GSE coordinates. [mms2_edi_traj4_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj1_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj1_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS2_EDI_BRST_L2_EFIELD (spase://NASA/NumericalData/MMS/2/FIELDS/EDI/Burst/Level2/ElectricField/PT0.0009765625S)
Description
EDI electric field data. Instrument papers for EDI can be found at:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7
Modification History
v1.0.0 - First version. TRI-TOF selection based on smallest error.
v1.1.0 - TRI-TOF merged by weighted average.
v1.2.0 - Fixed t_delta_plus/minus CDF_type.
v1.3.0 - Fixed Fixed vdrift SI conversion.
v1.4.0 - Fixed data duplication caused by multiple l2pre file locations.
v1.5.0 - Inplemented baseline*beams*Bmag filter for triangulation.
v1.6.0 - Inplemented null files for no or low quality data.
 
  • Data Variable Descriptions
      ExB drift velocity in DSL coordinates. [mms2_edi_vdrift_dsl_brst_l2]
      
      
      ---> ExB drift velocity in DSL coordinates (no error bars) [mms2_edi_vdrift_dsl_brst_l2_noerr]
      
      
      ExB drift velocity in GSE coordinates. [mms2_edi_vdrift_gse_brst_l2]
      
      
      ---> ExB drift velocity in GSE coordinates (no error bars) [mms2_edi_vdrift_gse_brst_l2_noerr]
      
      
      ExB drift velocity in GSM coordinates. [mms2_edi_vdrift_gsm_brst_l2]
      
      
      ---> ExB drift velocity in GSM coordinates (no error bars) [mms2_edi_vdrift_gsm_brst_l2_noerr]
      
      
      Electric field in DSL coordinates. [mms2_edi_e_dsl_brst_l2]
      
      
      ---> Electric field in DSL coordinates (no error bars) [mms2_edi_e_dsl_brst_l2_noerr]
      
      
      Electric field in GSE coordinates. [mms2_edi_e_gse_brst_l2]
      
      
      ---> Electric field in GSE coordinates (no error bars) [mms2_edi_e_gse_brst_l2_noerr]
      
      
      Electric field in GSM coordinates. [mms2_edi_e_gsm_brst_l2]
      
      
      ---> Electric field in GSM coordinates (no error bars) [mms2_edi_e_gsm_brst_l2_noerr]
      
      
      Weighted use of TRI method in L2 results. [mms2_edi_tri_weight_brst_l2]
      
      
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MMS2_EDI_BRST_L2_Q0 (spase://NASA/NumericalData/MMS/2/FIELDS/EDI/Burst/Level2/QualityZero/PT0.0078125S)
Description
EDI Q0 data. The EDI instrument paper and data products guidescan be found at
the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - First version.
v0.0.1 - Filled energy variables.
v0.0.2 - Energy written properly.
v1.0.0 - Update variable names.
v1.1.0 - Added optics state.
v2.0.0 - Added electron trajectories.
v2.1.0 - Deltas on trajectory vectors are now deltas.
v3.0.0 - Reduced file size with scalar errors. Add VAR_NOTES.
v3.1.0 - Fixed optics datatype.
v4.0.0 - Removed unused Epoch variable.
v5.0.0 - Trajectories are provided in DBCS coordinates.
 
  • Data Variable Descriptions
      Optics state [mms2_edi_optics_state_brst_l2]
      
      
      ---> GDU1 energy [mms2_edi_energy_gdu1_brst_l2]
      
      
      ---> GDU2 energy [mms2_edi_energy_gdu2_brst_l2]
      
      
      GDU1 quality 0 counts. [mms2_edi_counts_gdu1_brst_l2]
      Q0 data consists of raw electron counts. The error at any one time is the
      square-root of the counts. Note that there may be contamination from the EDI
      electron beams. See the data products guide or contact an EDI team member to
      learn about beam contamination.
      
      GDU2 quality 0 counts. [mms2_edi_counts_gdu2_brst_l2]
      
      
      GDU1 electron incident trajectory vectors in spherical BCS coordinates. [mms2_edi_traj_bcs_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical BCS coordinates. [mms2_edi_traj_bcs_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical DBCS coordinates. [mms2_edi_traj_dbcs_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical DBCS coordinates. [mms2_edi_traj_dbcs_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSE coordinates. [mms2_edi_traj_gse_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSE coordinates. [mms2_edi_traj_gse_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSM coordinates. [mms2_edi_traj_gsm_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSM coordinates. [mms2_edi_traj_gsm_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS2_EDI_SRVY_L2_AMB (spase://NASA/NumericalData/MMS/2/FIELDS/EDI/Survey/Level2/ElectronFluxAmbient/ProjectionMethod1/PT0.03125S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - Original version.
v1.0.0 - Include trajectory vectors and optics state.
v1.1.0 - Update metadata: counts -> flux.
v1.2.0 - Added flux error.
v1.3.0 - Trajectory vector errors are now deltas.
v1.4.0 - Fixed dead-time correction and error values.
v1.5.0 - Factor of 2 for accumulation time & 2 for abscal factor in srvy mode.
v1.6.0 - No factor of 2 for accumulation time in srvy mode.
v2.0.0 - Reduced file size with scalar errors. Update metadata.
v2.1.0 - Correct fill value for fluxes.
v3.0.0 - Omni-directional error for trajectories. Correct time deltas. Y-Version
linked to cal file. Single epoch for counts.
v4.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
 
  • Data Variable Descriptions
      Optics state [mms2_edi_optics_state_srvy_l2]
      
      
      ---> GDU1 energy [mms2_edi_energy_gdu1_srvy_l2]
      
      
      ---> GDU2 energy [mms2_edi_energy_gdu2_srvy_l2]
      
      
      Field-aligned electron flux from both GDUs [mms2_edi_flux1_0_srvy_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from both GDUs [mms2_edi_flux1_0_srvy_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from both GDUs. [mms2_edi_flux1_0_delta_srvy_l2]
      
      
      Anti-field-aligned electron flux from both GDUs [mms2_edi_flux1_180_srvy_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from both GDUs [mms2_edi_flux1_180_srvy_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from both GDUs. [mms2_edi_flux1_180_delta_srvy_l2]
      
      
      Trajectory of field-aligned electrons from both GDUs in DBCS coordinates. [mms2_edi_traj1_dbcs_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs in DBCS coordinates. [mms2_edi_traj1_dbcs_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from both GDUs in GSE coordinates. [mms2_edi_traj1_gse_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs, in GSE coordinates. [mms2_edi_traj1_gse_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj1_gsm_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj1_gsm_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS2_EDI_SRVY_L2_AMB-PM2 (spase://NASA/NumericalData/MMS/2/FIELDS/EDI/Survey/Level2/ElectronFluxAmbient/ProjectionMethod2/PT0.03125S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v1.0.0 - Original version.
v1.1.0 - Correct fill value for fluxes.
v2.0.0 - Omni-directional error for trajectories. Y-Version linked to cal file.
Single epoch for counts.
v3.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
v4.0.0 - Each trajectory has its own LABL_PTR_1 variable.
 
  • Data Variable Descriptions
      Optics state [mms2_edi_optics_state_srvy_l2]
      
      
      ---> GDU1 energy [mms2_edi_energy_gdu1_srvy_l2]
      
      
      ---> GDU2 energy [mms2_edi_energy_gdu2_srvy_l2]
      
      
      Field-aligned electron flux from both GDUs [mms2_edi_flux1_0_srvy_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from both GDUs [mms2_edi_flux1_0_srvy_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from both GDUs. [mms2_edi_flux1_0_delta_srvy_l2]
      
      
      Anti-field-aligned electron flux from both GDUs [mms2_edi_flux1_180_srvy_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from both GDUs [mms2_edi_flux1_180_srvy_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from both GDUs. [mms2_edi_flux1_180_delta_srvy_l2]
      
      
      Trajectory of field-aligned electrons from both GDUs in DBCS coordinates. [mms2_edi_traj1_dbcs_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs in DBCS coordinates. [mms2_edi_traj1_dbcs_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from both GDUs in GSE coordinates. [mms2_edi_traj1_gse_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs, in GSE coordinates. [mms2_edi_traj1_gse_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj1_gsm_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms2_edi_traj1_gsm_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS2_EDI_SRVY_L2_EFIELD (spase://NASA/NumericalData/MMS/2/FIELDS/EDI/Survey/Level2/ElectricField/PT5S)
Description
EDI electric field data. Instrument papers for EDI can be found at:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7
Modification History
v1.0.0 - First version. TRI-TOF selection based on smallest error.
v1.1.0 - TRI-TOF merged by weighted average.
v1.2.0 - Fixed t_delta_plus/minus CDF_type.
v1.3.0 - Fixed Fixed vdrift SI conversion.
v1.4.0 - Fixed data duplication caused by multiple l2pre file locations.
v1.5.0 - Inplemented baseline*beams*Bmag filter for triangulation.
v1.6.0 - Inplemented null files for no or low quality data.
 
  • Data Variable Descriptions
      ExB drift velocity in DSL coordinates. [mms2_edi_vdrift_dsl_srvy_l2]
      
      
      ---> ExB drift velocity in DSL coordinates (no error bars) [mms2_edi_vdrift_dsl_srvy_l2_noerr]
      
      
      ExB drift velocity in GSE coordinates. [mms2_edi_vdrift_gse_srvy_l2]
      
      
      ---> ExB drift velocity in GSE coordinates (no error bars) [mms2_edi_vdrift_gse_srvy_l2_noerr]
      
      
      ExB drift velocity in GSM coordinates. [mms2_edi_vdrift_gsm_srvy_l2]
      
      
      ---> ExB drift velocity in GSM coordinates (no error bars) [mms2_edi_vdrift_gsm_srvy_l2_noerr]
      
      
      Electric field in DSL coordinates. [mms2_edi_e_dsl_srvy_l2]
      
      
      ---> Electric field in DSL coordinates (no error bars) [mms2_edi_e_dsl_srvy_l2_noerr]
      
      
      Electric field in GSE coordinates. [mms2_edi_e_gse_srvy_l2]
      
      
      ---> Electric field in GSE coordinates (no error bars) [mms2_edi_e_gse_srvy_l2_noerr]
      
      
      Electric field in GSM coordinates. [mms2_edi_e_gsm_srvy_l2]
      
      
      ---> Electric field in GSM coordinates (no error bars) [mms2_edi_e_gsm_srvy_l2_noerr]
      
      
      Weighted use of TRI method in L2 results. [mms2_edi_tri_weight_srvy_l2]
      
      
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MMS2_EDI_SRVY_L2_Q0 (spase://NASA/NumericalData/MMS/2/FIELDS/EDI/Survey/Level2/QualityZero/PT0.125S)
Description
EDI Q0 data. The EDI instrument paper and data products guidescan be found at
the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - First version.
v0.0.1 - Filled energy variables.
v0.0.2 - Energy written properly.
v1.0.0 - Update variable names.
v1.1.0 - Added optics state.
v2.0.0 - Added electron trajectories.
v2.1.0 - Deltas on trajectory vectors are now deltas.
v3.0.0 - Reduced file size with scalar errors. Add VAR_NOTES.
v4.0.0 - Removed unused Epoch variable.
v5.0.0 - Trajectories are provided in DBCS coordinates.
 
  • Data Variable Descriptions
      Optics state [mms2_edi_optics_state_srvy_l2]
      
      
      ---> GDU1 energy [mms2_edi_energy_gdu1_srvy_l2]
      
      
      ---> GDU2 energy [mms2_edi_energy_gdu2_srvy_l2]
      
      
      GDU1 quality 0 counts. [mms2_edi_counts_gdu1_srvy_l2]
      Q0 data consists of raw electron counts. The error at any one time is the
      square-root of the counts. Note that there may be contamination from the EDI
      electron beams. See the data products guide or contact an EDI team member to
      learn about beam contamination.
      
      GDU2 quality 0 counts. [mms2_edi_counts_gdu2_srvy_l2]
      
      
      GDU1 electron incident trajectory vectors in spherical BCS coordinates. [mms2_edi_traj_bcs_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical BCS coordinates. [mms2_edi_traj_bcs_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical DBCS coordinates. [mms2_edi_traj_dbcs_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical DBCS coordinates. [mms2_edi_traj_dbcs_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSE coordinates. [mms2_edi_traj_gse_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSE coordinates. [mms2_edi_traj_gse_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSM coordinates. [mms2_edi_traj_gsm_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSM coordinates. [mms2_edi_traj_gsm_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS2_EDP_BRST_L2_DCE (spase://NASA/NumericalData/MMS/2/FIELDS/EDP/Burst/Level2/DCElectricField/PT0.0001220703125S)
Description
http://mms.gsfc.nasa.gov/
Modification History
V.0. Initial release.
 
  • Data Variable Descriptions
      L2 DC E Field (GSE coords) calibrated for SDP and ADP, all flag values included [mms2_edp_dce_gse_brst_l2]
      
      
      L2 DC E Field (DSL coords) calibrated for SDP and ADP, all flag values included [mms2_edp_dce_dsl_brst_l2]
      
      
      L2 DC E Parallel Field calibrated for SDP and ADP [mms2_edp_dce_par_epar_brst_l2]
      
      
      Quality indicator (3 good), (2 ok data, use with some caution), (1 bad data, use with caution), (0 Really bad data or no data at all) [mms2_edp_quality_brst_l2]
      
      
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MMS2_EDP_BRST_L2_HMFE (spase://NASA/NumericalData/MMS/2/FIELDS/EDP/Burst/Level2Pre/HMFE/PT0.00001525878906S)
Description
 d
 
  • Data Variable Descriptions
      DC E Field calibrated for SDP and ADP [mms2_edp_hmfe_dsl_brst_l2]
      
      
      DC E parallel Field from calibrated SDP and ADP [mms2_edp_hmfe_par_epar_brst_l2]
      
      
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MMS2_EDP_BRST_L2_SCPOT doi:10.48322/a6r6-hr28
Proper citations should include the "Accessed on date" in the form .
Description
http://mms.gsfc.nasa.gov/
The full name of PI affiliations: SWRI - Southwest Research Institute. LASP -
Laboratory for Atmospheric and Space Physics. KTH - Kungliga Tekniska Hogskolan
(Swedish Royal Institute of Technology). 
Modification History
V.0. Initial release.
V.1. QL (v1.0.z), SCPOT (v1.0.z), L2A (v0.1.z) now uses ASPOC srvy l2 and
DEFATT, if these are available. Brst QL uses intermediate L2A file from Fast
mode for delta offsets. Bitmask changed to uint16 and Quality to uint8.
V.2. SCPOT (v2.0.z), L2A (v1.0.z) now uses variable names in accordance with new
recommended standard for FIELDS, All products change shortening factor to 1.25
on SDP, offsets applied indicated by GlobalAttribute Calibration_file.
V.2. L2a (v2.0.z), QL (v1.6.z) now try to remove solar wind wake which
previously left a clear sinusodial signal in the data.
V.3. L2a (v3.0.z) Slow Mode probe Gain set to 1.0 when orbital radius less than
5 RE (1.25 otherwise), L2pre (v2.0.z) DSL offsets removed from field is now
included in the file as the Slow mode is dependent on scpot product (Fast/Brst
is simply based on offset in Calibration_file).
 
  • Data Variable Descriptions
      Spacecraft potential [mms2_edp_scpot_brst_l2]
      
      
      Probe to spacecraft potential, averaged [mms2_edp_psp_brst_l2]
      
      
      Probe to spacecraft potential, individual probes [mms2_edp_dcv_brst_l2]
      
      
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MMS2_EDP_FAST_L2_DCE (spase://NASA/NumericalData/MMS/2/FIELDS/EDP/Fast/Level2/DCElectricField/PT0.03125S)
Description
http://mms.gsfc.nasa.gov/
Modification History
V.0. Initial release.
 
  • Data Variable Descriptions
      L2 DC E Field (GSE coords) calibrated for SDP and ADP, all flag values included [mms2_edp_dce_gse_fast_l2]
      
      
      L2 DC E Field (DSL coords) calibrated for SDP and ADP, all flag values included [mms2_edp_dce_dsl_fast_l2]
      
      
      L2 DC E Parallel Field with error calibrated for SDP and ADP [mms2_edp_dce_par_epar_fast_l2]
      
      
      Approximate DC E field error derived from SDP (quality and bitmask) and ADP (residue) [mms2_edp_dce_err_fast_l2]
      
      
      Quality indicator (3 good), (2 ok data, use with some caution), (1 bad data, use with caution), (0 Really bad data or no data at all) [mms2_edp_quality_fast_l2]
      
      
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MMS2_EDP_FAST_L2_SCPOT doi:10.48322/myvz-be60
Proper citations should include the "Accessed on date" in the form .
Description
http://mms.gsfc.nasa.gov/
The full name of PI affiliations: SWRI - Southwest Research Institute. LASP -
Laboratory for Atmospheric and Space Physics. KTH - Kungliga Tekniska Hogskolan
(Swedish Royal Institute of Technology). 
Modification History
V.0. Initial release.
V.1. QL (v1.0.z), SCPOT (v1.0.z), L2A (v0.1.z) now uses ASPOC srvy l2 and
DEFATT, if these are available. Brst QL uses intermediate L2A file from Fast
mode for delta offsets. Bitmask changed to uint16 and Quality to uint8.
V.2. SCPOT (v2.0.z), L2A (v1.0.z) now uses variable names in accordance with new
recommended standard for FIELDS, All products change shortening factor to 1.25
on SDP, offsets applied indicated by GlobalAttribute Calibration_file.
V.2. L2a (v2.0.z), QL (v1.6.z) now try to remove solar wind wake which
previously left a clear sinusodial signal in the data.
V.3. L2a (v3.0.z) Slow Mode probe Gain set to 1.0 when orbital radius less than
5 RE (1.25 otherwise), L2pre (v2.0.z) DSL offsets removed from field is now
included in the file as the Slow mode is dependent on scpot product (Fast/Brst
is simply based on offset in Calibration_file).
 
  • Data Variable Descriptions
      Spacecraft potential [mms2_edp_scpot_fast_l2]
      
      
      Probe to spacecraft potential, averaged [mms2_edp_psp_fast_l2]
      
      
      Probe to spacecraft potential, individual probes [mms2_edp_dcv_fast_l2]
      
      
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MMS2_EDP_SLOW_L2_DCE (spase://NASA/NumericalData/MMS/2/FIELDS/EDP/Slow/Level2/DCElectricField/PT0.125S)
Description
http://mms.gsfc.nasa.gov/
Modification History
V.0. Initial release.
 
  • Data Variable Descriptions
      L2 DC E Field (GSE coords) calibrated for SDP and ADP, all flag values included [mms2_edp_dce_gse_slow_l2]
      
      
      L2 DC E Field (DSL coords) calibrated for SDP and ADP, all flag values included [mms2_edp_dce_dsl_slow_l2]
      
      
      L2 DC E Parallel Field with error calibrated for SDP and ADP [mms2_edp_dce_par_epar_slow_l2]
      
      
      Approximate DC E field error derived from SDP (quality and bitmask) and ADP (residue) [mms2_edp_dce_err_slow_l2]
      
      
      Quality indicator (3 good), (2 ok data, use with some caution), (1 bad data, use with caution), (0 Really bad data or no data at all) [mms2_edp_quality_slow_l2]
      
      
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MMS2_EDP_SLOW_L2_SCPOT doi:10.48322/mgay-bk26
Proper citations should include the "Accessed on date" in the form .
Description
http://mms.gsfc.nasa.gov/
The full name of PI affiliations: SWRI - Southwest Research Institute. LASP -
Laboratory for Atmospheric and Space Physics. KTH - Kungliga Tekniska Hogskolan
(Swedish Royal Institute of Technology). 
Modification History
V.0. Initial release.
V.1. QL (v1.0.z), SCPOT (v1.0.z), L2A (v0.1.z) now uses ASPOC srvy l2 and
DEFATT, if these are available. Brst QL uses intermediate L2A file from Fast
mode for delta offsets. Bitmask changed to uint16 and Quality to uint8.
V.2. SCPOT (v2.0.z), L2A (v1.0.z) now uses variable names in accordance with new
recommended standard for FIELDS, All products change shortening factor to 1.25
on SDP, offsets applied indicated by GlobalAttribute Calibration_file.
V.2. L2a (v2.0.z), QL (v1.6.z) now try to remove solar wind wake which
previously left a clear sinusodial signal in the data.
V.3. L2a (v3.0.z) Slow Mode probe Gain set to 1.0 when orbital radius less than
5 RE (1.25 otherwise), L2pre (v2.0.z) DSL offsets removed from field is now
included in the file as the Slow mode is dependent on scpot product (Fast/Brst
is simply based on offset in Calibration_file).
 
  • Data Variable Descriptions
      Spacecraft potential [mms2_edp_scpot_slow_l2]
      
      
      Probe to spacecraft potential, averaged [mms2_edp_psp_slow_l2]
      
      
      Probe to spacecraft potential, individual probes [mms2_edp_dcv_slow_l2]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS2_EDP_SRVY_L2_HFESP (spase://NASA/NumericalData/MMS/2/FIELDS/EDP/Survey/Level2/HighFrequencyElectricFieldSpectra/PT16S)
Description
 AC Electric Field
 
  • Data Variable Descriptions
      HF ACE E Field Spectral Density [mms2_edp_hfesp_srvy_l2]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS2_EPD-EIS_BRST_L2_EXTOF (spase://NASA/NumericalData/MMS/2/EnergeticParticleDetector/EIS/Burst/Level2/EnergyByTimeOfFlight/PT0.605S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms2_epd_eis_brst_l2_extof_duration]
      
      
      ---> Instrument Deadtime [mms2_epd_eis_brst_l2_extof_deadtime]
      
      
      ---> Instrument Large Pixel in Use [mms2_epd_eis_brst_l2_extof_largepixel]
      
      
      ---> Spin [mms2_epd_eis_brst_l2_extof_spin]
      
      
      ---> Sector [mms2_epd_eis_brst_l2_extof_sector]
      
      
      ---> Quality Word [mms2_epd_eis_brst_l2_extof_quality]
      
      
      MMS2 ExTOF-Burst proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_extof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms2_epd_eis_brst_l2_extof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms2_epd_eis_brst_l2_extof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms2_epd_eis_brst_l2_extof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms2_epd_eis_brst_l2_extof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms2_epd_eis_brst_l2_extof_proton_P6_counts_t5]
      
      
      MMS2 ExTOF-Burst proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_extof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms2_epd_eis_brst_l2_extof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms2_epd_eis_brst_l2_extof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms2_epd_eis_brst_l2_extof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms2_epd_eis_brst_l2_extof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms2_epd_eis_brst_l2_extof_proton_P6_cps_t5]
      
      
      MMS2 ExTOF-Burst proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_extof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms2_epd_eis_brst_l2_extof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms2_epd_eis_brst_l2_extof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms2_epd_eis_brst_l2_extof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms2_epd_eis_brst_l2_extof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms2_epd_eis_brst_l2_extof_proton_P6_flux_t5]
      
      
      MMS2 ExTOF-Burst helium_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_extof_helium_P6_counts_t0]
      
      
      ---> helium_P6_counts_t1 [mms2_epd_eis_brst_l2_extof_helium_P6_counts_t1]
      
      
      ---> helium_P6_counts_t2 [mms2_epd_eis_brst_l2_extof_helium_P6_counts_t2]
      
      
      ---> helium_P6_counts_t3 [mms2_epd_eis_brst_l2_extof_helium_P6_counts_t3]
      
      
      ---> helium_P6_counts_t4 [mms2_epd_eis_brst_l2_extof_helium_P6_counts_t4]
      
      
      ---> helium_P6_counts_t5 [mms2_epd_eis_brst_l2_extof_helium_P6_counts_t5]
      
      
      MMS2 ExTOF-Burst helium_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_extof_helium_P6_cps_t0]
      
      
      ---> helium_P6_cps_t1 [mms2_epd_eis_brst_l2_extof_helium_P6_cps_t1]
      
      
      ---> helium_P6_cps_t2 [mms2_epd_eis_brst_l2_extof_helium_P6_cps_t2]
      
      
      ---> helium_P6_cps_t3 [mms2_epd_eis_brst_l2_extof_helium_P6_cps_t3]
      
      
      ---> helium_P6_cps_t4 [mms2_epd_eis_brst_l2_extof_helium_P6_cps_t4]
      
      
      ---> helium_P6_cps_t5 [mms2_epd_eis_brst_l2_extof_helium_P6_cps_t5]
      
      
      MMS2 ExTOF-Burst helium_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_extof_helium_P6_flux_t0]
      
      
      ---> helium_P6_flux_t1 [mms2_epd_eis_brst_l2_extof_helium_P6_flux_t1]
      
      
      ---> helium_P6_flux_t2 [mms2_epd_eis_brst_l2_extof_helium_P6_flux_t2]
      
      
      ---> helium_P6_flux_t3 [mms2_epd_eis_brst_l2_extof_helium_P6_flux_t3]
      
      
      ---> helium_P6_flux_t4 [mms2_epd_eis_brst_l2_extof_helium_P6_flux_t4]
      
      
      ---> helium_P6_flux_t5 [mms2_epd_eis_brst_l2_extof_helium_P6_flux_t5]
      
      
      MMS2 ExTOF-Burst oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_extof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms2_epd_eis_brst_l2_extof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms2_epd_eis_brst_l2_extof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms2_epd_eis_brst_l2_extof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms2_epd_eis_brst_l2_extof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms2_epd_eis_brst_l2_extof_oxygen_P6_counts_t5]
      
      
      MMS2 ExTOF-Burst oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_extof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms2_epd_eis_brst_l2_extof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms2_epd_eis_brst_l2_extof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms2_epd_eis_brst_l2_extof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms2_epd_eis_brst_l2_extof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms2_epd_eis_brst_l2_extof_oxygen_P6_cps_t5]
      
      
      MMS2 ExTOF-Burst oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_extof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms2_epd_eis_brst_l2_extof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms2_epd_eis_brst_l2_extof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms2_epd_eis_brst_l2_extof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms2_epd_eis_brst_l2_extof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms2_epd_eis_brst_l2_extof_oxygen_P6_flux_t5]
      
      
      MMS2 ExTOF-Burst dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_extof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms2_epd_eis_brst_l2_extof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms2_epd_eis_brst_l2_extof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms2_epd_eis_brst_l2_extof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms2_epd_eis_brst_l2_extof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms2_epd_eis_brst_l2_extof_dump_P6_counts_t5]
      
      
      MMS2 ExTOF-Burst dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_extof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms2_epd_eis_brst_l2_extof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms2_epd_eis_brst_l2_extof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms2_epd_eis_brst_l2_extof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms2_epd_eis_brst_l2_extof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms2_epd_eis_brst_l2_extof_dump_P6_cps_t5]
      
      
      MMS2 ExTOF-Burst dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_extof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms2_epd_eis_brst_l2_extof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms2_epd_eis_brst_l2_extof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms2_epd_eis_brst_l2_extof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms2_epd_eis_brst_l2_extof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms2_epd_eis_brst_l2_extof_dump_P6_flux_t5]
      
      
      MMS2 ExTOF-Burst proton_P5_counts_t0 [data available from 2020/09/24 to 2025/01/06] [mms2_epd_eis_brst_l2_extof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms2_epd_eis_brst_l2_extof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms2_epd_eis_brst_l2_extof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms2_epd_eis_brst_l2_extof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms2_epd_eis_brst_l2_extof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms2_epd_eis_brst_l2_extof_proton_P5_counts_t5]
      
      
      MMS2 ExTOF-Burst proton_P5_cps_t0 [data available from 2020/09/24 to 2025/01/06] [mms2_epd_eis_brst_l2_extof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms2_epd_eis_brst_l2_extof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms2_epd_eis_brst_l2_extof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms2_epd_eis_brst_l2_extof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms2_epd_eis_brst_l2_extof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms2_epd_eis_brst_l2_extof_proton_P5_cps_t5]
      
      
      MMS2 ExTOF-Burst proton_P5_flux_t0 [data available from 2020/09/24 to 2025/01/06] [mms2_epd_eis_brst_l2_extof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms2_epd_eis_brst_l2_extof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms2_epd_eis_brst_l2_extof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms2_epd_eis_brst_l2_extof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms2_epd_eis_brst_l2_extof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms2_epd_eis_brst_l2_extof_proton_P5_flux_t5]
      
      
      MMS2 ExTOF-Burst oxygen_P5_counts_t0 [data available from 2020/09/24 to 2025/01/06] [mms2_epd_eis_brst_l2_extof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms2_epd_eis_brst_l2_extof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms2_epd_eis_brst_l2_extof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms2_epd_eis_brst_l2_extof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms2_epd_eis_brst_l2_extof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms2_epd_eis_brst_l2_extof_oxygen_P5_counts_t5]
      
      
      MMS2 ExTOF-Burst oxygen_P5_cps_t0 [data available from 2020/09/24 to 2025/01/06] [mms2_epd_eis_brst_l2_extof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms2_epd_eis_brst_l2_extof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms2_epd_eis_brst_l2_extof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms2_epd_eis_brst_l2_extof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms2_epd_eis_brst_l2_extof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms2_epd_eis_brst_l2_extof_oxygen_P5_cps_t5]
      
      
      MMS2 ExTOF-Burst oxygen_P5_flux_t0 [data available from 2020/09/24 to 2025/01/06] [mms2_epd_eis_brst_l2_extof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms2_epd_eis_brst_l2_extof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms2_epd_eis_brst_l2_extof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms2_epd_eis_brst_l2_extof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms2_epd_eis_brst_l2_extof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms2_epd_eis_brst_l2_extof_oxygen_P5_flux_t5]
      
      
      MMS2 ExTOF-Burst helium_P5_counts_t0 [data available from 2020/09/24 to 2025/01/06] [mms2_epd_eis_brst_l2_extof_helium_P5_counts_t0]
      
      
      ---> helium_P5_counts_t1 [mms2_epd_eis_brst_l2_extof_helium_P5_counts_t1]
      
      
      ---> helium_P5_counts_t2 [mms2_epd_eis_brst_l2_extof_helium_P5_counts_t2]
      
      
      ---> helium_P5_counts_t3 [mms2_epd_eis_brst_l2_extof_helium_P5_counts_t3]
      
      
      ---> helium_P5_counts_t4 [mms2_epd_eis_brst_l2_extof_helium_P5_counts_t4]
      
      
      ---> helium_P5_counts_t5 [mms2_epd_eis_brst_l2_extof_helium_P5_counts_t5]
      
      
      MMS2 ExTOF-Burst helium_P5_cps_t0 [data available from 2020/09/24 to 2025/01/06] [mms2_epd_eis_brst_l2_extof_helium_P5_cps_t0]
      
      
      ---> helium_P5_cps_t1 [mms2_epd_eis_brst_l2_extof_helium_P5_cps_t1]
      
      
      ---> helium_P5_cps_t2 [mms2_epd_eis_brst_l2_extof_helium_P5_cps_t2]
      
      
      ---> helium_P5_cps_t3 [mms2_epd_eis_brst_l2_extof_helium_P5_cps_t3]
      
      
      ---> helium_P5_cps_t4 [mms2_epd_eis_brst_l2_extof_helium_P5_cps_t4]
      
      
      ---> helium_P5_cps_t5 [mms2_epd_eis_brst_l2_extof_helium_P5_cps_t5]
      
      
      MMS2 ExTOF-Burst helium_P5_flux_t0 [data available from 2020/09/24 to 2025/01/06] [mms2_epd_eis_brst_l2_extof_helium_P5_flux_t0]
      
      
      ---> helium_P5_flux_t1 [mms2_epd_eis_brst_l2_extof_helium_P5_flux_t1]
      
      
      ---> helium_P5_flux_t2 [mms2_epd_eis_brst_l2_extof_helium_P5_flux_t2]
      
      
      ---> helium_P5_flux_t3 [mms2_epd_eis_brst_l2_extof_helium_P5_flux_t3]
      
      
      ---> helium_P5_flux_t4 [mms2_epd_eis_brst_l2_extof_helium_P5_flux_t4]
      
      
      ---> helium_P5_flux_t5 [mms2_epd_eis_brst_l2_extof_helium_P5_flux_t5]
      
      
      MMS2 ExTOF-Burst proton_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_extof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms2_epd_eis_brst_l2_extof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms2_epd_eis_brst_l2_extof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms2_epd_eis_brst_l2_extof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms2_epd_eis_brst_l2_extof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms2_epd_eis_brst_l2_extof_proton_P4_counts_t5]
      
      
      MMS2 ExTOF-Burst proton_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_extof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms2_epd_eis_brst_l2_extof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms2_epd_eis_brst_l2_extof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms2_epd_eis_brst_l2_extof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms2_epd_eis_brst_l2_extof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms2_epd_eis_brst_l2_extof_proton_P4_cps_t5]
      
      
      MMS2 ExTOF-Burst proton_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_extof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms2_epd_eis_brst_l2_extof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms2_epd_eis_brst_l2_extof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms2_epd_eis_brst_l2_extof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms2_epd_eis_brst_l2_extof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms2_epd_eis_brst_l2_extof_proton_P4_flux_t5]
      
      
      MMS2 ExTOF-Burst alpha_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_extof_helium_P4_counts_t0]
      
      
      ---> alpha_P4_counts_t1 [mms2_epd_eis_brst_l2_extof_helium_P4_counts_t1]
      
      
      ---> alpha_P4_counts_t2 [mms2_epd_eis_brst_l2_extof_helium_P4_counts_t2]
      
      
      ---> alpha_P4_counts_t3 [mms2_epd_eis_brst_l2_extof_helium_P4_counts_t3]
      
      
      ---> alpha_P4_counts_t4 [mms2_epd_eis_brst_l2_extof_helium_P4_counts_t4]
      
      
      ---> alpha_P4_counts_t5 [mms2_epd_eis_brst_l2_extof_helium_P4_counts_t5]
      
      
      MMS2 ExTOF-Burst alpha_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_extof_helium_P4_cps_t0]
      
      
      ---> alpha_P4_cps_t1 [mms2_epd_eis_brst_l2_extof_helium_P4_cps_t1]
      
      
      ---> alpha_P4_cps_t2 [mms2_epd_eis_brst_l2_extof_helium_P4_cps_t2]
      
      
      ---> alpha_P4_cps_t3 [mms2_epd_eis_brst_l2_extof_helium_P4_cps_t3]
      
      
      ---> alpha_P4_cps_t4 [mms2_epd_eis_brst_l2_extof_helium_P4_cps_t4]
      
      
      ---> alpha_P4_cps_t5 [mms2_epd_eis_brst_l2_extof_helium_P4_cps_t5]
      
      
      MMS2 ExTOF-Burst alpha_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_extof_helium_P4_flux_t0]
      
      
      ---> alpha_P4_flux_t1 [mms2_epd_eis_brst_l2_extof_helium_P4_flux_t1]
      
      
      ---> alpha_P4_flux_t2 [mms2_epd_eis_brst_l2_extof_helium_P4_flux_t2]
      
      
      ---> alpha_P4_flux_t3 [mms2_epd_eis_brst_l2_extof_helium_P4_flux_t3]
      
      
      ---> alpha_P4_flux_t4 [mms2_epd_eis_brst_l2_extof_helium_P4_flux_t4]
      
      
      ---> alpha_P4_flux_t5 [mms2_epd_eis_brst_l2_extof_helium_P4_flux_t5]
      
      
      MMS2 ExTOF-Burst oxygen_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_extof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms2_epd_eis_brst_l2_extof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms2_epd_eis_brst_l2_extof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms2_epd_eis_brst_l2_extof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms2_epd_eis_brst_l2_extof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms2_epd_eis_brst_l2_extof_oxygen_P4_counts_t5]
      
      
      MMS2 ExTOF-Burst oxygen_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_extof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms2_epd_eis_brst_l2_extof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms2_epd_eis_brst_l2_extof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms2_epd_eis_brst_l2_extof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms2_epd_eis_brst_l2_extof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms2_epd_eis_brst_l2_extof_oxygen_P4_cps_t5]
      
      
      MMS2 ExTOF-Burst oxygen_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_extof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms2_epd_eis_brst_l2_extof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms2_epd_eis_brst_l2_extof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms2_epd_eis_brst_l2_extof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms2_epd_eis_brst_l2_extof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms2_epd_eis_brst_l2_extof_oxygen_P4_flux_t5]
      
      
      MMS2 ExTOF-Burst proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_extof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms2_epd_eis_brst_l2_extof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms2_epd_eis_brst_l2_extof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms2_epd_eis_brst_l2_extof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms2_epd_eis_brst_l2_extof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms2_epd_eis_brst_l2_extof_proton_P3_counts_t5]
      
      
      MMS2 ExTOF-Burst proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_extof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms2_epd_eis_brst_l2_extof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms2_epd_eis_brst_l2_extof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms2_epd_eis_brst_l2_extof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms2_epd_eis_brst_l2_extof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms2_epd_eis_brst_l2_extof_proton_P3_cps_t5]
      
      
      MMS2 ExTOF-Burst proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_extof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms2_epd_eis_brst_l2_extof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms2_epd_eis_brst_l2_extof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms2_epd_eis_brst_l2_extof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms2_epd_eis_brst_l2_extof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms2_epd_eis_brst_l2_extof_proton_P3_flux_t5]
      
      
      MMS2 ExTOF-Burst alpha_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_extof_helium_P3_counts_t0]
      
      
      ---> alpha_P3_counts_t1 [mms2_epd_eis_brst_l2_extof_helium_P3_counts_t1]
      
      
      ---> alpha_P3_counts_t2 [mms2_epd_eis_brst_l2_extof_helium_P3_counts_t2]
      
      
      ---> alpha_P3_counts_t3 [mms2_epd_eis_brst_l2_extof_helium_P3_counts_t3]
      
      
      ---> alpha_P3_counts_t4 [mms2_epd_eis_brst_l2_extof_helium_P3_counts_t4]
      
      
      ---> alpha_P3_counts_t5 [mms2_epd_eis_brst_l2_extof_helium_P3_counts_t5]
      
      
      MMS2 ExTOF-Burst alpha_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_extof_helium_P3_cps_t0]
      
      
      ---> alpha_P3_cps_t1 [mms2_epd_eis_brst_l2_extof_helium_P3_cps_t1]
      
      
      ---> alpha_P3_cps_t2 [mms2_epd_eis_brst_l2_extof_helium_P3_cps_t2]
      
      
      ---> alpha_P3_cps_t3 [mms2_epd_eis_brst_l2_extof_helium_P3_cps_t3]
      
      
      ---> alpha_P3_cps_t4 [mms2_epd_eis_brst_l2_extof_helium_P3_cps_t4]
      
      
      ---> alpha_P3_cps_t5 [mms2_epd_eis_brst_l2_extof_helium_P3_cps_t5]
      
      
      MMS2 ExTOF-Burst alpha_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_extof_helium_P3_flux_t0]
      
      
      ---> alpha_P3_flux_t1 [mms2_epd_eis_brst_l2_extof_helium_P3_flux_t1]
      
      
      ---> alpha_P3_flux_t2 [mms2_epd_eis_brst_l2_extof_helium_P3_flux_t2]
      
      
      ---> alpha_P3_flux_t3 [mms2_epd_eis_brst_l2_extof_helium_P3_flux_t3]
      
      
      ---> alpha_P3_flux_t4 [mms2_epd_eis_brst_l2_extof_helium_P3_flux_t4]
      
      
      ---> alpha_P3_flux_t5 [mms2_epd_eis_brst_l2_extof_helium_P3_flux_t5]
      
      
      MMS2 ExTOF-Burst oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_extof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms2_epd_eis_brst_l2_extof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms2_epd_eis_brst_l2_extof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms2_epd_eis_brst_l2_extof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms2_epd_eis_brst_l2_extof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms2_epd_eis_brst_l2_extof_oxygen_P3_counts_t5]
      
      
      MMS2 ExTOF-Burst oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_extof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t2 [mms2_epd_eis_brst_l2_extof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms2_epd_eis_brst_l2_extof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms2_epd_eis_brst_l2_extof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms2_epd_eis_brst_l2_extof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms2_epd_eis_brst_l2_extof_oxygen_P3_cps_t5]
      
      
      MMS2 ExTOF-Burst oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_extof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms2_epd_eis_brst_l2_extof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms2_epd_eis_brst_l2_extof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms2_epd_eis_brst_l2_extof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms2_epd_eis_brst_l2_extof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms2_epd_eis_brst_l2_extof_oxygen_P3_flux_t5]
      
      
      MMS2 ExTOF-Burst dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_extof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms2_epd_eis_brst_l2_extof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms2_epd_eis_brst_l2_extof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms2_epd_eis_brst_l2_extof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms2_epd_eis_brst_l2_extof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms2_epd_eis_brst_l2_extof_dump_P3_counts_t5]
      
      
      MMS2 ExTOF-Burst dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_extof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms2_epd_eis_brst_l2_extof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms2_epd_eis_brst_l2_extof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms2_epd_eis_brst_l2_extof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms2_epd_eis_brst_l2_extof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms2_epd_eis_brst_l2_extof_dump_P4_counts_t5]
      
      
      MMS2 ExTOF-Burst dump_P5_counts_t0 [data available from 2020/09/24 to 2025/01/06] [mms2_epd_eis_brst_l2_extof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms2_epd_eis_brst_l2_extof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms2_epd_eis_brst_l2_extof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms2_epd_eis_brst_l2_extof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms2_epd_eis_brst_l2_extof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms2_epd_eis_brst_l2_extof_dump_P5_counts_t5]
      
      
      MMS2 ExTOF-Burst dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_extof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms2_epd_eis_brst_l2_extof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms2_epd_eis_brst_l2_extof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms2_epd_eis_brst_l2_extof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms2_epd_eis_brst_l2_extof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms2_epd_eis_brst_l2_extof_dump_P3_cps_t5]
      
      
      MMS2 ExTOF-Burst dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_extof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms2_epd_eis_brst_l2_extof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms2_epd_eis_brst_l2_extof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms2_epd_eis_brst_l2_extof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms2_epd_eis_brst_l2_extof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms2_epd_eis_brst_l2_extof_dump_P4_cps_t5]
      
      
      MMS2 ExTOF-Burst dump_P5_cps_t0 [data available from 2020/09/24 to 2025/01/06] [mms2_epd_eis_brst_l2_extof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms2_epd_eis_brst_l2_extof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms2_epd_eis_brst_l2_extof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms2_epd_eis_brst_l2_extof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms2_epd_eis_brst_l2_extof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms2_epd_eis_brst_l2_extof_dump_P5_cps_t5]
      
      
      MMS2 ExTOF-Burst dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_extof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms2_epd_eis_brst_l2_extof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms2_epd_eis_brst_l2_extof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms2_epd_eis_brst_l2_extof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms2_epd_eis_brst_l2_extof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms2_epd_eis_brst_l2_extof_dump_P3_flux_t5]
      
      
      MMS2 ExTOF-Burst dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_extof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms2_epd_eis_brst_l2_extof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms2_epd_eis_brst_l2_extof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms2_epd_eis_brst_l2_extof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms2_epd_eis_brst_l2_extof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms2_epd_eis_brst_l2_extof_dump_P4_flux_t5]
      
      
      MMS2 ExTOF-Burst dump_P5_flux_t0 [data available from 2020/09/24 to 2025/01/06] [mms2_epd_eis_brst_l2_extof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms2_epd_eis_brst_l2_extof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms2_epd_eis_brst_l2_extof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms2_epd_eis_brst_l2_extof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms2_epd_eis_brst_l2_extof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms2_epd_eis_brst_l2_extof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS2 [mms2_epd_eis_brst_l2_extof_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS2 [mms2_epd_eis_brst_l2_extof_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS2 [mms2_epd_eis_brst_l2_extof_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS2 [mms2_epd_eis_brst_l2_extof_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS2 [mms2_epd_eis_brst_l2_extof_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS2 [mms2_epd_eis_brst_l2_extof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS2 [mms2_epd_eis_brst_l2_extof_look_t0]
      
      
      Look Direction for Telescope 1 MMS2 [mms2_epd_eis_brst_l2_extof_look_t1]
      
      
      Look Direction for Telescope 2 MMS2 [mms2_epd_eis_brst_l2_extof_look_t2]
      
      
      Look Direction for Telescope 3 MMS2 [mms2_epd_eis_brst_l2_extof_look_t3]
      
      
      Look Direction for Telescope 4 MMS2 [mms2_epd_eis_brst_l2_extof_look_t4]
      
      
      Look Direction for Telescope 5 MMS2 [mms2_epd_eis_brst_l2_extof_look_t5]
      
      
      Magnetic Field BCS MMS2 [mms2_epd_eis_brst_l2_extof_b]
      
      
      Spacecraft position GSE MMS2 [mms2_epd_eis_brst_l2_extof_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS2 [mms2_epd_eis_brst_l2_extof_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS2 [mms2_epd_eis_brst_l2_extof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS2 [mms2_epd_eis_brst_l2_extof_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS2 [mms2_epd_eis_brst_l2_extof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS2 [mms2_epd_eis_brst_l2_extof_r]
      
      
      Dipole L-shell MMS2 [mms2_epd_eis_brst_l2_extof_l]
      
      
      Latitude in GSE Frame MMS2 [mms2_epd_eis_brst_l2_extof_gse_lat]
      
      
      Longitude in GSE Frame MMS2 [mms2_epd_eis_brst_l2_extof_gse_lon]
      
      
      Latitude in GSM Frame MMS2 [mms2_epd_eis_brst_l2_extof_gsm_lat]
      
      
      Longitude in GSM Frame MMS2 [mms2_epd_eis_brst_l2_extof_gsm_lon]
      
      
      Latitude in SM Frame MMS2 [mms2_epd_eis_brst_l2_extof_sm_lat]
      
      
      Longitude in SM Frame MMS2 [mms2_epd_eis_brst_l2_extof_sm_lon]
      
      
      Orbit number MMS2 [mms2_epd_eis_brst_l2_extof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS2 [mms2_epd_eis_brst_l2_extof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS2 [mms2_epd_eis_brst_l2_extof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS2 [mms2_epd_eis_brst_l2_extof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS2 [mms2_epd_eis_brst_l2_extof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS2 [mms2_epd_eis_brst_l2_extof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS2 [mms2_epd_eis_brst_l2_extof_ssd5]
      
      
      Valid Events Processed per second MMS2 [mms2_epd_eis_brst_l2_extof_vep]
      
      
      Start 0 Anode Count Rate MMS2 [mms2_epd_eis_brst_l2_extof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS2 [mms2_epd_eis_brst_l2_extof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS2 [mms2_epd_eis_brst_l2_extof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS2 [mms2_epd_eis_brst_l2_extof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS2 [mms2_epd_eis_brst_l2_extof_vtofxphe]
      
      
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MMS2_EPD-EIS_BRST_L2_PHXTOF (spase://NASA/NumericalData/MMS/2/EnergeticParticleDetector/EIS/Burst/Level2/PulseHeightByTimeOfFlight/PT0.605S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms2_epd_eis_brst_l2_phxtof_duration]
      
      
      ---> Instrument Deadtime [mms2_epd_eis_brst_l2_phxtof_deadtime]
      
      
      ---> Instrument Large Pixel in Use [mms2_epd_eis_brst_l2_phxtof_largepixel]
      
      
      ---> Spin [mms2_epd_eis_brst_l2_phxtof_spin]
      
      
      ---> Sector [mms2_epd_eis_brst_l2_phxtof_sector]
      
      
      ---> Quality Word [mms2_epd_eis_brst_l2_phxtof_quality]
      
      
      MMS2 PhxTOF-Burst proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms2_epd_eis_brst_l2_phxtof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms2_epd_eis_brst_l2_phxtof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms2_epd_eis_brst_l2_phxtof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms2_epd_eis_brst_l2_phxtof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms2_epd_eis_brst_l2_phxtof_proton_P6_counts_t5]
      
      
      MMS2 PhxTOF-Burst proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms2_epd_eis_brst_l2_phxtof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms2_epd_eis_brst_l2_phxtof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms2_epd_eis_brst_l2_phxtof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms2_epd_eis_brst_l2_phxtof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms2_epd_eis_brst_l2_phxtof_proton_P6_cps_t5]
      
      
      MMS2 PhxTOF-Burst proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms2_epd_eis_brst_l2_phxtof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms2_epd_eis_brst_l2_phxtof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms2_epd_eis_brst_l2_phxtof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms2_epd_eis_brst_l2_phxtof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms2_epd_eis_brst_l2_phxtof_proton_P6_flux_t5]
      
      
      MMS2 PhxTOF-Burst oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t5]
      
      
      MMS2 PhxTOF-Burst oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t5]
      
      
      MMS2 PhxTOF-Burst oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms2_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t5]
      
      
      MMS2 PhxTOF-Burst dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms2_epd_eis_brst_l2_phxtof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms2_epd_eis_brst_l2_phxtof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms2_epd_eis_brst_l2_phxtof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms2_epd_eis_brst_l2_phxtof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms2_epd_eis_brst_l2_phxtof_dump_P6_counts_t5]
      
      
      MMS2 PhxTOF-Burst dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms2_epd_eis_brst_l2_phxtof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms2_epd_eis_brst_l2_phxtof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms2_epd_eis_brst_l2_phxtof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms2_epd_eis_brst_l2_phxtof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms2_epd_eis_brst_l2_phxtof_dump_P6_cps_t5]
      
      
      MMS2 PhxTOF-Burst dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms2_epd_eis_brst_l2_phxtof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms2_epd_eis_brst_l2_phxtof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms2_epd_eis_brst_l2_phxtof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms2_epd_eis_brst_l2_phxtof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms2_epd_eis_brst_l2_phxtof_dump_P6_flux_t5]
      
      
      MMS2 PhxTOF-Burst proton_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms2_epd_eis_brst_l2_phxtof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms2_epd_eis_brst_l2_phxtof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms2_epd_eis_brst_l2_phxtof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms2_epd_eis_brst_l2_phxtof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms2_epd_eis_brst_l2_phxtof_proton_P5_counts_t5]
      
      
      MMS2 PhxTOF-Burst proton_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms2_epd_eis_brst_l2_phxtof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms2_epd_eis_brst_l2_phxtof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms2_epd_eis_brst_l2_phxtof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms2_epd_eis_brst_l2_phxtof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms2_epd_eis_brst_l2_phxtof_proton_P5_cps_t5]
      
      
      MMS2 PhxTOF-Burst proton_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms2_epd_eis_brst_l2_phxtof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms2_epd_eis_brst_l2_phxtof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms2_epd_eis_brst_l2_phxtof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms2_epd_eis_brst_l2_phxtof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms2_epd_eis_brst_l2_phxtof_proton_P5_flux_t5]
      
      
      MMS2 PhxTOF-Burst oxygen_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t5]
      
      
      MMS2 PhxTOF-Burst oxygen_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t5]
      
      
      MMS2 PhxTOF-Burst oxygen_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms2_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t5]
      
      
      MMS2 PhxTOF-Burst proton_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_phxtof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms2_epd_eis_brst_l2_phxtof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms2_epd_eis_brst_l2_phxtof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms2_epd_eis_brst_l2_phxtof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms2_epd_eis_brst_l2_phxtof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms2_epd_eis_brst_l2_phxtof_proton_P4_counts_t5]
      
      
      MMS2 PhxTOF-Burst proton_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_phxtof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms2_epd_eis_brst_l2_phxtof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms2_epd_eis_brst_l2_phxtof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms2_epd_eis_brst_l2_phxtof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms2_epd_eis_brst_l2_phxtof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms2_epd_eis_brst_l2_phxtof_proton_P4_cps_t5]
      
      
      MMS2 PhxTOF-Burst proton_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_phxtof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms2_epd_eis_brst_l2_phxtof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms2_epd_eis_brst_l2_phxtof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms2_epd_eis_brst_l2_phxtof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms2_epd_eis_brst_l2_phxtof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms2_epd_eis_brst_l2_phxtof_proton_P4_flux_t5]
      
      
      MMS2 PhxTOF-Burst oxygen_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t5]
      
      
      MMS2 PhxTOF-Burst oxygen_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t5]
      
      
      MMS2 PhxTOF-Burst oxygen_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms2_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t5]
      
      
      MMS2 PhxTOF-Burst proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_phxtof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms2_epd_eis_brst_l2_phxtof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms2_epd_eis_brst_l2_phxtof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms2_epd_eis_brst_l2_phxtof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms2_epd_eis_brst_l2_phxtof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms2_epd_eis_brst_l2_phxtof_proton_P3_counts_t5]
      
      
      MMS2 PhxTOF-Burst proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_phxtof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms2_epd_eis_brst_l2_phxtof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms2_epd_eis_brst_l2_phxtof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms2_epd_eis_brst_l2_phxtof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms2_epd_eis_brst_l2_phxtof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms2_epd_eis_brst_l2_phxtof_proton_P3_cps_t5]
      
      
      MMS2 PhxTOF-Burst proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_phxtof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms2_epd_eis_brst_l2_phxtof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms2_epd_eis_brst_l2_phxtof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms2_epd_eis_brst_l2_phxtof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms2_epd_eis_brst_l2_phxtof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms2_epd_eis_brst_l2_phxtof_proton_P3_flux_t5]
      
      
      MMS2 PhxTOF-Burst oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t5]
      
      
      MMS2 PhxTOF-Burst oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t5]
      
      
      MMS2 PhxTOF-Burst oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms2_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t5]
      
      
      MMS2 PhxTOF-Burst dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_phxtof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms2_epd_eis_brst_l2_phxtof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms2_epd_eis_brst_l2_phxtof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms2_epd_eis_brst_l2_phxtof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms2_epd_eis_brst_l2_phxtof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms2_epd_eis_brst_l2_phxtof_dump_P3_counts_t5]
      
      
      MMS2 PhxTOF-Burst dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_phxtof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms2_epd_eis_brst_l2_phxtof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms2_epd_eis_brst_l2_phxtof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms2_epd_eis_brst_l2_phxtof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms2_epd_eis_brst_l2_phxtof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms2_epd_eis_brst_l2_phxtof_dump_P4_counts_t5]
      
      
      MMS2 PhxTOF-Burst dump_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms2_epd_eis_brst_l2_phxtof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms2_epd_eis_brst_l2_phxtof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms2_epd_eis_brst_l2_phxtof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms2_epd_eis_brst_l2_phxtof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms2_epd_eis_brst_l2_phxtof_dump_P5_counts_t5]
      
      
      MMS2 PhxTOF-Burst dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_phxtof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms2_epd_eis_brst_l2_phxtof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms2_epd_eis_brst_l2_phxtof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms2_epd_eis_brst_l2_phxtof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms2_epd_eis_brst_l2_phxtof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms2_epd_eis_brst_l2_phxtof_dump_P3_cps_t5]
      
      
      MMS2 PhxTOF-Burst dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_phxtof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms2_epd_eis_brst_l2_phxtof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms2_epd_eis_brst_l2_phxtof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms2_epd_eis_brst_l2_phxtof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms2_epd_eis_brst_l2_phxtof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms2_epd_eis_brst_l2_phxtof_dump_P4_cps_t5]
      
      
      MMS2 PhxTOF-Burst dump_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms2_epd_eis_brst_l2_phxtof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms2_epd_eis_brst_l2_phxtof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms2_epd_eis_brst_l2_phxtof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms2_epd_eis_brst_l2_phxtof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms2_epd_eis_brst_l2_phxtof_dump_P5_cps_t5]
      
      
      MMS2 PhxTOF-Burst dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_brst_l2_phxtof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms2_epd_eis_brst_l2_phxtof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms2_epd_eis_brst_l2_phxtof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms2_epd_eis_brst_l2_phxtof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms2_epd_eis_brst_l2_phxtof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms2_epd_eis_brst_l2_phxtof_dump_P3_flux_t5]
      
      
      MMS2 PhxTOF-Burst dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_brst_l2_phxtof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms2_epd_eis_brst_l2_phxtof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms2_epd_eis_brst_l2_phxtof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms2_epd_eis_brst_l2_phxtof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms2_epd_eis_brst_l2_phxtof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms2_epd_eis_brst_l2_phxtof_dump_P4_flux_t5]
      
      
      MMS2 PhxTOF-Burst dump_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_brst_l2_phxtof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms2_epd_eis_brst_l2_phxtof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms2_epd_eis_brst_l2_phxtof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms2_epd_eis_brst_l2_phxtof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms2_epd_eis_brst_l2_phxtof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms2_epd_eis_brst_l2_phxtof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS2 [mms2_epd_eis_brst_l2_phxtof_pitch_angle_t0]
      
      
      ---> Pitch Angle for Telescope 1 MMS2 [mms2_epd_eis_brst_l2_phxtof_pitch_angle_t1]
      
      
      ---> Pitch Angle for Telescope 2 MMS2 [mms2_epd_eis_brst_l2_phxtof_pitch_angle_t2]
      
      
      ---> Pitch Angle for Telescope 3 MMS2 [mms2_epd_eis_brst_l2_phxtof_pitch_angle_t3]
      
      
      ---> Pitch Angle for Telescope 4 MMS2 [mms2_epd_eis_brst_l2_phxtof_pitch_angle_t4]
      
      
      ---> Pitch Angle for Telescope 5 MMS2 [mms2_epd_eis_brst_l2_phxtof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS2 [mms2_epd_eis_brst_l2_phxtof_look_t0]
      
      
      ---> Look Direction for Telescope 1 MMS2 [mms2_epd_eis_brst_l2_phxtof_look_t1]
      
      
      ---> Look Direction for Telescope 2 MMS2 [mms2_epd_eis_brst_l2_phxtof_look_t2]
      
      
      ---> Look Direction for Telescope 3 MMS2 [mms2_epd_eis_brst_l2_phxtof_look_t3]
      
      
      ---> Look Direction for Telescope 4 MMS2 [mms2_epd_eis_brst_l2_phxtof_look_t4]
      
      
      ---> Look Direction for Telescope 5 MMS2 [mms2_epd_eis_brst_l2_phxtof_look_t5]
      
      
      Magnetic Field BCS MMS2 [mms2_epd_eis_brst_l2_phxtof_b]
      
      
      Spacecraft position GSE MMS2 [mms2_epd_eis_brst_l2_phxtof_position_gse]
      
      
      ---> Spacecraft position in GSM coordinates MMS2 [mms2_epd_eis_brst_l2_phxtof_position_gsm]
      
      
      ---> Spacecraft-Moon vector in GSE coordinates MMS2 [mms2_epd_eis_brst_l2_phxtof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS2 [mms2_epd_eis_brst_l2_phxtof_sc_to_gse]
      
      
      ---> Transformation Matrix GSE to GSM Frame MMS2 [mms2_epd_eis_brst_l2_phxtof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS2 [mms2_epd_eis_brst_l2_phxtof_r]
      
      
      Dipole L-shell MMS2 [mms2_epd_eis_brst_l2_phxtof_l]
      
      
      Latitude in GSE Frame MMS2 [mms2_epd_eis_brst_l2_phxtof_gse_lat]
      
      
      Longitude in GSE Frame MMS2 [mms2_epd_eis_brst_l2_phxtof_gse_lon]
      
      
      Latitude in GSM Frame MMS2 [mms2_epd_eis_brst_l2_phxtof_gsm_lat]
      
      
      Longitude in GSM Frame MMS2 [mms2_epd_eis_brst_l2_phxtof_gsm_lon]
      
      
      Latitude in SM Frame MMS2 [mms2_epd_eis_brst_l2_phxtof_sm_lat]
      
      
      Longitude in SM Frame MMS2 [mms2_epd_eis_brst_l2_phxtof_sm_lon]
      
      
      Orbit number MMS2 [mms2_epd_eis_brst_l2_phxtof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS2 [mms2_epd_eis_brst_l2_phxtof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS2 [mms2_epd_eis_brst_l2_phxtof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS2 [mms2_epd_eis_brst_l2_phxtof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS2 [mms2_epd_eis_brst_l2_phxtof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS2 [mms2_epd_eis_brst_l2_phxtof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS2 [mms2_epd_eis_brst_l2_phxtof_ssd5]
      
      
      Valid Events Processed per second MMS2 [mms2_epd_eis_brst_l2_phxtof_vep]
      
      
      Start 0 Anode Count Rate MMS2 [mms2_epd_eis_brst_l2_phxtof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS2 [mms2_epd_eis_brst_l2_phxtof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS2 [mms2_epd_eis_brst_l2_phxtof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS2 [mms2_epd_eis_brst_l2_phxtof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS2 [mms2_epd_eis_brst_l2_phxtof_vtofxphe]
      
      
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MMS2_EPD-EIS_SRVY_L2_ELECTRONENERGY (spase://NASA/NumericalData/MMS/2/EnergeticParticleDetector/EIS/Survey/Level2/ElectronEnergySpectra/PT2.42S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms2_epd_eis_srvy_l2_electronenergy_duration]
      
      
      Instrument Deadtime [mms2_epd_eis_srvy_l2_electronenergy_deadtime]
      
      
      Instrument Large Pixel in Use [mms2_epd_eis_srvy_l2_electronenergy_largepixel]
      
      
      Spin [mms2_epd_eis_srvy_l2_electronenergy_spin]
      
      
      Sector [mms2_epd_eis_srvy_l2_electronenergy_sector]
      
      
      Quality Word [mms2_epd_eis_srvy_l2_electronenergy_quality]
      
      
      MMS2 ElectronEnergy-Survey electron_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t0]
      
      
      ---> electron_P6_counts_t1 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t1]
      
      
      ---> electron_P6_counts_t2 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t2]
      
      
      ---> electron_P6_counts_t3 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t3]
      
      
      ---> electron_P6_counts_t4 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t4]
      
      
      ---> electron_P6_counts_t5 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t5]
      
      
      MMS2 ElectronEnergy-Survey electron_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t0]
      
      
      ---> electron_P6_cps_t1 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t1]
      
      
      ---> electron_P6_cps_t2 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t2]
      
      
      ---> electron_P6_cps_t3 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t3]
      
      
      ---> electron_P6_cps_t4 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t4]
      
      
      ---> electron_P6_cps_t5 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t5]
      
      
      MMS2 ElectronEnergy-Survey electron_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t0]
      
      
      ---> electron_P6_flux_t1 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t1]
      
      
      ---> electron_P6_flux_t2 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t2]
      
      
      ---> electron_P6_flux_t3 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t3]
      
      
      ---> electron_P6_flux_t4 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t4]
      
      
      ---> electron_P6_flux_t5 [mms2_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t5]
      
      
      MMS2 ElectronEnergy-Survey dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t5]
      
      
      MMS2 ElectronEnergy-Survey dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t5]
      
      
      MMS2 ElectronEnergy-Survey dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms2_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t5]
      
      
      MMS2 ElectronEnergy-Survey electron_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t0]
      
      
      ---> electron_P5_counts_t1 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t1]
      
      
      ---> electron_P5_counts_t2 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t2]
      
      
      ---> electron_P5_counts_t3 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t3]
      
      
      ---> electron_P5_counts_t4 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t4]
      
      
      ---> electron_P5_counts_t5 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t5]
      
      
      MMS2 ElectronEnergy-Survey electron_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t0]
      
      
      ---> electron_P5_cps_t1 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t1]
      
      
      ---> electron_P5_cps_t2 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t2]
      
      
      ---> electron_P5_cps_t3 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t3]
      
      
      ---> electron_P5_cps_t4 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t4]
      
      
      ---> electron_P5_cps_t5 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t5]
      
      
      MMS2 ElectronEnergy-Survey electron_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t0]
      
      
      ---> electron_P5_flux_t1 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t1]
      
      
      ---> electron_P5_flux_t2 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t2]
      
      
      ---> electron_P5_flux_t3 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t3]
      
      
      ---> electron_P5_flux_t4 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t4]
      
      
      ---> electron_P5_flux_t5 [mms2_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t5]
      
      
      MMS2 ElectronEnergy-Survey electron_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t0]
      
      
      ---> electron_P4_counts_t1 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t1]
      
      
      ---> electron_P4_counts_t2 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t2]
      
      
      ---> electron_P4_counts_t3 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t3]
      
      
      ---> electron_P4_counts_t4 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t4]
      
      
      ---> electron_P4_counts_t5 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t5]
      
      
      MMS2 ElectronEnergy-Survey electron_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t0]
      
      
      ---> electron_P4_cps_t1 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t1]
      
      
      ---> electron_P4_cps_t2 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t2]
      
      
      ---> electron_P4_cps_t3 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t3]
      
      
      ---> electron_P4_cps_t4 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t4]
      
      
      ---> electron_P4_cps_t5 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t5]
      
      
      MMS2 ElectronEnergy-Survey electron_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t0]
      
      
      ---> electron_P4_flux_t1 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t1]
      
      
      ---> electron_P4_flux_t2 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t2]
      
      
      ---> electron_P4_flux_t3 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t3]
      
      
      ---> electron_P4_flux_t4 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t4]
      
      
      ---> electron_P4_flux_t5 [mms2_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t5]
      
      
      MMS2 ElectronEnergy-Survey electron_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t0]
      
      
      ---> electron_P3_counts_t1 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t1]
      
      
      ---> electron_P3_counts_t2 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t2]
      
      
      ---> electron_P3_counts_t3 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t3]
      
      
      ---> electron_P3_counts_t4 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t4]
      
      
      ---> electron_P3_counts_t5 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t5]
      
      
      MMS2 ElectronEnergy-Survey electron_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t0]
      
      
      ---> electron_P3_cps_t1 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t1]
      
      
      ---> electron_P3_cps_t2 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t2]
      
      
      ---> electron_P3_cps_t3 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t3]
      
      
      ---> electron_P3_cps_t4 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t4]
      
      
      ---> electron_P3_cps_t5 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t5]
      
      
      MMS2 ElectronEnergy-Survey electron_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t0]
      
      
      ---> electron_P3_flux_t1 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t1]
      
      
      ---> electron_P3_flux_t2 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t2]
      
      
      ---> electron_P3_flux_t3 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t3]
      
      
      ---> electron_P3_flux_t4 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t4]
      
      
      ---> electron_P3_flux_t5 [mms2_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t5]
      
      
      MMS2 ElectronEnergy-Survey dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t5]
      
      
      MMS2 ElectronEnergy-Survey dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t5]
      
      
      MMS2 ElectronEnergy-Survey dump_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t5]
      
      
      MMS2 ElectronEnergy-Survey dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t5]
      
      
      MMS2 ElectronEnergy-Survey dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t5]
      
      
      MMS2 ElectronEnergy-Survey dump_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t5]
      
      
      MMS2 ElectronEnergy-Survey dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms2_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t5]
      
      
      MMS2 ElectronEnergy-Survey dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms2_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t5]
      
      
      MMS2 ElectronEnergy-Survey dump_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms2_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS2 [mms2_epd_eis_srvy_l2_electronenergy_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS2 [mms2_epd_eis_srvy_l2_electronenergy_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS2 [mms2_epd_eis_srvy_l2_electronenergy_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS2 [mms2_epd_eis_srvy_l2_electronenergy_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS2 [mms2_epd_eis_srvy_l2_electronenergy_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS2 [mms2_epd_eis_srvy_l2_electronenergy_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS2 [mms2_epd_eis_srvy_l2_electronenergy_look_t0]
      
      
      Look Direction for Telescope 1 MMS2 [mms2_epd_eis_srvy_l2_electronenergy_look_t1]
      
      
      Look Direction for Telescope 2 MMS2 [mms2_epd_eis_srvy_l2_electronenergy_look_t2]
      
      
      Look Direction for Telescope 3 MMS2 [mms2_epd_eis_srvy_l2_electronenergy_look_t3]
      
      
      Look Direction for Telescope 4 MMS2 [mms2_epd_eis_srvy_l2_electronenergy_look_t4]
      
      
      Look Direction for Telescope 5 MMS2 [mms2_epd_eis_srvy_l2_electronenergy_look_t5]
      
      
      Magnetic Field BCS MMS2 [mms2_epd_eis_srvy_l2_electronenergy_b]
      
      
      Spacecraft position GSE MMS2 [mms2_epd_eis_srvy_l2_electronenergy_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS2 [mms2_epd_eis_srvy_l2_electronenergy_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS2 [mms2_epd_eis_srvy_l2_electronenergy_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS2 [mms2_epd_eis_srvy_l2_electronenergy_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS2 [mms2_epd_eis_srvy_l2_electronenergy_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS2 [mms2_epd_eis_srvy_l2_electronenergy_r]
      
      
      Dipole L-shell MMS2 [mms2_epd_eis_srvy_l2_electronenergy_l]
      
      
      Latitude in GSE Frame MMS2 [mms2_epd_eis_srvy_l2_electronenergy_gse_lat]
      
      
      Longitude in GSE Frame MMS2 [mms2_epd_eis_srvy_l2_electronenergy_gse_lon]
      
      
      Latitude in GSM Frame MMS2 [mms2_epd_eis_srvy_l2_electronenergy_gsm_lat]
      
      
      Longitude in GSM Frame MMS2 [mms2_epd_eis_srvy_l2_electronenergy_gsm_lon]
      
      
      Latitude in SM Frame MMS2 [mms2_epd_eis_srvy_l2_electronenergy_sm_lat]
      
      
      Longitude in SM Frame MMS2 [mms2_epd_eis_srvy_l2_electronenergy_sm_lon]
      
      
      Orbit number MMS2 [mms2_epd_eis_srvy_l2_electronenergy_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS2 [mms2_epd_eis_srvy_l2_electronenergy_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS2 [mms2_epd_eis_srvy_l2_electronenergy_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS2 [mms2_epd_eis_srvy_l2_electronenergy_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS2 [mms2_epd_eis_srvy_l2_electronenergy_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS2 [mms2_epd_eis_srvy_l2_electronenergy_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS2 [mms2_epd_eis_srvy_l2_electronenergy_ssd5]
      
      
      Valid Events Processed per second MMS2 [mms2_epd_eis_srvy_l2_electronenergy_vep]
      
      
      Valid Electron Events per second MMS2 [mms2_epd_eis_srvy_l2_electronenergy_vee]
      
      
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MMS2_EPD-EIS_SRVY_L2_EXTOF (spase://NASA/NumericalData/MMS/2/EnergeticParticleDetector/EIS/Survey/Level2/EnergyByTimeOfFlight/PT2.42S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms2_epd_eis_srvy_l2_extof_duration]
      
      
      ---> Instrument Deadtime [mms2_epd_eis_srvy_l2_extof_deadtime]
      
      
      ---> Instrument Large Pixel in Use [mms2_epd_eis_srvy_l2_extof_largepixel]
      
      
      ---> Spin [mms2_epd_eis_srvy_l2_extof_spin]
      
      
      ---> Sector [mms2_epd_eis_srvy_l2_extof_sector]
      
      
      ---> Quality Word [mms2_epd_eis_srvy_l2_extof_quality]
      
      
      MMS2 ExTOF-Survey proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_extof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms2_epd_eis_srvy_l2_extof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms2_epd_eis_srvy_l2_extof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms2_epd_eis_srvy_l2_extof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms2_epd_eis_srvy_l2_extof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms2_epd_eis_srvy_l2_extof_proton_P6_counts_t5]
      
      
      MMS2 ExTOF-Survey proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_extof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms2_epd_eis_srvy_l2_extof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms2_epd_eis_srvy_l2_extof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms2_epd_eis_srvy_l2_extof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms2_epd_eis_srvy_l2_extof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms2_epd_eis_srvy_l2_extof_proton_P6_cps_t5]
      
      
      MMS2 ExTOF-Survey proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_extof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms2_epd_eis_srvy_l2_extof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms2_epd_eis_srvy_l2_extof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms2_epd_eis_srvy_l2_extof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms2_epd_eis_srvy_l2_extof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms2_epd_eis_srvy_l2_extof_proton_P6_flux_t5]
      
      
      MMS2 ExTOF-Survey helium_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_extof_helium_P6_counts_t0]
      
      
      ---> helium_P6_counts_t1 [mms2_epd_eis_srvy_l2_extof_helium_P6_counts_t1]
      
      
      ---> helium_P6_counts_t2 [mms2_epd_eis_srvy_l2_extof_helium_P6_counts_t2]
      
      
      ---> helium_P6_counts_t3 [mms2_epd_eis_srvy_l2_extof_helium_P6_counts_t3]
      
      
      ---> helium_P6_counts_t4 [mms2_epd_eis_srvy_l2_extof_helium_P6_counts_t4]
      
      
      ---> helium_P6_counts_t5 [mms2_epd_eis_srvy_l2_extof_helium_P6_counts_t5]
      
      
      MMS2 ExTOF-Survey helium_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_extof_helium_P6_cps_t0]
      
      
      ---> helium_P6_cps_t1 [mms2_epd_eis_srvy_l2_extof_helium_P6_cps_t1]
      
      
      ---> helium_P6_cps_t2 [mms2_epd_eis_srvy_l2_extof_helium_P6_cps_t2]
      
      
      ---> helium_P6_cps_t3 [mms2_epd_eis_srvy_l2_extof_helium_P6_cps_t3]
      
      
      ---> helium_P6_cps_t4 [mms2_epd_eis_srvy_l2_extof_helium_P6_cps_t4]
      
      
      ---> helium_P6_cps_t5 [mms2_epd_eis_srvy_l2_extof_helium_P6_cps_t5]
      
      
      MMS2 ExTOF-Survey helium_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_extof_helium_P6_flux_t0]
      
      
      ---> helium_P6_flux_t1 [mms2_epd_eis_srvy_l2_extof_helium_P6_flux_t1]
      
      
      ---> helium_P6_flux_t2 [mms2_epd_eis_srvy_l2_extof_helium_P6_flux_t2]
      
      
      ---> helium_P6_flux_t3 [mms2_epd_eis_srvy_l2_extof_helium_P6_flux_t3]
      
      
      ---> helium_P6_flux_t4 [mms2_epd_eis_srvy_l2_extof_helium_P6_flux_t4]
      
      
      ---> helium_P6_flux_t5 [mms2_epd_eis_srvy_l2_extof_helium_P6_flux_t5]
      
      
      MMS2 ExTOF-Survey oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_extof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_counts_t5]
      
      
      MMS2 ExTOF-Survey oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_extof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_cps_t5]
      
      
      MMS2 ExTOF-Survey oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_extof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms2_epd_eis_srvy_l2_extof_oxygen_P6_flux_t5]
      
      
      MMS2 ExTOF-Survey dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_extof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms2_epd_eis_srvy_l2_extof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms2_epd_eis_srvy_l2_extof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms2_epd_eis_srvy_l2_extof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms2_epd_eis_srvy_l2_extof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms2_epd_eis_srvy_l2_extof_dump_P6_counts_t5]
      
      
      MMS2 ExTOF-Survey dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_extof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms2_epd_eis_srvy_l2_extof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms2_epd_eis_srvy_l2_extof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms2_epd_eis_srvy_l2_extof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms2_epd_eis_srvy_l2_extof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms2_epd_eis_srvy_l2_extof_dump_P6_cps_t5]
      
      
      MMS2 ExTOF-Survey dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_extof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms2_epd_eis_srvy_l2_extof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms2_epd_eis_srvy_l2_extof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms2_epd_eis_srvy_l2_extof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms2_epd_eis_srvy_l2_extof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms2_epd_eis_srvy_l2_extof_dump_P6_flux_t5]
      
      
      MMS2 ExTOF-Survey proton_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms2_epd_eis_srvy_l2_extof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms2_epd_eis_srvy_l2_extof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms2_epd_eis_srvy_l2_extof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms2_epd_eis_srvy_l2_extof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms2_epd_eis_srvy_l2_extof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms2_epd_eis_srvy_l2_extof_proton_P5_counts_t5]
      
      
      MMS2 ExTOF-Survey proton_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms2_epd_eis_srvy_l2_extof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms2_epd_eis_srvy_l2_extof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms2_epd_eis_srvy_l2_extof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms2_epd_eis_srvy_l2_extof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms2_epd_eis_srvy_l2_extof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms2_epd_eis_srvy_l2_extof_proton_P5_cps_t5]
      
      
      MMS2 ExTOF-Survey proton_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms2_epd_eis_srvy_l2_extof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms2_epd_eis_srvy_l2_extof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms2_epd_eis_srvy_l2_extof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms2_epd_eis_srvy_l2_extof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms2_epd_eis_srvy_l2_extof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms2_epd_eis_srvy_l2_extof_proton_P5_flux_t5]
      
      
      MMS2 ExTOF-Survey oxygen_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms2_epd_eis_srvy_l2_extof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_counts_t5]
      
      
      MMS2 ExTOF-Survey oxygen_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms2_epd_eis_srvy_l2_extof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_cps_t5]
      
      
      MMS2 ExTOF-Survey oxygen_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms2_epd_eis_srvy_l2_extof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms2_epd_eis_srvy_l2_extof_oxygen_P5_flux_t5]
      
      
      MMS2 ExTOF-Survey helium_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms2_epd_eis_srvy_l2_extof_helium_P5_counts_t0]
      
      
      ---> helium_P5_counts_t1 [mms2_epd_eis_srvy_l2_extof_helium_P5_counts_t1]
      
      
      ---> helium_P5_counts_t2 [mms2_epd_eis_srvy_l2_extof_helium_P5_counts_t2]
      
      
      ---> helium_P5_counts_t3 [mms2_epd_eis_srvy_l2_extof_helium_P5_counts_t3]
      
      
      ---> helium_P5_counts_t4 [mms2_epd_eis_srvy_l2_extof_helium_P5_counts_t4]
      
      
      ---> helium_P5_counts_t5 [mms2_epd_eis_srvy_l2_extof_helium_P5_counts_t5]
      
      
      MMS2 ExTOF-Survey helium_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms2_epd_eis_srvy_l2_extof_helium_P5_cps_t0]
      
      
      ---> helium_P5_cps_t1 [mms2_epd_eis_srvy_l2_extof_helium_P5_cps_t1]
      
      
      ---> helium_P5_cps_t2 [mms2_epd_eis_srvy_l2_extof_helium_P5_cps_t2]
      
      
      ---> helium_P5_cps_t3 [mms2_epd_eis_srvy_l2_extof_helium_P5_cps_t3]
      
      
      ---> helium_P5_cps_t4 [mms2_epd_eis_srvy_l2_extof_helium_P5_cps_t4]
      
      
      ---> helium_P5_cps_t5 [mms2_epd_eis_srvy_l2_extof_helium_P5_cps_t5]
      
      
      MMS2 ExTOF-Survey helium_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms2_epd_eis_srvy_l2_extof_helium_P5_flux_t0]
      
      
      ---> helium_P5_flux_t1 [mms2_epd_eis_srvy_l2_extof_helium_P5_flux_t1]
      
      
      ---> helium_P5_flux_t2 [mms2_epd_eis_srvy_l2_extof_helium_P5_flux_t2]
      
      
      ---> helium_P5_flux_t3 [mms2_epd_eis_srvy_l2_extof_helium_P5_flux_t3]
      
      
      ---> helium_P5_flux_t4 [mms2_epd_eis_srvy_l2_extof_helium_P5_flux_t4]
      
      
      ---> helium_P5_flux_t5 [mms2_epd_eis_srvy_l2_extof_helium_P5_flux_t5]
      
      
      MMS2 ExTOF-Survey proton_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms2_epd_eis_srvy_l2_extof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms2_epd_eis_srvy_l2_extof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms2_epd_eis_srvy_l2_extof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms2_epd_eis_srvy_l2_extof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms2_epd_eis_srvy_l2_extof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms2_epd_eis_srvy_l2_extof_proton_P4_counts_t5]
      
      
      MMS2 ExTOF-Survey proton_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms2_epd_eis_srvy_l2_extof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms2_epd_eis_srvy_l2_extof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms2_epd_eis_srvy_l2_extof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms2_epd_eis_srvy_l2_extof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms2_epd_eis_srvy_l2_extof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms2_epd_eis_srvy_l2_extof_proton_P4_cps_t5]
      
      
      MMS2 ExTOF-Survey proton_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms2_epd_eis_srvy_l2_extof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms2_epd_eis_srvy_l2_extof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms2_epd_eis_srvy_l2_extof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms2_epd_eis_srvy_l2_extof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms2_epd_eis_srvy_l2_extof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms2_epd_eis_srvy_l2_extof_proton_P4_flux_t5]
      
      
      MMS2 ExTOF-Survey alpha_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms2_epd_eis_srvy_l2_extof_helium_P4_counts_t0]
      
      
      ---> alpha_P4_counts_t1 [mms2_epd_eis_srvy_l2_extof_helium_P4_counts_t1]
      
      
      ---> alpha_P4_counts_t2 [mms2_epd_eis_srvy_l2_extof_helium_P4_counts_t2]
      
      
      ---> alpha_P4_counts_t3 [mms2_epd_eis_srvy_l2_extof_helium_P4_counts_t3]
      
      
      ---> alpha_P4_counts_t4 [mms2_epd_eis_srvy_l2_extof_helium_P4_counts_t4]
      
      
      ---> alpha_P4_counts_t5 [mms2_epd_eis_srvy_l2_extof_helium_P4_counts_t5]
      
      
      MMS2 ExTOF-Survey alpha_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms2_epd_eis_srvy_l2_extof_helium_P4_cps_t0]
      
      
      ---> alpha_P4_cps_t1 [mms2_epd_eis_srvy_l2_extof_helium_P4_cps_t1]
      
      
      ---> alpha_P4_cps_t2 [mms2_epd_eis_srvy_l2_extof_helium_P4_cps_t2]
      
      
      ---> alpha_P4_cps_t3 [mms2_epd_eis_srvy_l2_extof_helium_P4_cps_t3]
      
      
      ---> alpha_P4_cps_t4 [mms2_epd_eis_srvy_l2_extof_helium_P4_cps_t4]
      
      
      ---> alpha_P4_cps_t5 [mms2_epd_eis_srvy_l2_extof_helium_P4_cps_t5]
      
      
      MMS2 ExTOF-Survey alpha_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms2_epd_eis_srvy_l2_extof_helium_P4_flux_t0]
      
      
      ---> alpha_P4_flux_t1 [mms2_epd_eis_srvy_l2_extof_helium_P4_flux_t1]
      
      
      ---> alpha_P4_flux_t2 [mms2_epd_eis_srvy_l2_extof_helium_P4_flux_t2]
      
      
      ---> alpha_P4_flux_t3 [mms2_epd_eis_srvy_l2_extof_helium_P4_flux_t3]
      
      
      ---> alpha_P4_flux_t4 [mms2_epd_eis_srvy_l2_extof_helium_P4_flux_t4]
      
      
      ---> alpha_P4_flux_t5 [mms2_epd_eis_srvy_l2_extof_helium_P4_flux_t5]
      
      
      MMS2 ExTOF-Survey oxygen_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms2_epd_eis_srvy_l2_extof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_counts_t5]
      
      
      MMS2 ExTOF-Survey oxygen_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms2_epd_eis_srvy_l2_extof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_cps_t5]
      
      
      MMS2 ExTOF-Survey oxygen_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms2_epd_eis_srvy_l2_extof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms2_epd_eis_srvy_l2_extof_oxygen_P4_flux_t5]
      
      
      MMS2 ExTOF-Survey proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_extof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms2_epd_eis_srvy_l2_extof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms2_epd_eis_srvy_l2_extof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms2_epd_eis_srvy_l2_extof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms2_epd_eis_srvy_l2_extof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms2_epd_eis_srvy_l2_extof_proton_P3_counts_t5]
      
      
      MMS2 ExTOF-Survey proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_extof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms2_epd_eis_srvy_l2_extof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms2_epd_eis_srvy_l2_extof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms2_epd_eis_srvy_l2_extof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms2_epd_eis_srvy_l2_extof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms2_epd_eis_srvy_l2_extof_proton_P3_cps_t5]
      
      
      MMS2 ExTOF-Survey proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_extof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms2_epd_eis_srvy_l2_extof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms2_epd_eis_srvy_l2_extof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms2_epd_eis_srvy_l2_extof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms2_epd_eis_srvy_l2_extof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms2_epd_eis_srvy_l2_extof_proton_P3_flux_t5]
      
      
      MMS2 ExTOF-Survey alpha_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_extof_helium_P3_counts_t0]
      
      
      ---> alpha_P3_counts_t1 [mms2_epd_eis_srvy_l2_extof_helium_P3_counts_t1]
      
      
      ---> alpha_P3_counts_t2 [mms2_epd_eis_srvy_l2_extof_helium_P3_counts_t2]
      
      
      ---> alpha_P3_counts_t3 [mms2_epd_eis_srvy_l2_extof_helium_P3_counts_t3]
      
      
      ---> alpha_P3_counts_t4 [mms2_epd_eis_srvy_l2_extof_helium_P3_counts_t4]
      
      
      ---> alpha_P3_counts_t5 [mms2_epd_eis_srvy_l2_extof_helium_P3_counts_t5]
      
      
      MMS2 ExTOF-Survey alpha_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_extof_helium_P3_cps_t0]
      
      
      ---> alpha_P3_cps_t1 [mms2_epd_eis_srvy_l2_extof_helium_P3_cps_t1]
      
      
      ---> alpha_P3_cps_t2 [mms2_epd_eis_srvy_l2_extof_helium_P3_cps_t2]
      
      
      ---> alpha_P3_cps_t3 [mms2_epd_eis_srvy_l2_extof_helium_P3_cps_t3]
      
      
      ---> alpha_P3_cps_t4 [mms2_epd_eis_srvy_l2_extof_helium_P3_cps_t4]
      
      
      ---> alpha_P3_cps_t5 [mms2_epd_eis_srvy_l2_extof_helium_P3_cps_t5]
      
      
      MMS2 ExTOF-Survey alpha_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_extof_helium_P3_flux_t0]
      
      
      ---> alpha_P3_flux_t1 [mms2_epd_eis_srvy_l2_extof_helium_P3_flux_t1]
      
      
      ---> alpha_P3_flux_t2 [mms2_epd_eis_srvy_l2_extof_helium_P3_flux_t2]
      
      
      ---> alpha_P3_flux_t3 [mms2_epd_eis_srvy_l2_extof_helium_P3_flux_t3]
      
      
      ---> alpha_P3_flux_t4 [mms2_epd_eis_srvy_l2_extof_helium_P3_flux_t4]
      
      
      ---> alpha_P3_flux_t5 [mms2_epd_eis_srvy_l2_extof_helium_P3_flux_t5]
      
      
      MMS2 ExTOF-Survey oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_extof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_counts_t5]
      
      
      MMS2 ExTOF-Survey oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_extof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_cps_t5]
      
      
      MMS2 ExTOF-Survey oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_extof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms2_epd_eis_srvy_l2_extof_oxygen_P3_flux_t5]
      
      
      MMS2 ExTOF-Survey dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_extof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms2_epd_eis_srvy_l2_extof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms2_epd_eis_srvy_l2_extof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms2_epd_eis_srvy_l2_extof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms2_epd_eis_srvy_l2_extof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms2_epd_eis_srvy_l2_extof_dump_P3_counts_t5]
      
      
      MMS2 ExTOF-Survey dump_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms2_epd_eis_srvy_l2_extof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms2_epd_eis_srvy_l2_extof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms2_epd_eis_srvy_l2_extof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms2_epd_eis_srvy_l2_extof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms2_epd_eis_srvy_l2_extof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms2_epd_eis_srvy_l2_extof_dump_P4_counts_t5]
      
      
      MMS2 ExTOF-Survey dump_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms2_epd_eis_srvy_l2_extof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms2_epd_eis_srvy_l2_extof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms2_epd_eis_srvy_l2_extof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms2_epd_eis_srvy_l2_extof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms2_epd_eis_srvy_l2_extof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms2_epd_eis_srvy_l2_extof_dump_P5_counts_t5]
      
      
      MMS2 ExTOF-Survey dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_extof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms2_epd_eis_srvy_l2_extof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms2_epd_eis_srvy_l2_extof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms2_epd_eis_srvy_l2_extof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms2_epd_eis_srvy_l2_extof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms2_epd_eis_srvy_l2_extof_dump_P3_cps_t5]
      
      
      MMS2 ExTOF-Survey dump_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms2_epd_eis_srvy_l2_extof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms2_epd_eis_srvy_l2_extof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms2_epd_eis_srvy_l2_extof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms2_epd_eis_srvy_l2_extof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms2_epd_eis_srvy_l2_extof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms2_epd_eis_srvy_l2_extof_dump_P4_cps_t5]
      
      
      MMS2 ExTOF-Survey dump_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms2_epd_eis_srvy_l2_extof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms2_epd_eis_srvy_l2_extof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms2_epd_eis_srvy_l2_extof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms2_epd_eis_srvy_l2_extof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms2_epd_eis_srvy_l2_extof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms2_epd_eis_srvy_l2_extof_dump_P5_cps_t5]
      
      
      MMS2 ExTOF-Survey dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_extof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms2_epd_eis_srvy_l2_extof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms2_epd_eis_srvy_l2_extof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms2_epd_eis_srvy_l2_extof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms2_epd_eis_srvy_l2_extof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms2_epd_eis_srvy_l2_extof_dump_P3_flux_t5]
      
      
      MMS2 ExTOF-Survey dump_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms2_epd_eis_srvy_l2_extof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms2_epd_eis_srvy_l2_extof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms2_epd_eis_srvy_l2_extof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms2_epd_eis_srvy_l2_extof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms2_epd_eis_srvy_l2_extof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms2_epd_eis_srvy_l2_extof_dump_P4_flux_t5]
      
      
      MMS2 ExTOF-Survey dump_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms2_epd_eis_srvy_l2_extof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms2_epd_eis_srvy_l2_extof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms2_epd_eis_srvy_l2_extof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms2_epd_eis_srvy_l2_extof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms2_epd_eis_srvy_l2_extof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms2_epd_eis_srvy_l2_extof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS2 [mms2_epd_eis_srvy_l2_extof_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS2 [mms2_epd_eis_srvy_l2_extof_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS2 [mms2_epd_eis_srvy_l2_extof_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS2 [mms2_epd_eis_srvy_l2_extof_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS2 [mms2_epd_eis_srvy_l2_extof_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS2 [mms2_epd_eis_srvy_l2_extof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS2 [mms2_epd_eis_srvy_l2_extof_look_t0]
      
      
      Look Direction for Telescope 1 MMS2 [mms2_epd_eis_srvy_l2_extof_look_t1]
      
      
      Look Direction for Telescope 2 MMS2 [mms2_epd_eis_srvy_l2_extof_look_t2]
      
      
      Look Direction for Telescope 3 MMS2 [mms2_epd_eis_srvy_l2_extof_look_t3]
      
      
      Look Direction for Telescope 4 MMS2 [mms2_epd_eis_srvy_l2_extof_look_t4]
      
      
      Look Direction for Telescope 5 MMS2 [mms2_epd_eis_srvy_l2_extof_look_t5]
      
      
      Magnetic Field BCS MMS2 [mms2_epd_eis_srvy_l2_extof_b]
      
      
      Spacecraft position GSE MMS2 [mms2_epd_eis_srvy_l2_extof_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS2 [mms2_epd_eis_srvy_l2_extof_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS2 [mms2_epd_eis_srvy_l2_extof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS2 [mms2_epd_eis_srvy_l2_extof_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS2 [mms2_epd_eis_srvy_l2_extof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS2 [mms2_epd_eis_srvy_l2_extof_r]
      
      
      Dipole L-shell MMS2 [mms2_epd_eis_srvy_l2_extof_l]
      
      
      Latitude in GSE Frame MMS2 [mms2_epd_eis_srvy_l2_extof_gse_lat]
      
      
      Longitude in GSE Frame MMS2 [mms2_epd_eis_srvy_l2_extof_gse_lon]
      
      
      Latitude in GSM Frame MMS2 [mms2_epd_eis_srvy_l2_extof_gsm_lat]
      
      
      Longitude in GSM Frame MMS2 [mms2_epd_eis_srvy_l2_extof_gsm_lon]
      
      
      Latitude in SM Frame MMS2 [mms2_epd_eis_srvy_l2_extof_sm_lat]
      
      
      Longitude in SM Frame MMS2 [mms2_epd_eis_srvy_l2_extof_sm_lon]
      
      
      Orbit number MMS2 [mms2_epd_eis_srvy_l2_extof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS2 [mms2_epd_eis_srvy_l2_extof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS2 [mms2_epd_eis_srvy_l2_extof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS2 [mms2_epd_eis_srvy_l2_extof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS2 [mms2_epd_eis_srvy_l2_extof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS2 [mms2_epd_eis_srvy_l2_extof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS2 [mms2_epd_eis_srvy_l2_extof_ssd5]
      
      
      Valid Events Processed per second MMS2 [mms2_epd_eis_srvy_l2_extof_vep]
      
      
      Start 0 Anode Count Rate MMS2 [mms2_epd_eis_srvy_l2_extof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS2 [mms2_epd_eis_srvy_l2_extof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS2 [mms2_epd_eis_srvy_l2_extof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS2 [mms2_epd_eis_srvy_l2_extof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS2 [mms2_epd_eis_srvy_l2_extof_vtofxphe]
      
      
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MMS2_EPD-EIS_SRVY_L2_PHXTOF (spase://NASA/NumericalData/MMS/2/EnergeticParticleDetector/EIS/Survey/Level2/PulseHeightByTimeOfFlight/PT2.42S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms2_epd_eis_srvy_l2_phxtof_duration]
      
      
      Instrument Deadtime [mms2_epd_eis_srvy_l2_phxtof_deadtime]
      
      
      Instrument Large Pixel in Use [mms2_epd_eis_srvy_l2_phxtof_largepixel]
      
      
      Spin [mms2_epd_eis_srvy_l2_phxtof_spin]
      
      
      Sector [mms2_epd_eis_srvy_l2_phxtof_sector]
      
      
      Quality Word [mms2_epd_eis_srvy_l2_phxtof_quality]
      
      
      MMS2 PhxTOF-Survey proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_counts_t5]
      
      
      MMS2 PhxTOF-Survey proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_cps_t5]
      
      
      MMS2 PhxTOF-Survey proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms2_epd_eis_srvy_l2_phxtof_proton_P6_flux_t5]
      
      
      MMS2 PhxTOF-Survey oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t5]
      
      
      MMS2 PhxTOF-Survey oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t5]
      
      
      MMS2 PhxTOF-Survey oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t5]
      
      
      MMS2 PhxTOF-Survey dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_counts_t5]
      
      
      MMS2 PhxTOF-Survey dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_cps_t5]
      
      
      MMS2 PhxTOF-Survey dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms2_epd_eis_srvy_l2_phxtof_dump_P6_flux_t5]
      
      
      MMS2 PhxTOF-Survey proton_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_counts_t5]
      
      
      MMS2 PhxTOF-Survey proton_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_cps_t5]
      
      
      MMS2 PhxTOF-Survey proton_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms2_epd_eis_srvy_l2_phxtof_proton_P5_flux_t5]
      
      
      MMS2 PhxTOF-Survey oxygen_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t5]
      
      
      MMS2 PhxTOF-Survey oxygen_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t5]
      
      
      MMS2 PhxTOF-Survey oxygen_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t5]
      
      
      MMS2 PhxTOF-Survey proton_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_phxtof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_counts_t5]
      
      
      MMS2 PhxTOF-Survey proton_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_phxtof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_cps_t5]
      
      
      MMS2 PhxTOF-Survey proton_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_phxtof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms2_epd_eis_srvy_l2_phxtof_proton_P4_flux_t5]
      
      
      MMS2 PhxTOF-Survey oxygen_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t5]
      
      
      MMS2 PhxTOF-Survey oxygen_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t5]
      
      
      MMS2 PhxTOF-Survey oxygen_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t5]
      
      
      MMS2 PhxTOF-Survey proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_phxtof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_counts_t5]
      
      
      MMS2 PhxTOF-Survey proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_phxtof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_cps_t5]
      
      
      MMS2 PhxTOF-Survey proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_phxtof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms2_epd_eis_srvy_l2_phxtof_proton_P3_flux_t5]
      
      
      MMS2 PhxTOF-Survey oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t5]
      
      
      MMS2 PhxTOF-Survey oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t5]
      
      
      MMS2 PhxTOF-Survey oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms2_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t5]
      
      
      MMS2 PhxTOF-Survey dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_phxtof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_counts_t5]
      
      
      MMS2 PhxTOF-Survey dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_phxtof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_counts_t5]
      
      
      MMS2 PhxTOF-Survey dump_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_counts_t5]
      
      
      MMS2 PhxTOF-Survey dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_phxtof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_cps_t5]
      
      
      MMS2 PhxTOF-Survey dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_phxtof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_cps_t5]
      
      
      MMS2 PhxTOF-Survey dump_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_cps_t5]
      
      
      MMS2 PhxTOF-Survey dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms2_epd_eis_srvy_l2_phxtof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms2_epd_eis_srvy_l2_phxtof_dump_P3_flux_t5]
      
      
      MMS2 PhxTOF-Survey dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms2_epd_eis_srvy_l2_phxtof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms2_epd_eis_srvy_l2_phxtof_dump_P4_flux_t5]
      
      
      MMS2 PhxTOF-Survey dump_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms2_epd_eis_srvy_l2_phxtof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms2_epd_eis_srvy_l2_phxtof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS2 [mms2_epd_eis_srvy_l2_phxtof_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS2 [mms2_epd_eis_srvy_l2_phxtof_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS2 [mms2_epd_eis_srvy_l2_phxtof_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS2 [mms2_epd_eis_srvy_l2_phxtof_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS2 [mms2_epd_eis_srvy_l2_phxtof_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS2 [mms2_epd_eis_srvy_l2_phxtof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS2 [mms2_epd_eis_srvy_l2_phxtof_look_t0]
      
      
      Look Direction for Telescope 1 MMS2 [mms2_epd_eis_srvy_l2_phxtof_look_t1]
      
      
      Look Direction for Telescope 2 MMS2 [mms2_epd_eis_srvy_l2_phxtof_look_t2]
      
      
      Look Direction for Telescope 3 MMS2 [mms2_epd_eis_srvy_l2_phxtof_look_t3]
      
      
      Look Direction for Telescope 4 MMS2 [mms2_epd_eis_srvy_l2_phxtof_look_t4]
      
      
      Look Direction for Telescope 5 MMS2 [mms2_epd_eis_srvy_l2_phxtof_look_t5]
      
      
      Magnetic Field BCS MMS2 [mms2_epd_eis_srvy_l2_phxtof_b]
      
      
      Spacecraft position GSE MMS2 [mms2_epd_eis_srvy_l2_phxtof_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS2 [mms2_epd_eis_srvy_l2_phxtof_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS2 [mms2_epd_eis_srvy_l2_phxtof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS2 [mms2_epd_eis_srvy_l2_phxtof_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS2 [mms2_epd_eis_srvy_l2_phxtof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS2 [mms2_epd_eis_srvy_l2_phxtof_r]
      
      
      Dipole L-shell MMS2 [mms2_epd_eis_srvy_l2_phxtof_l]
      
      
      Latitude in GSE Frame MMS2 [mms2_epd_eis_srvy_l2_phxtof_gse_lat]
      
      
      Longitude in GSE Frame MMS2 [mms2_epd_eis_srvy_l2_phxtof_gse_lon]
      
      
      Latitude in GSM Frame MMS2 [mms2_epd_eis_srvy_l2_phxtof_gsm_lat]
      
      
      Longitude in GSM Frame MMS2 [mms2_epd_eis_srvy_l2_phxtof_gsm_lon]
      
      
      Latitude in SM Frame MMS2 [mms2_epd_eis_srvy_l2_phxtof_sm_lat]
      
      
      Longitude in SM Frame MMS2 [mms2_epd_eis_srvy_l2_phxtof_sm_lon]
      
      
      Orbit number MMS2 [mms2_epd_eis_srvy_l2_phxtof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS2 [mms2_epd_eis_srvy_l2_phxtof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS2 [mms2_epd_eis_srvy_l2_phxtof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS2 [mms2_epd_eis_srvy_l2_phxtof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS2 [mms2_epd_eis_srvy_l2_phxtof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS2 [mms2_epd_eis_srvy_l2_phxtof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS2 [mms2_epd_eis_srvy_l2_phxtof_ssd5]
      
      
      Valid Events Processed per second MMS2 [mms2_epd_eis_srvy_l2_phxtof_vep]
      
      
      Start 0 Anode Count Rate MMS2 [mms2_epd_eis_srvy_l2_phxtof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS2 [mms2_epd_eis_srvy_l2_phxtof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS2 [mms2_epd_eis_srvy_l2_phxtof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS2 [mms2_epd_eis_srvy_l2_phxtof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS2 [mms2_epd_eis_srvy_l2_phxtof_vtofxphe]
      
      
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MMS2_FEEPS_BRST_L2_ELECTRON (spase://NASA/NumericalData/MMS/2/EnergeticParticleDetector/FEEPS/Burst/Level2/Electron/PT0.3025S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms2_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms2_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms2_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms2_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms2_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms2_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms2_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms2_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms2_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_12]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms2_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms2_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms2_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms2_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms2_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms2_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms2_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms2_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms2_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_12]
      
      
      MMS2 FEEPS top side burst mode electron count rate sensor 1 [mms2_epd_feeps_brst_l2_electron_top_count_rate_sensorid_1]
      
      
      MMS2 FEEPS top side burst mode electron count rate sensor 2 [mms2_epd_feeps_brst_l2_electron_top_count_rate_sensorid_2]
      
      
      MMS2 FEEPS top side burst mode electron count rate sensor 3 [mms2_epd_feeps_brst_l2_electron_top_count_rate_sensorid_3]
      
      
      MMS2 FEEPS top side burst mode electron count rate sensor 4 [mms2_epd_feeps_brst_l2_electron_top_count_rate_sensorid_4]
      
      
      MMS2 FEEPS top side burst mode electron count rate sensor 5 [mms2_epd_feeps_brst_l2_electron_top_count_rate_sensorid_5]
      
      
      MMS2 FEEPS top side burst mode electron count rate sensor 9 [mms2_epd_feeps_brst_l2_electron_top_count_rate_sensorid_9]
      
      
      MMS2 FEEPS top side burst mode electron count rate sensor 10 [mms2_epd_feeps_brst_l2_electron_top_count_rate_sensorid_10]
      
      
      MMS2 FEEPS top side burst mode electron count rate sensor 11 [mms2_epd_feeps_brst_l2_electron_top_count_rate_sensorid_11]
      
      
      MMS2 FEEPS top side burst mode electron count rate sensor 12 [mms2_epd_feeps_brst_l2_electron_top_count_rate_sensorid_12]
      
      
      MMS2 FEEPS bottom side burst mode electron count rate sensor 1 [mms2_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_1]
      
      
      MMS2 FEEPS bottom side burst mode electron count rate sensor 2 [mms2_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_2]
      
      
      MMS2 FEEPS bottom side burst mode electron count rate sensor 3 [mms2_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_3]
      
      
      MMS2 FEEPS bottom side burst mode electron count rate sensor 4 [mms2_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_4]
      
      
      MMS2 FEEPS bottom side burst mode electron count rate sensor 5 [mms2_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_5]
      
      
      MMS2 FEEPS bottom side burst mode electron count rate sensor 9 [mms2_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_9]
      
      
      MMS2 FEEPS bottom side burst mode electron count rate sensor 10 [mms2_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_10]
      
      
      MMS2 FEEPS bottom side burst mode electron count rate sensor 11 [mms2_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_11]
      
      
      MMS2 FEEPS bottom side burst mode electron count rate sensor 12 [mms2_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_12]
      
      
      MMS2 FEEPS top side burst mode electron intensity sensor 1 [mms2_epd_feeps_brst_l2_electron_top_intensity_sensorid_1]
      
      
      MMS2 FEEPS top side burst mode electron intensity sensor 2 [mms2_epd_feeps_brst_l2_electron_top_intensity_sensorid_2]
      
      
      MMS2 FEEPS top side burst mode electron intensity sensor 3 [mms2_epd_feeps_brst_l2_electron_top_intensity_sensorid_3]
      
      
      MMS2 FEEPS top side burst mode electron intensity sensor 4 [mms2_epd_feeps_brst_l2_electron_top_intensity_sensorid_4]
      
      
      MMS2 FEEPS top side burst mode electron intensity sensor 5 [mms2_epd_feeps_brst_l2_electron_top_intensity_sensorid_5]
      
      
      MMS2 FEEPS top side burst mode electron intensity sensor 9 [mms2_epd_feeps_brst_l2_electron_top_intensity_sensorid_9]
      
      
      MMS2 FEEPS top side burst mode electron intensity sensor 10 [mms2_epd_feeps_brst_l2_electron_top_intensity_sensorid_10]
      
      
      MMS2 FEEPS top side burst mode electron intensity sensor 11 [mms2_epd_feeps_brst_l2_electron_top_intensity_sensorid_11]
      
      
      MMS2 FEEPS top side burst mode electron intensity sensor 12 [mms2_epd_feeps_brst_l2_electron_top_intensity_sensorid_12]
      
      
      MMS2 FEEPS bottom side burst mode electron intensity sensor 1 [mms2_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_1]
      
      
      MMS2 FEEPS bottom side burst mode electron intensity sensor 2 [mms2_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_2]
      
      
      MMS2 FEEPS bottom side burst mode electron intensity sensor 3 [mms2_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_3]
      
      
      MMS2 FEEPS bottom side burst mode electron intensity sensor 4 [mms2_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_4]
      
      
      MMS2 FEEPS bottom side burst mode electron intensity sensor 5 [mms2_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_5]
      
      
      MMS2 FEEPS bottom side burst mode electron intensity sensor 9 [mms2_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_9]
      
      
      MMS2 FEEPS bottom side burst mode electron intensity sensor 10 [mms2_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_10]
      
      
      MMS2 FEEPS bottom side burst mode electron intensity sensor 11 [mms2_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_11]
      
      
      MMS2 FEEPS bottom side burst mode electron intensity sensor 12 [mms2_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_12]
      
      
      MMS2 FEEPS top side burst mode electron count error statistics sensor 1 [mms2_epd_feeps_brst_l2_electron_top_percent_error_sensorid_1]
      
      
      MMS2 FEEPS top side burst mode electron count error statistics sensor 2 [mms2_epd_feeps_brst_l2_electron_top_percent_error_sensorid_2]
      
      
      MMS2 FEEPS top side burst mode electron count error statistics sensor 3 [mms2_epd_feeps_brst_l2_electron_top_percent_error_sensorid_3]
      
      
      MMS2 FEEPS top side burst mode electron count error statistics sensor 4 [mms2_epd_feeps_brst_l2_electron_top_percent_error_sensorid_4]
      
      
      MMS2 FEEPS top side burst mode electron count error statistics sensor 5 [mms2_epd_feeps_brst_l2_electron_top_percent_error_sensorid_5]
      
      
      MMS2 FEEPS top side burst mode electron count error statistics sensor 9 [mms2_epd_feeps_brst_l2_electron_top_percent_error_sensorid_9]
      
      
      MMS2 FEEPS top side burst mode electron count error statistics sensor 10 [mms2_epd_feeps_brst_l2_electron_top_percent_error_sensorid_10]
      
      
      MMS2 FEEPS top side burst mode electron count error statistics sensor 11 [mms2_epd_feeps_brst_l2_electron_top_percent_error_sensorid_11]
      
      
      MMS2 FEEPS top side burst mode electron count error statistics sensor 12 [mms2_epd_feeps_brst_l2_electron_top_percent_error_sensorid_12]
      
      
      MMS2 FEEPS bottom side burst mode electron count error statistics sensor 1 [mms2_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_1]
      
      
      MMS2 FEEPS bottom side burst mode electron count error statistics sensor 2 [mms2_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_2]
      
      
      MMS2 FEEPS bottom side burst mode electron count error statistics sensor 3 [mms2_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_3]
      
      
      MMS2 FEEPS bottom side burst mode electron count error statistics sensor 4 [mms2_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_4]
      
      
      MMS2 FEEPS bottom side burst mode electron count error statistics sensor 5 [mms2_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_5]
      
      
      MMS2 FEEPS bottom side burst mode electron count error statistics sensor 9 [mms2_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_9]
      
      
      MMS2 FEEPS bottom side burst mode electron count error statistics sensor 10 [mms2_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_10]
      
      
      MMS2 FEEPS bottom side burst mode electron count error statistics sensor 11 [mms2_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_11]
      
      
      MMS2 FEEPS bottom side burst mode electron count error statistics sensor 12 [mms2_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_12]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms2_epd_feeps_brst_l2_electron_pitch_angle]
      
      
      Latitude [mms2_epd_feeps_brst_l2_electron_lat_gse]
      
      
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MMS2_FEEPS_BRST_L2_ION (spase://NASA/NumericalData/MMS/2/EnergeticParticleDetector/FEEPS/Burst/Level2/Ion/PT0.3025S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms2_epd_feeps_brst_l2_ion_top_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms2_epd_feeps_brst_l2_ion_top_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms2_epd_feeps_brst_l2_ion_top_quality_indicator_sensorid_8]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms2_epd_feeps_brst_l2_ion_bottom_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms2_epd_feeps_brst_l2_ion_bottom_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms2_epd_feeps_brst_l2_ion_bottom_quality_indicator_sensorid_8]
      
      
      MMS2 FEEPS top side burst mode ion count rate sensor 6 [mms2_epd_feeps_brst_l2_ion_top_count_rate_sensorid_6]
      
      
      MMS2 FEEPS top side burst mode ion count rate sensor 7 [mms2_epd_feeps_brst_l2_ion_top_count_rate_sensorid_7]
      
      
      MMS2 FEEPS top side burst mode ion count rate sensor 8 [mms2_epd_feeps_brst_l2_ion_top_count_rate_sensorid_8]
      
      
      MMS2 FEEPS bottom side burst mode ion count rate sensor 6 [mms2_epd_feeps_brst_l2_ion_bottom_count_rate_sensorid_6]
      
      
      MMS2 FEEPS bottom side burst mode ion count rate sensor 7 [mms2_epd_feeps_brst_l2_ion_bottom_count_rate_sensorid_7]
      
      
      MMS2 FEEPS bottom side burst mode ion count rate sensor 8 [mms2_epd_feeps_brst_l2_ion_bottom_count_rate_sensorid_8]
      
      
      MMS2 FEEPS top side burst mode ion intensity sensor 6 [mms2_epd_feeps_brst_l2_ion_top_intensity_sensorid_6]
      
      
      MMS2 FEEPS top side burst mode ion intensity sensor 7 [mms2_epd_feeps_brst_l2_ion_top_intensity_sensorid_7]
      
      
      MMS2 FEEPS top side burst mode ion intensity sensor 8 [mms2_epd_feeps_brst_l2_ion_top_intensity_sensorid_8]
      
      
      MMS2 FEEPS bottom side burst mode ion intensity sensor 6 [mms2_epd_feeps_brst_l2_ion_bottom_intensity_sensorid_6]
      
      
      MMS2 FEEPS bottom side burst mode ion intensity sensor 7 [mms2_epd_feeps_brst_l2_ion_bottom_intensity_sensorid_7]
      
      
      MMS2 FEEPS bottom side burst mode ion intensity sensor 8 [mms2_epd_feeps_brst_l2_ion_bottom_intensity_sensorid_8]
      
      
      MMS2 FEEPS top side burst mode ion count error statistics sensor 6 [mms2_epd_feeps_brst_l2_ion_top_percent_error_sensorid_6]
      
      
      MMS2 FEEPS top side burst mode ion count error statistics sensor 7 [mms2_epd_feeps_brst_l2_ion_top_percent_error_sensorid_7]
      
      
      MMS2 FEEPS top side burst mode ion count error statistics sensor 8 [mms2_epd_feeps_brst_l2_ion_top_percent_error_sensorid_8]
      
      
      MMS2 FEEPS bottom side burst mode ion count error statistics sensor 6 [mms2_epd_feeps_brst_l2_ion_bottom_percent_error_sensorid_6]
      
      
      MMS2 FEEPS bottom side burst mode ion count error statistics sensor 7 [mms2_epd_feeps_brst_l2_ion_bottom_percent_error_sensorid_7]
      
      
      MMS2 FEEPS bottom side burst mode ion count error statistics sensor 8 [mms2_epd_feeps_brst_l2_ion_bottom_percent_error_sensorid_8]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms2_epd_feeps_brst_l2_ion_pitch_angle]
      
      
      Latitude [mms2_epd_feeps_brst_l2_ion_lat_gse]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS2_FEEPS_SRVY_L2_ELECTRON (spase://NASA/NumericalData/MMS/2/EnergeticParticleDetector/FEEPS/Survey/Level2/Electron/PT2.42S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms2_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms2_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms2_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms2_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms2_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms2_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms2_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms2_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms2_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_12]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms2_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms2_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms2_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms2_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms2_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms2_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms2_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms2_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms2_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_12]
      
      
      MMS2 FEEPS top side survey mode electron count rate sensor 1 [mms2_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_1]
      
      
      MMS2 FEEPS top side survey mode electron count rate sensor 2 [mms2_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_2]
      
      
      MMS2 FEEPS top side survey mode electron count rate sensor 3 [mms2_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_3]
      
      
      MMS2 FEEPS top side survey mode electron count rate sensor 4 [mms2_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_4]
      
      
      MMS2 FEEPS top side survey mode electron count rate sensor 5 [mms2_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_5]
      
      
      MMS2 FEEPS top side survey mode electron count rate sensor 9 [mms2_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_9]
      
      
      MMS2 FEEPS top side survey mode electron count rate sensor 10 [mms2_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_10]
      
      
      MMS2 FEEPS top side survey mode electron count rate sensor 11 [mms2_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_11]
      
      
      MMS2 FEEPS top side survey mode electron count rate sensor 12 [mms2_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_12]
      
      
      MMS2 FEEPS bottom side survey mode electron count rate sensor 1 [mms2_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_1]
      
      
      MMS2 FEEPS bottom side survey mode electron count rate sensor 2 [mms2_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_2]
      
      
      MMS2 FEEPS bottom side survey mode electron count rate sensor 3 [mms2_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_3]
      
      
      MMS2 FEEPS bottom side survey mode electron count rate sensor 4 [mms2_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_4]
      
      
      MMS2 FEEPS bottom side survey mode electron count rate sensor 5 [mms2_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_5]
      
      
      MMS2 FEEPS bottom side survey mode electron count rate sensor 9 [mms2_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_9]
      
      
      MMS2 FEEPS bottom side survey mode electron count rate sensor 10 [mms2_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_10]
      
      
      MMS2 FEEPS bottom side survey mode electron count rate sensor 11 [mms2_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_11]
      
      
      MMS2 FEEPS bottom side survey mode electron count rate sensor 12 [mms2_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_12]
      
      
      MMS2 FEEPS top side survey mode electron intensity sensor 1 [mms2_epd_feeps_srvy_l2_electron_top_intensity_sensorid_1]
      
      
      MMS2 FEEPS top side survey mode electron intensity sensor 2 [mms2_epd_feeps_srvy_l2_electron_top_intensity_sensorid_2]
      
      
      MMS2 FEEPS top side survey mode electron intensity sensor 3 [mms2_epd_feeps_srvy_l2_electron_top_intensity_sensorid_3]
      
      
      MMS2 FEEPS top side survey mode electron intensity sensor 4 [mms2_epd_feeps_srvy_l2_electron_top_intensity_sensorid_4]
      
      
      MMS2 FEEPS top side survey mode electron intensity sensor 5 [mms2_epd_feeps_srvy_l2_electron_top_intensity_sensorid_5]
      
      
      MMS2 FEEPS top side survey mode electron intensity sensor 9 [mms2_epd_feeps_srvy_l2_electron_top_intensity_sensorid_9]
      
      
      MMS2 FEEPS top side survey mode electron intensity sensor 10 [mms2_epd_feeps_srvy_l2_electron_top_intensity_sensorid_10]
      
      
      MMS2 FEEPS top side survey mode electron intensity sensor 11 [mms2_epd_feeps_srvy_l2_electron_top_intensity_sensorid_11]
      
      
      MMS2 FEEPS top side survey mode electron intensity sensor 12 [mms2_epd_feeps_srvy_l2_electron_top_intensity_sensorid_12]
      
      
      MMS2 FEEPS bottom side survey mode electron intensity sensor 1 [mms2_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_1]
      
      
      MMS2 FEEPS bottom side survey mode electron intensity sensor 2 [mms2_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_2]
      
      
      MMS2 FEEPS bottom side survey mode electron intensity sensor 3 [mms2_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_3]
      
      
      MMS2 FEEPS bottom side survey mode electron intensity sensor 4 [mms2_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_4]
      
      
      MMS2 FEEPS bottom side survey mode electron intensity sensor 5 [mms2_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_5]
      
      
      MMS2 FEEPS bottom side survey mode electron intensity sensor 9 [mms2_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_9]
      
      
      MMS2 FEEPS bottom side survey mode electron intensity sensor 10 [mms2_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_10]
      
      
      MMS2 FEEPS bottom side survey mode electron intensity sensor 11 [mms2_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_11]
      
      
      MMS2 FEEPS bottom side survey mode electron intensity sensor 12 [mms2_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_12]
      
      
      MMS2 FEEPS top side survey mode electron count error statistics sensor 1 [mms2_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_1]
      
      
      MMS2 FEEPS top side survey mode electron count error statistics sensor 2 [mms2_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_2]
      
      
      MMS2 FEEPS top side survey mode electron count error statistics sensor 3 [mms2_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_3]
      
      
      MMS2 FEEPS top side survey mode electron count error statistics sensor 4 [mms2_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_4]
      
      
      MMS2 FEEPS top side survey mode electron count error statistics sensor 5 [mms2_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_5]
      
      
      MMS2 FEEPS top side survey mode electron count error statistics sensor 9 [mms2_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_9]
      
      
      MMS2 FEEPS top side survey mode electron count error statistics sensor 10 [mms2_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_10]
      
      
      MMS2 FEEPS top side survey mode electron count error statistics sensor 11 [mms2_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_11]
      
      
      MMS2 FEEPS top side survey mode electron count error statistics sensor 12 [mms2_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_12]
      
      
      MMS2 FEEPS bottom side survey mode electron count error statistics sensor 1 [mms2_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_1]
      
      
      MMS2 FEEPS bottom side survey mode electron count error statistics sensor 2 [mms2_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_2]
      
      
      MMS2 FEEPS bottom side survey mode electron count error statistics sensor 3 [mms2_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_3]
      
      
      MMS2 FEEPS bottom side survey mode electron count error statistics sensor 4 [mms2_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_4]
      
      
      MMS2 FEEPS bottom side survey mode electron count error statistics sensor 5 [mms2_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_5]
      
      
      MMS2 FEEPS bottom side survey mode electron count error statistics sensor 9 [mms2_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_9]
      
      
      MMS2 FEEPS bottom side survey mode electron count error statistics sensor 10 [mms2_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_10]
      
      
      MMS2 FEEPS bottom side survey mode electron count error statistics sensor 11 [mms2_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_11]
      
      
      MMS2 FEEPS bottom side survey mode electron count error statistics sensor 12 [mms2_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_12]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms2_epd_feeps_srvy_l2_electron_pitch_angle]
      
      
      Latitude [mms2_epd_feeps_srvy_l2_electron_lat_gse]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS2_FEEPS_SRVY_L2_ION (spase://NASA/NumericalData/MMS/2/EnergeticParticleDetector/FEEPS/Survey/Level2/Ion/PT2.42S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms2_epd_feeps_srvy_l2_ion_top_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms2_epd_feeps_srvy_l2_ion_top_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms2_epd_feeps_srvy_l2_ion_top_quality_indicator_sensorid_8]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms2_epd_feeps_srvy_l2_ion_bottom_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms2_epd_feeps_srvy_l2_ion_bottom_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms2_epd_feeps_srvy_l2_ion_bottom_quality_indicator_sensorid_8]
      
      
      MMS2 FEEPS top side survey mode ion count rate sensor 6 [mms2_epd_feeps_srvy_l2_ion_top_count_rate_sensorid_6]
      
      
      MMS2 FEEPS top side survey mode ion count rate sensor 7 [mms2_epd_feeps_srvy_l2_ion_top_count_rate_sensorid_7]
      
      
      MMS2 FEEPS top side survey mode ion count rate sensor 8 [mms2_epd_feeps_srvy_l2_ion_top_count_rate_sensorid_8]
      
      
      MMS2 FEEPS bottom side survey mode ion count rate sensor 6 [mms2_epd_feeps_srvy_l2_ion_bottom_count_rate_sensorid_6]
      
      
      MMS2 FEEPS bottom side survey mode ion count rate sensor 7 [mms2_epd_feeps_srvy_l2_ion_bottom_count_rate_sensorid_7]
      
      
      MMS2 FEEPS bottom side survey mode ion count rate sensor 8 [mms2_epd_feeps_srvy_l2_ion_bottom_count_rate_sensorid_8]
      
      
      MMS2 FEEPS top side survey mode ion intensity sensor 6 [mms2_epd_feeps_srvy_l2_ion_top_intensity_sensorid_6]
      
      
      MMS2 FEEPS top side survey mode ion intensity sensor 7 [mms2_epd_feeps_srvy_l2_ion_top_intensity_sensorid_7]
      
      
      MMS2 FEEPS top side survey mode ion intensity sensor 8 [mms2_epd_feeps_srvy_l2_ion_top_intensity_sensorid_8]
      
      
      MMS2 FEEPS bottom side survey mode ion intensity sensor 6 [mms2_epd_feeps_srvy_l2_ion_bottom_intensity_sensorid_6]
      
      
      MMS2 FEEPS bottom side survey mode ion intensity sensor 7 [mms2_epd_feeps_srvy_l2_ion_bottom_intensity_sensorid_7]
      
      
      MMS2 FEEPS bottom side survey mode ion intensity sensor 8 [mms2_epd_feeps_srvy_l2_ion_bottom_intensity_sensorid_8]
      
      
      MMS2 FEEPS top side survey mode ion count error statistics sensor 6 [mms2_epd_feeps_srvy_l2_ion_top_percent_error_sensorid_6]
      
      
      MMS2 FEEPS top side survey mode ion count error statistics sensor 7 [mms2_epd_feeps_srvy_l2_ion_top_percent_error_sensorid_7]
      
      
      MMS2 FEEPS top side survey mode ion count error statistics sensor 8 [mms2_epd_feeps_srvy_l2_ion_top_percent_error_sensorid_8]
      
      
      MMS2 FEEPS bottom side survey mode ion count error statistics sensor 6 [mms2_epd_feeps_srvy_l2_ion_bottom_percent_error_sensorid_6]
      
      
      MMS2 FEEPS bottom side survey mode ion count error statistics sensor 7 [mms2_epd_feeps_srvy_l2_ion_bottom_percent_error_sensorid_7]
      
      
      MMS2 FEEPS bottom side survey mode ion count error statistics sensor 8 [mms2_epd_feeps_srvy_l2_ion_bottom_percent_error_sensorid_8]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms2_epd_feeps_srvy_l2_ion_pitch_angle]
      
      
      Latitude [mms2_epd_feeps_srvy_l2_ion_lat_gse]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS2_FGM_BRST_L2 (spase://NASA/NumericalData/MMS/2/FIELDS/FGM/Burst/Level2/PT0.0078125S)
Description
The Fluxgate Magnetometers (FGM) on Magnetospheric Multiscale consist of a
traditional Analog Fluxgate Magnetometer (AFG), and a Digital Fluxgate
magnetometer (DFG). The dual magnetometers are operated as a single instrument
providing a single intercalibrated data product. Range changes occur at
different times on the two instruments so the gains checked each periapsis can
be carried out unambiguously to apoapsis. Cross correlation of calibration
parameters can separate causes of the any apparent calibration changes. Use of
Electron Drift Instrument (EDI) to determine the field along the rotation axis
allows accurate monitoring of the zero levels along the rotation axis.  Prior to
launch the magnetometers were calibrated at the Technical University,
Braunschweig, except for the AFG magnetometers on MMS3 and MMS4, which were
calibrated at UCLA.  Both sets of sensors are operated for the entire MMS orbit,
with slow survey (8 samples per second) outside of the Region of Interest (ROI),
and fast survey (16 samples per second) inside the ROI. Within the ROI burst
mode data (128 samples per second) are also acquired.  A detailed description of
the MMS fluxgate magnetometers, including science objectives, instrument
description, calibration, magnetic cleanliness program, and data flow can be
found at http://link.springer.com/article/10.1007%2Fs11214-014-0057-3 (DOI 
10.1007/s11214-014-0057-3).Additional information can also be found at
http://www-spc.igpp.ucla.edu/ssc/mms (UCLA),and http://www.iwf.oeaw.ac.at (IWF,
Graz).
For the purpose of creating a unified FGM Level2 data product, burst mode data
is taken from DFG and survey mode data is taken from AFG.  Because AFG and DFG
are cross-calibrated on an orbit-averaged basis, small differences in offset may
be observed between Level2 burst and survey mode data.  Consequently, any
differences are within the error of the measurement. Based on preliminary
analysis of the data, the absolute error within the Region of Interest (ROI) is
estimated to be no more than 0.1 nT in the spin-plane, 0.15 nT along the
spin-axis and 0.2 nT in total magnitude.
Modification History
version X=5:  * Y-version number comes from cal file entries. 
              *
Ensures there are 2 ephemeris points before/after data to enable proper spline. 

              * Fix to depend_0 of rdeltahalf:  fixes bug when reading position
data.
              * L-vector for DMPA2GSE transformation is smoothed with a
gaussian filter, instead 
                of using a single average value for
the day.  This short-term filter avoids  
                introduding artificial
jumps at 00:00 UTC and removes 7-minute 'wobble' after  
               
maneuvers in the GSE result.   
              * Fixes error with DEFATT file
selection found when choosing the 
                daily DEFATT files to be used
in Phase 2.
              * Fixed bug where reference Etemp was used for high
range gain.  Now uses measured Etemp.
version X=4:  First version for public
release of L2.
              Renamed variables to conform with new MMS variable
name guidelines 
              (obs_instr_paramName[_coordSys]_mode_level):  
  
             Mag field parameters include 'b' for paramName.  
               
Use 'r' instead of 'pos' for S/C position paramName.  
               
Eliminated 'rate', replaced with 'bdeltahalf'.  Added 'rdeltahalf'.
            
   l1a_mode is now just 'mode'.
version X=3:  fixed removal of overlap between
modes.
              fixed a bug that caused stemp and etemp to be
empty.
version X=2:  flag parameter name corrected: was 'status'
               
        added bits 4, 5, 6 to flag saturation on B1, B2, and B3, respectively
  
                     added bit 7 to flag bad data at range changes
             
Added etemp and l1a_mode parameters.  
              rate, hirange, and stemp
parameters now comply with MMS CDF Guidlelines, e.g.
              FILLVAL now
defined for stemp and etemp, and is set to !values.f_nan
              No longer
use Var_Parents attribute in stemp -- see Parents instead
              In this
version, temperature-corrected gains are applied.  Reference temperatures are
used when 
              stemp or etemp are set to FILLVAL. 
             
Non-linearity correction is applied to high rage DFG data.
version X=1:  added
'flag', rate and hirange parameters (but 'flag' is actually called 'status')
 
  • Data Variable Descriptions
      Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (128 S/s) [mms2_fgm_b_gse_brst_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms2_fgm_b_gse_brst_l2]
      
      
      Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (128 S/s) [mms2_fgm_b_gsm_brst_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms2_fgm_b_gsm_brst_l2]
      
      
      Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (128 S/s) [mms2_fgm_b_dmpa_brst_l2_clean]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      ---> Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (128 S/s), including flagged data [mms2_fgm_b_dmpa_brst_l2]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (128 S/s) [mms2_fgm_b_bcs_brst_l2_clean]
      
      
      ---> Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (128 S/s), including flagged data [mms2_fgm_b_bcs_brst_l2]
      
      
      Quality Flag: 0 = No identified problems, non-zero = blank out the data [mms2_fgm_flag_brst_l2]
      bit definitions: .    0: TBD, 1: TBD, 2: user flagged, 3: TBD, .    4: B1
      saturated, 5: B2 saturated, 6: B3 saturated, 7: range-change glitch, .    8-31:
      TBD
      
      Definitive Position in GSE coordinates, 30 second [mms2_fgm_r_gse_brst_l2]
      
      
      Definitive Position in GSM coordinates, 30 second [mms2_fgm_r_gsm_brst_l2]
      
      
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MMS2_FGM_SRVY_L2 (spase://NASA/NumericalData/MMS/2/FIELDS/FGM/Survey/Level2/PT0.125S)
Description
The Fluxgate Magnetometers (FGM) on Magnetospheric Multiscale consist of a
traditional Analog Fluxgate Magnetometer (AFG), and a Digital Fluxgate
magnetometer (DFG). The dual magnetometers are operated as a single instrument
providing a single intercalibrated data product. Range changes occur at
different times on the two instruments so the gains checked each periapsis can
be carried out unambiguously to apoapsis. Cross correlation of calibration
parameters can separate causes of the any apparent calibration changes. Use of
Electron Drift Instrument (EDI) to determine the field along the rotation axis
allows accurate monitoring of the zero levels along the rotation axis.  Prior to
launch the magnetometers were calibrated at the Technical University,
Braunschweig, except for the AFG magnetometers on MMS3 and MMS4, which were
calibrated at UCLA.  Both sets of sensors are operated for the entire MMS orbit,
with slow survey (8 samples per second) outside of the Region of Interest (ROI),
and fast survey (16 samples per second) inside the ROI. Within the ROI burst
mode data (128 samples per second) are also acquired.  A detailed description of
the MMS fluxgate magnetometers, including science objectives, instrument
description, calibration, magnetic cleanliness program, and data flow can be
found at http://link.springer.com/article/10.1007%2Fs11214-014-0057-3 (DOI 
10.1007/s11214-014-0057-3).Additional information can also be found at
http://www-spc.igpp.ucla.edu/ssc/mms (UCLA),and http://www.iwf.oeaw.ac.at (IWF,
Graz).
For the purpose of creating a unified FGM Level2 data product, burst mode data
is taken from DFG and survey mode data is taken from AFG.  Because AFG and DFG
are cross-calibrated on an orbit-averaged basis, small differences in offset may
be observed between Level2 burst and survey mode data.  Consequently, any
differences are within the error of the measurement. Based on preliminary
analysis of the data, the absolute error within the Region of Interest (ROI) is
estimated to be no more than 0.1 nT in the spin-plane, 0.15 nT along the
spin-axis and 0.2 nT in total magnitude.
Modification History
version X=5:  * Y-version number comes from cal file entries. 
              *
Ensures there are 2 ephemeris points before/after data to enable proper spline. 

              * Fix to depend_0 of rdeltahalf:  fixes bug when reading position
data.
              * L-vector for DMPA2GSE transformation is smoothed with a
gaussian filter, instead 
                of using a single average value for
the day.  This short-term filter avoids  
                introduding artificial
jumps at 00:00 UTC and removes 7-minute 'wobble' after  
               
maneuvers in the GSE result.   
              * Fixes error with DEFATT file
selection found when choosing the 
                daily DEFATT files to be used
in Phase 2.
              * Fixed bug where reference Etemp was used for high
range gain.  Now uses measured Etemp.
version X=4:  First version for public
release of L2.
              Renamed variables to conform with new MMS variable
name guidelines 
              (obs_instr_paramName[_coordSys]_mode_level):  
  
             Mag field parameters include 'b' for paramName.  
               
Use 'r' instead of 'pos' for S/C position paramName.  
               
Eliminated 'rate', replaced with 'bdeltahalf'.  Added 'rdeltahalf'.
            
   l1a_mode is now just 'mode'.
version X=3:  fixed removal of overlap between
modes.
              fixed a bug that caused stemp and etemp to be
empty.
version X=2:  flag parameter name corrected: was 'status'
               
        added bits 4, 5, 6 to flag saturation on B1, B2, and B3, respectively
  
                     added bit 7 to flag bad data at range changes
             
Added etemp and l1a_mode parameters.  
              rate, hirange, and stemp
parameters now comply with MMS CDF Guidlelines, e.g.
              FILLVAL now
defined for stemp and etemp, and is set to !values.f_nan
              No longer
use Var_Parents attribute in stemp -- see Parents instead
              In this
version, temperature-corrected gains are applied.  Reference temperatures are
used when 
              stemp or etemp are set to FILLVAL. 
             
Non-linearity correction is applied to high rage DFG data.
version X=1:  added
'flag', rate and hirange parameters (but 'flag' is actually called 'status')
 
  • Data Variable Descriptions
      Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (8 or 16 S/s) [mms2_fgm_b_gse_srvy_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms2_fgm_b_gse_srvy_l2]
      
      
      Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (8 or 16 S/s) [mms2_fgm_b_gsm_srvy_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms2_fgm_b_gsm_srvy_l2]
      
      
      Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (8 or 16 S/s) [mms2_fgm_b_dmpa_srvy_l2_clean]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      ---> Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms2_fgm_b_dmpa_srvy_l2]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (8 or 16 S/s) [mms2_fgm_b_bcs_srvy_l2_clean]
      
      
      ---> Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms2_fgm_b_bcs_srvy_l2]
      
      
      Quality Flag: 0 = No identified problems, non-zero = blank out the data [mms2_fgm_flag_srvy_l2]
      bit definitions: .    0: TBD, 1: TBD, 2: user flagged, 3: TBD, .    4: B1
      saturated, 5: B2 saturated, 6: B3 saturated, 7: range-change glitch, .    8-31:
      TBD
      
      Definitive Position in GSE coordinates, 30 second [mms2_fgm_r_gse_srvy_l2]
      
      
      Definitive Position in GSM coordinates, 30 second [mms2_fgm_r_gsm_srvy_l2]
      
      
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MMS2_FPI_BRST_L2_DES-DIST (spase://NASA/NumericalData/MMS/2/FastPlasmaInvestigation/DES/Burst/Level2/Distribution/PT0.03S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data are taken at burst (30/150 ms for DES/DIS)
resolution in this mode.  Data are also made available at survey (4.5 s, etc)
resolution; these form a separate product from this.  Per mission design, not
all burst-resolution data are downlinked.  This product contains phase-space
distribution maps of those burst-resolution data selected for downlink.  In
particular, the (highest possible quality at the time of release)
corrected/converted "Burst SkyMap" distributions are reported with time-stamps
and other annotation characterizing the state of the instrument system at the
indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      [CDAWeb List/Download/Create ONLY] MMS2 FPI/DES burst sky-map instrument distribution [mms2_des_dist_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 10.9 eV (E1/even) [mms2_des_dist_brst1_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 12.4 eV (E1/odd) [mms2_des_dist_brst1_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~11.6 eV (E1 even-odd) [mms2_des_dist_brst1_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 10.9 eV (E1/even) [mms2_des_dist_brst1_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 12.4 eV (E1/odd) [mms2_des_dist_brst1_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 37.9 eV (E6/even) [mms2_des_dist_brst6_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 42.9 eV (E6/odd) [mms2_des_dist_brst6_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~40.4 eV (E6 even-odd) [mms2_des_dist_brst6_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 37.9 eV (E6/even) [mms2_des_dist_brst6_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 42.9 eV (E6/odd) [mms2_des_dist_brst6_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 80.0 eV (E9/even) [mms2_des_dist_brst9_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 90.6 eV (E9/odd) [mms2_des_dist_brst9_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~85 eV (E9 even-odd) [mms2_des_dist_brst9_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 80.0 eV (E9/even) [mms2_des_dist_brst9_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 90.6 eV (E9/odd) [mms2_des_dist_brst9_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 169 eV (E12/even) [mms2_des_dist_brst12_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 191 eV (E12/odd) [mms2_des_dist_brst12_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~180 eV (E12 even-odd) [mms2_des_dist_brst12_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 169 eV (E12/even) [mms2_des_dist_brst12_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 191 eV (E12/odd) [mms2_des_dist_brst12_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 277 eV (E14/even) [mms2_des_dist_brst14_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 314 eV (E14/odd) [mms2_des_dist_brst14_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~295 eV (E14 even-odd) [mms2_des_dist_brst14_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 277 eV (E14/even) [mms2_des_dist_brst14_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 314 eV (E14/odd) [mms2_des_dist_brst14_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 456 eV (E16/even) [mms2_des_dist_brst16_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 517 eV (E16/odd) [mms2_des_dist_brst16_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~485 eV (E16 even-odd) [mms2_des_dist_brst16_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 456 eV (E16/even) [mms2_des_dist_brst16_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 517 eV (E16/odd) [mms2_des_dist_brst16_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 750 eV (E18/even) [mms2_des_dist_brst18_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 850 eV (E18/odd) [mms2_des_dist_brst18_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~800 eV (E18 even-odd) [mms2_des_dist_brst18_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 750 eV (E18/even) [mms2_des_dist_brst18_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 850 eV (E18/odd) [mms2_des_dist_brst18_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 1230 eV (E20/even) [mms2_des_dist_brst20_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 1400 eV (E20/odd) [mms2_des_dist_brst20_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~1310 eV (E20 even-odd) [mms2_des_dist_brst20_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1230 eV (E20/even) [mms2_des_dist_brst20_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1400 eV (E20/odd) [mms2_des_dist_brst20_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 2600 eV (E23/even) [mms2_des_dist_brst23_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 2950 eV (E23/odd) [mms2_des_dist_brst23_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~2770 eV (E23 even-odd) [mms2_des_dist_brst23_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2600 eV (E23/even) [mms2_des_dist_brst23_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2950 eV (E23/odd) [mms2_des_dist_brst23_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 5490 eV (E26/even) [mms2_des_dist_brst26_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 6210 eV (E26/odd) [mms2_des_dist_brst26_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~5840 eV (E26 even-odd) [mms2_des_dist_brst26_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5490 eV (E26/even) [mms2_des_dist_brst26_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 6210 eV (E26/odd) [mms2_des_dist_brst26_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 24400 eV (E32/even) [mms2_des_dist_brst32_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES burst sky-map instrument distribution - 27600 eV (E32/odd) [mms2_des_dist_brst32_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~26000 eV (E32 even-odd) [mms2_des_dist_brst32_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 24400 eV (E32/even) [mms2_des_dist_brst32_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 27600 eV (E32/odd) [mms2_des_dist_brst32_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [List/Create only in CDAWeb] 1-sigma error: MMS2 FPI/DES burst sky-map instrument distribution [mms2_des_disterr_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES vector of data-quality indicators at burst-start time [mms2_des_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS2 FPI/DES compression lossless/lossy indicator at survey-start time [mms2_des_compressionloss_brst]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS2 FPI/DES step table parity, this burst [mms2_des_steptable_parity_brst]
      FPI/DES alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS2 FPI/DES Del-Phi (obs spin-phase) count at burst-start time [mms2_des_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS2 FPI/DES Del-Phi (obs spin-phase) angle at burst-start time [mms2_des_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS2 FPI/DES burst average f1 count values [mms2_des_avgf1counts_brst]
      Average f1-count level as a function of energy
      
      MMS2 FPI/DES burst sky-map microsecond offsets from Epoch [mms2_des_steptimeoffsets_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order. Offsets reflect 128 steps over the 30 msec sweep
      period. See FPI docs for details.
      
      ---> MMS2 FPI/DES sector de-Spin P value, this burst [mms2_des_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS2 FPI/DES burst sky-map instrument azimuthal angles [mms2_des_phi_brst]
      see FPI docs for details
      
      MMS FPI/DES burst sky-map parity 0/1 energies [mms2_des_energy_brst]
      Energies (parity 0/1) in the 64-step FPI energy table
      
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MMS2_FPI_BRST_L2_DES-MOMS (spase://NASA/NumericalData/MMS/2/FastPlasmaInvestigation/DES/Burst/Level2/Moments/PT0.03S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode.  Data are also made available at survey (4.5
s, etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked.  Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available.  This product contains results from
integrating the standard moments of phase-space distributions formed from the
indicated data type (DES/DIS burst, FS or SS).  For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DES 32-bit vector of data-quality indicators at burst-start time [mms2_des_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>25%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied
      
      ---> MMS2 FPI/DES compression lossless/lossy indicator at survey-start time [mms2_des_compressionloss_brst]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS2 FPI/DES step table parity, this burst [mms2_des_steptable_parity_brst]
      FPI/DES alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS2 FPI/DES Del-Phi (obs spin-phase) count at burst-start time [mms2_des_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS2 FPI/DES Del-Phi (obs spin-phase) angle at burst-start time [mms2_des_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      ---> MMS2 FPI/DES sector de-Spin P value, this burst [mms2_des_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS2 FPI/DES electron pitch-angle distribution for "low" energies during this burst [mms2_des_pitchangdist_lowen_brst]
      low energy bin: 0 eV - 200 eV.  pitch-angle bin size: 6 deg.
      
      ---> MMS2 FPI/DES electron pitch-angle distribution for "mid" energies during this burst [mms2_des_pitchangdist_miden_brst]
      mid energy bin: 200 eV - 2 keV.  pitch-angle bin size: 6 deg.
      
      ---> MMS2 FPI/DES electron pitch-angle distribution for "high" energies during this burst [mms2_des_pitchangdist_highen_brst]
      high energy bin: 2 keV - 30 keV.  pitch-angle bin size: 6 deg.
      
      MMS2 FPI/DES electron energy spectrum "near" +X_DSC during this burst [mms2_des_energyspectr_px_brst]
      Counts, summed over DSC velocity-dirs closest to +X_DSC, by energy bin.
      
      ---> MMS2 FPI/DES electron energy spectrum "near" -X_DSC during this burst [mms2_des_energyspectr_mx_brst]
      Counts, summed over DSC velocity-dirs closest to -X_DSC, by energy bin.
      
      ---> MMS2 FPI/DES electron energy spectrum "near" +Y_DSC during this burst [mms2_des_energyspectr_py_brst]
      Counts, summed over DSC velocity-dirs closest to +Y_DSC, by energy bin.
      
      ---> MMS2 FPI/DES electron energy spectrum "near" -Y_DSC during this burst [mms2_des_energyspectr_my_brst]
      Counts, summed over DSC velocity-dirs closest to -Y_DSC, by energy bin.
      
      ---> MMS2 FPI/DES electron energy spectrum "near" +Z_DSC during this burst [mms2_des_energyspectr_pz_brst]
      Counts, summed over DSC velocity-dirs closest to +Z_DSC, by energy bin.
      
      ---> MMS2 FPI/DES electron energy spectrum "near" -Z_DSC during this burst [mms2_des_energyspectr_mz_brst]
      Counts, summed over DSC velocity-dirs closest to -Z_DSC, by energy bin.
      
      MMS2 FPI/DES electron energy parallel spectrum 30 degrees parallel to B during this burst [mms2_des_energyspectr_par_brst]
      Counts, summed within 30 degrees parallel bentPipe magnetic field.
      
      ---> MMS2 FPI/DES electron energy anti-parallel spectrum 30 degrees anti-parallel to B during this burst [mms2_des_energyspectr_anti_brst]
      Counts, summed within 30 degrees antiparallel to bentPipe magnetic field.
      
      ---> MMS2 FPI/DES electron energy perpendicular spectrum 60 degrees perpendicular to B during this burst [mms2_des_energyspectr_perp_brst]
      Counts, summed within 60 degrees perpendicular to bentPipe magnetic field.
      
      MMS2 FPI/DES omni-directional electron energy spectrum during this burst [mms2_des_energyspectr_omni_brst]
      Differential energy flux, averaged (weighted by solid angle) over all look
      directions, by energy bin.
      
      MMS2 FPI/DES electron number density during this burst [mms2_des_numberdensity_brst]
      
      
      ---> (no error bars displayed) MMS2 FPI/DES electron number density during this burst [mms2_des_numberdensity_brst_noerr]
      
      
      ---> MMS2 FPI/DES electron number density error during this burst [mms2_des_numberdensity_err_brst]
      
      
      MMS2 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms2_des_densityextrapolation_low_brst]
      
      
      MMS2 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms2_des_densityextrapolation_high_brst]
      
      
      MMS2 FPI/DES electron bulk-velocity DBCS vector during this burst [mms2_des_bulkv_dbcs_brst]
      
      
      MMS2 FPI/DES electron bulk-velocity estimated spintone vector in DBCS during this burst [mms2_des_bulkv_spintone_dbcs_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS2 FPI/DES electron bulk-velocity DBCS vector during this burst [mms2_des_bulkv_dbcs_brst_noerr]
      
      
      MMS2 FPI/DES electron bulk-velocity GSE vector during this burst [mms2_des_bulkv_gse_brst]
      
      
      MMS2 FPI/DES electron bulk-velocity estimated spintone vector in GSE during this burst [mms2_des_bulkv_spintone_gse_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS2 FPI/DES electron bulk-velocity GSE vector during this burst [mms2_des_bulkv_gse_brst_noerr]
      
      
      MMS2 FPI/DES electron bulk-velocity spintone vector in DBCS during this burst [mms2_des_bulkv_spin_dbcs_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS2 FPI/DES electron bulk-velocity spintone vector in GSE during this burst [mms2_des_bulkv_spin_gse_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS2 FPI/DES electron pressure tensor DBCS matrix during this burst [mms2_des_prestensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES electron pressure tensor GSE matrix during this burst [mms2_des_prestensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES electron temperature tensor DBCS matrix during this burst [mms2_des_temptensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES electron temperature tensor GSE matrix during this burst [mms2_des_temptensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES electron heat-flux DBCS vector during this burst [mms2_des_heatq_dbcs_brst]
      
      
      MMS2 FPI/DES electron heat-flux GSE vector during this burst [mms2_des_heatq_gse_brst]
      
      
      MMS2 FPI/DES electron parallel temperature during this BP [mms2_des_temppara_brst]
      
      
      MMS2 FPI/DES electron perpendicular temperature during this BP [mms2_des_tempperp_brst]
      
      
Dataset in CDAWeb
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MMS2_FPI_BRST_L2_DES-PARTMOMS (spase://NASA/NumericalData/MMS/2/FastPlasmaInvestigation/DES/Burst/Level2/PartialMoments/PT0.03S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s,
etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked. Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available. This product contains partial moments that
come from performing the standard moment integrals over a limited portion of
velocity space. The resulting quantities are named similarly to their
corresponding standard moments, but are decorated with 'part' to differentiate.
For example, density_part is the density moment integrated from a particular
energy step to infinity. These partial moments are formed from the indicated
data type (DES/DIS burst, FS or SS). For convenience, some additional parameters
are included to augment those most commonly found in a moments product of this
sort, plus time-stamps and other annotation characterizing the state of the
instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DES vector of data-quality indicators at burst-start time [mms2_des_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only)
      
      MMS2 FPI/DES partial electron number density during this burst [mms2_des_numberdensity_part_brst]
      
      
      MMS2 FPI/DES partial electron bulk-velocity vector in DBCS during this burst [mms2_des_bulkv_part_dbcs_brst]
      
      
      MMS2 FPI/DES partial electron bulk-velocity vector in GSE during this burst [mms2_des_bulkv_part_gse_brst]
      
      
      MMS2 FPI/DES partial electron pressure tensor in DBCS during this burst [mms2_des_prestensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES partial electron pressure tensor in GSE during this burst [mms2_des_prestensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES partial electron temperature tensor in DBCS during this burst [mms2_des_temptensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES partial electron temperature tensor in GSE during this burst [mms2_des_temptensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES partial electron parallel temperature during this burst [mms2_des_temppara_part_brst]
      
      
      MMS2 FPI/DES partial electron perpendicular temperature during this burst [mms2_des_tempperp_part_brst]
      
      
      MMS2 FPI/DES recommended energy index during this burst [mms2_des_part_index_brst]
      Recommended energy index during this burst
      
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MMS2_FPI_BRST_L2_DIS-DIST (spase://NASA/NumericalData/MMS/2/FastPlasmaInvestigation/DIS/Burst/Level2/Distribution/PT0.15S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data are taken at burst (30/150 ms for DES/DIS)
resolution in this mode.  Data are also made available at survey (4.5 s, etc)
resolution; these form a separate product from this.  Per mission design, not
all burst-resolution data are downlinked.  This product contains phase-space
distribution maps of those burst-resolution data selected for downlink.  In
particular, the (highest possible quality at the time of release)
corrected/converted "Burst SkyMap" distributions are reported with time-stamps
and other annotation characterizing the state of the instrument system at the
indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      [CDAWeb List/Download/Create ONLY] MMS2 FPI/DIS burst sky-map instrument distribution [mms2_dis_dist_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 10.6 eV (E1/even) [mms2_dis_dist_brst1_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 12.0 eV (E1/odd) [mms2_dis_dist_brst1_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~11.3 eV (E1 even-odd) [mms2_dis_dist_brst1_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 10.6 eV (E1/even) [mms2_dis_dist_brst1_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 12.0 eV (E1/odd) [mms2_dis_dist_brst1_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 37.2 eV (E6/even) [mms2_dis_dist_brst6_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 42.1 eV (E6/odd) [mms2_dis_dist_brst6_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~39.6 eV (E6 even-odd) [mms2_dis_dist_brst6_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 37.2 eV (E6/even) [mms2_dis_dist_brst6_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 42.1 eV (E6/odd) [mms2_dis_dist_brst6_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 78.8 eV (E9/even) [mms2_dis_dist_brst9_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 89.3 eV (E9/odd) [mms2_dis_dist_brst9_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~83.9 eV (E9 even-odd) [mms2_dis_dist_brst9_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 78.8 eV (E9/even) [mms2_dis_dist_brst9_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 89.3 eV (E9/odd) [mms2_dis_dist_brst9_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 167 eV (E12/even) [mms2_dis_dist_brst12_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 189 eV (E12/odd) [mms2_dis_dist_brst12_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~178 eV (E12 even-odd) [mms2_dis_dist_brst12_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 167 eV (E12/even) [mms2_dis_dist_brst12_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 189 eV (E12/odd) [mms2_dis_dist_brst12_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 275 eV (E14/even) [mms2_dis_dist_brst14_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 312 eV (E14/odd) [mms2_dis_dist_brst14_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~293 eV (E14 even-odd) [mms2_dis_dist_brst14_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 275 eV (E14/even) [mms2_dis_dist_brst14_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 312 eV (E14/odd) [mms2_dis_dist_brst14_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 455 eV (E16/even) [mms2_dis_dist_brst16_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 515 eV (E16/odd) [mms2_dis_dist_brst16_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~484 eV (E16 even-odd) [mms2_dis_dist_brst16_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 455 eV (E16/even) [mms2_dis_dist_brst16_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 515 eV (E16/odd) [mms2_dis_dist_brst16_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 750 eV (E18/even) [mms2_dis_dist_brst18_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 850 eV (E18/odd) [mms2_dis_dist_brst18_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~800 eV (E18 even-odd) [mms2_dis_dist_brst18_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 750 eV (E18/even) [mms2_dis_dist_brst18_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 850 eV (E18/odd) [mms2_dis_dist_brst18_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 1240 eV (E20/even) [mms2_dis_dist_brst20_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 1400 eV (E20/odd) [mms2_dis_dist_brst20_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~1320 eV (E20 even-odd) [mms2_dis_dist_brst20_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1240 eV (E20/even) [mms2_dis_dist_brst20_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1400 eV (E20/odd) [mms2_dis_dist_brst20_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 2620 eV (E23/even) [mms2_dis_dist_brst23_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 2970 eV (E23/odd) [mms2_dis_dist_brst23_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~2800 eV (E23 even-odd) [mms2_dis_dist_brst23_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2620 eV (E23/even) [mms2_dis_dist_brst23_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2970 eV (E23/odd) [mms2_dis_dist_brst23_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 5560 eV (E26/even) [mms2_dis_dist_brst26_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 6300 eV (E26/odd) [mms2_dis_dist_brst26_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~5920 eV (E26 even-odd) [mms2_dis_dist_brst26_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5560 eV (E26/even) [mms2_dis_dist_brst26_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 6300 eV (E26/odd) [mms2_dis_dist_brst26_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 25000 eV (E32/even) [mms2_dis_dist_brst32_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS burst sky-map instrument distribution - 28300 eV (E32/odd) [mms2_dis_dist_brst32_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~26600 eV (E32 even-odd) [mms2_dis_dist_brst32_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 25000 eV (E32/even) [mms2_dis_dist_brst32_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 28300 eV (E32/odd) [mms2_dis_dist_brst32_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [List/Create only in CDAWeb] 1-sigma error: MMS2 FPI/DIS burst sky-map instrument distribution [mms2_dis_disterr_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS vector of data-quality indicators at burst-start time [mms2_dis_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS2 FPI/DIS compression lossless/lossy indicator at survey-start time [mms2_dis_compressionloss_brst]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS2 FPI/DIS step table parity, this burst [mms2_dis_steptable_parity_brst]
      FPI/DIS alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS2 FPI/DIS Del-Phi (obs spin-phase) count at burst-start time [mms2_dis_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS2 FPI/DIS Del-Phi (obs spin-phase) angle at burst-start time [mms2_dis_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS2 FPI/DIS burst average f1 count values [mms2_dis_avgf1counts_brst]
      Average f1-count level as a function of energy
      
      MMS2 FPI/DIS burst sky-map microsecond offsets from Epoch [mms2_dis_steptimeoffsets_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order. Offsets reflect 128 steps over the 150 msec sweep
      period. See FPI docs for details.
      
      ---> MMS2 FPI/DIS sector de-Spin P value, this burst [mms2_dis_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS2 FPI/DIS burst sky-map instrument azimuthal angles [mms2_dis_phi_brst]
      see FPI docs for details
      
      MMS FPI/DIS burst sky-map parity 0/1 energies [mms2_dis_energy_brst]
      Energies (parity 0/1) in the 64-step FPI energy table
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS2_FPI_BRST_L2_DIS-MOMS (spase://NASA/NumericalData/MMS/2/FastPlasmaInvestigation/DIS/Burst/Level2/Moments/PT0.15S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode.  Data are also made available at survey (4.5
s, etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked.  Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available.  This product contains results from
integrating the standard moments of phase-space distributions formed from the
indicated data type (DES/DIS burst, FS or SS).  For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DIS 32-bit vector of data-quality indicators at burst-start time [mms2_dis_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>25%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied
      
      ---> MMS2 FPI/DIS compression lossless/lossy indicator at survey-start time [mms2_dis_compressionloss_brst]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS2 FPI/DIS step table parity, this burst [mms2_dis_steptable_parity_brst]
      FPI/DIS alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS2 FPI/DIS Del-Phi (obs spin-phase) count at burst-start time [mms2_dis_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS2 FPI/DIS Del-Phi (obs spin-phase) angle at burst-start time [mms2_dis_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      ---> MMS2 FPI/DIS sector de-Spin P value, this burst [mms2_dis_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS2 FPI/DIS ion energy spectrum "near" +X_DSC during this burst [mms2_dis_energyspectr_px_brst]
      Counts, summed over DSC velocity-dirs closest to +X_DSC, by energy bin.
      
      ---> MMS2 FPI/DIS ion energy spectrum "near" -X_DSC during this burst [mms2_dis_energyspectr_mx_brst]
      Counts, summed over DSC velocity-dirs closest to -X_DSC, by energy bin.
      
      ---> MMS2 FPI/DIS ion energy spectrum "near" +Y_DSC during this burst [mms2_dis_energyspectr_py_brst]
      Counts, summed over DSC velocity-dirs closest to +Y_DSC, by energy bin.
      
      ---> MMS2 FPI/DIS ion energy spectrum "near" -Y_DSC during this burst [mms2_dis_energyspectr_my_brst]
      Counts, summed over DSC velocity-dirs closest to -Y_DSC, by energy bin.
      
      ---> MMS2 FPI/DIS ion energy spectrum "near" +Z_DSC during this burst [mms2_dis_energyspectr_pz_brst]
      Counts, summed over DSC velocity-dirs closest to +Z_DSC, by energy bin.
      
      ---> MMS2 FPI/DIS ion energy spectrum "near" -Z_DSC during this burst [mms2_dis_energyspectr_mz_brst]
      Counts, summed over DSC velocity-dirs closest to -Z_DSC, by energy bin.
      
      MMS2 FPI/DIS omni-directional ion energy spectrum during this burst [mms2_dis_energyspectr_omni_brst]
      Differential energy flux, averaged (weighted by solid angle) over all look
      directions, by energy bin.
      
      MMS2 FPI/DIS ion background energy during this burst [mms2_dis_spectr_bg_brst]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look) background level.
      
      MMS2 FPI/DIS ion background number density during this burst [mms2_dis_numberdensity_bg_brst]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS2 FPI/DIS ion number density during this burst [mms2_dis_numberdensity_brst]
      
      
      ---> (no error bars displayed) MMS2 FPI/DIS ion number density during this burst [mms2_dis_numberdensity_brst_noerr]
      
      
      ---> MMS2 FPI/DIS ion number density error during this burst [mms2_dis_numberdensity_err_brst]
      
      
      MMS2 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms2_dis_densityextrapolation_low_brst]
      
      
      MMS2 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms2_dis_densityextrapolation_high_brst]
      
      
      MMS2 FPI/DIS ion bulk-velocity DBCS vector during this burst [mms2_dis_bulkv_dbcs_brst]
      
      
      MMS2 FPI/DIS ion bulk-velocity estimated spintone vector in DBCS during this burst [mms2_dis_bulkv_spintone_dbcs_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS2 FPI/DIS ion bulk-velocity DBCS vector during this burst [mms2_dis_bulkv_dbcs_brst_noerr]
      
      
      MMS2 FPI/DIS ion bulk-velocity GSE vector during this burst [mms2_dis_bulkv_gse_brst]
      
      
      MMS2 FPI/DIS ion bulk-velocity estimated spintone vector in GSE during this burst [mms2_dis_bulkv_spintone_gse_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS2 FPI/DIS ion bulk-velocity GSE vector during this burst [mms2_dis_bulkv_gse_brst_noerr]
      
      
      MMS2 FPI/DIS ion bulk-velocity spintone vector in DBCS during this burst [mms2_dis_bulkv_spin_dbcs_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS2 FPI/DIS ion bulk-velocity spintone vector in GSE during this burst [mms2_dis_bulkv_spin_gse_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS2 FPI/DIS ion pressure tensor DBCS matrix during this burst [mms2_dis_prestensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS ion pressure tensor GSE matrix during this burst [mms2_dis_prestensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS ion background pressure during this survey [mms2_dis_pres_bg_brst]
      
      
      MMS2 FPI/DIS ion temperature tensor DBCS matrix during this burst [mms2_dis_temptensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS ion temperature tensor GSE matrix during this burst [mms2_dis_temptensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS ion heat-flux DBCS vector during this burst [mms2_dis_heatq_dbcs_brst]
      
      
      MMS2 FPI/DIS ion heat-flux GSE vector during this burst [mms2_dis_heatq_gse_brst]
      
      
      MMS2 FPI/DIS ion parallel temperature during this BP [mms2_dis_temppara_brst]
      
      
      MMS2 FPI/DIS ion perpendicular temperature during this BP [mms2_dis_tempperp_brst]
      
      
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MMS2_FPI_BRST_L2_DIS-PARTMOMS (spase://NASA/NumericalData/MMS/2/FastPlasmaInvestigation/DIS/Burst/Level2/PartialMoments/PT0.15S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s,
etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked. Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available. This product contains partial moments that
come from performing the standard moment integrals over a limited portion of
velocity space. The resulting quantities are named similarly to their
corresponding standard moments, but are decorated with 'part' to differentiate.
For example, density_part is the density moment integrated from a particular
energy step to infinity. These partial moments are formed from the indicated
data type (DES/DIS burst, FS or SS). For convenience, some additional parameters
are included to augment those most commonly found in a moments product of this
sort, plus time-stamps and other annotation characterizing the state of the
instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DIS vector of data-quality indicators at burst-start time [mms2_dis_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation
      
      MMS2 FPI/DIS partial ion number density during this burst [mms2_dis_numberdensity_part_brst]
      
      
      MMS2 FPI/DIS partial ion bulk-velocity vector in DBCS during this burst [mms2_dis_bulkv_part_dbcs_brst]
      
      
      MMS2 FPI/DIS partial ion bulk-velocity vector in GSE during this burst [mms2_dis_bulkv_part_gse_brst]
      
      
      MMS2 FPI/DIS partial ion pressure tensor in DBCS during this burst [mms2_dis_prestensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS partial ion pressure tensor in GSE during this burst [mms2_dis_prestensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS partial ion temperature tensor in DBCS during this burst [mms2_dis_temptensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS partial ion temperature tensor in GSE during this burst [mms2_dis_temptensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS partial ion parallel temperature during this burst [mms2_dis_temppara_part_brst]
      
      
      MMS2 FPI/DIS partial ion perpendicular temperature during this burst [mms2_dis_tempperp_part_brst]
      
      
      MMS2 FPI/DIS recommended energy index during this burst [mms2_dis_part_index_brst]
      Recommended energy index during this burst
      
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MMS2_FPI_FAST_L2_DES-DIST (spase://NASA/NumericalData/MMS/2/FastPlasmaInvestigation/DES/Fast/Level2/Distribution/PT4.5S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data taken at burst (30/150 ms for DES/DIS)
resolution are aggregated on board and made available at survey (4.5 s)
resolution in this mode.  This product contains phase-space distribution maps of
results from surveying the high-resolution observations during each 4.5 s
period.  In particular, the (highest possible quality at the time of release)
corrected/converted "Fast Survey SkyMap" distributions are reported with
time-stamps and other annotation characterizing the state of the instrument
system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DES fast sky-map instrument distribution - 11.6 eV (E1) using averaged even/odd steps [mms2_des_dist_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 11.6 eV [mms2_des_dist_fast1_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES fast sky-map instrument distribution - 40.4 eV (E6) using averaged even/odd steps [mms2_des_dist_fast6]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 40.4 eV [mms2_des_dist_fast6_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES fast sky-map instrument distribution - 85.1 eV (E9) using averaged even/odd steps [mms2_des_dist_fast9]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 85.1 eV [mms2_des_dist_fast9_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES fast sky-map instrument distribution - 179 eV (E12) using averaged even/odd steps [mms2_des_dist_fast12]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 179 eV [mms2_des_dist_fast12_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES fast sky-map instrument distribution - 295 eV (E14) using averaged even/odd steps [mms2_des_dist_fast14]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 295 eV [mms2_des_dist_fast14_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES fast sky-map instrument distribution - 485 eV (E16) using averaged even/odd steps [mms2_des_dist_fast16]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 485 eV [mms2_des_dist_fast16_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES fast sky-map instrument distribution - 798 eV (E18) using averaged even/odd steps [mms2_des_dist_fast18]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 798 eV [mms2_des_dist_fast18_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES fast sky-map instrument distribution - 1310 eV (E20) using averaged even/odd steps [mms2_des_dist_fast20]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1310 eV [mms2_des_dist_fast20_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES fast sky-map instrument distribution - 2770 eV (E23) using averaged even/odd steps [mms2_des_dist_fast23]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2770 eV [mms2_des_dist_fast23_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES fast sky-map instrument distribution - 5840 eV (E26) using averaged even/odd steps [mms2_des_dist_fast26]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5840 eV [mms2_des_dist_fast26_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES fast sky-map instrument distribution - 26000 eV (E32) using averaged even/odd steps [mms2_des_dist_fast32]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 26000 eV [mms2_des_dist_fast32_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [Only List/Create in CDAWeb] MMS2 FPI/DES fast sky-map instrument distribution 1-sigma error [mms2_des_disterr_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES vector of data-quality indicators at fast survey-start time - 32-bit error flags [mms2_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS2 FPI/DES compression lossless/lossy indicator at survey-start time [mms2_des_compressionloss_fast]
      FPI/DES compression loss indicator,0=lossless, 1=lossy
      
      ---> MMS2 FPI/DES Del-Phi (obs spin-phase) count at fast survey-start time [mms2_des_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS2 FPI/DES Del-Phi (obs spin-phase) angle at fast survey-start time [mms2_des_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS2 FPI/DES fast survey average f1 count values [mms2_des_avgf1counts_fast]
      Average f1-count level as a function of energy
      
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MMS2_FPI_FAST_L2_DES-MOMS (spase://NASA/NumericalData/MMS/2/FastPlasmaInvestigation/DES/Fast/Level2/Moments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution.  Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This moments product
contains results from integrating the standard moments of phase-space
distributions formed from the indicated data type (DES/DIS burst, FS or SS). For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotation characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DES 32-bit vector of data-quality indicators at survey-start time [mms2_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>25%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied
      
      ---> MMS2 FPI/DES compression lossless/lossy indicator at survey-start time [mms2_des_compressionloss_fast]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS2 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms2_des_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS2 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms2_des_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS2 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms2_des_pitchangdist_lowen_fast]
      low energy bin: 0 eV - 200 eV.  pitch-angle bin size: 6 deg.
      
      ---> MMS2 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms2_des_pitchangdist_miden_fast]
      mid energy bin: 200 eV - 2 keV.  pitch-angle bin size: 6 deg.
      
      ---> MMS2 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms2_des_pitchangdist_highen_fast]
      high energy bin: 2 keV - 30 keV.  pitch-angle bin size: 6 deg.
      
      MMS2 FPI/DES electron energy spectrum "near" +X_DSC during this survey [mms2_des_energyspectr_px_fast]
      Counts, summed over DSC velocity-dirs closest to +X_DSC, by energy bin.
      
      ---> MMS2 FPI/DES electron energy spectrum "near" -X_DSC during this survey [mms2_des_energyspectr_mx_fast]
      Counts, summed over DSC velocity-dirs closest to -X_DSC, by energy bin.
      
      ---> MMS2 FPI/DES electron energy spectrum "near" +Y_DSC during this survey [mms2_des_energyspectr_py_fast]
      Counts, summed over DSC velocity-dirs closest to +Y_DSC, by energy bin.
      
      ---> MMS2 FPI/DES electron energy spectrum "near" -Y_DSC during this survey [mms2_des_energyspectr_my_fast]
      Counts, summed over DSC velocity-dirs closest to -Y_DSC, by energy bin.
      
      ---> MMS2 FPI/DES electron energy spectrum "near" +Z_DSC during this survey [mms2_des_energyspectr_pz_fast]
      Counts, summed over DSC velocity-dirs closest to +Z_DSC, by energy bin.
      
      ---> MMS2 FPI/DES electron energy spectrum "near" -Z_DSC during this survey [mms2_des_energyspectr_mz_fast]
      Counts, summed over DSC velocity-dirs closest to -Z_DSC, by energy bin.
      
      MMS2 FPI/DES electron energy parallel spectrum 30 degrees parallel to B during this survey [mms2_des_energyspectr_par_fast]
      Counts, summed within 30 degrees parallel bentPipe magnetic field.
      
      ---> MMS2 FPI/DES electron energy anti-parallel spectrum 30 degrees anti-parallel to B during this survey [mms2_des_energyspectr_anti_fast]
      Counts, summed within 30 degrees antiparallel to bentPipe magnetic field.
      
      ---> MMS2 FPI/DES electron energy perpendicular spectrum 60 degrees perpendicular to B during this survey [mms2_des_energyspectr_perp_fast]
      Counts, summed within 60 degrees perpendicular to bentPipe magnetic field.
      
      MMS2 FPI/DES omni-directional electron energy spectrum during this survey [mms2_des_energyspectr_omni_fast]
      Differential energy flux, averaged (weighted by solid angle) over all look
      directions, by energy bin.
      
      MMS2 FPI/DES electron number density during this survey [mms2_des_numberdensity_fast]
      
      
      ---> (no error bars displayed) MMS2 FPI/DES electron number density during this survey [mms2_des_numberdensity_fast_noerr]
      
      
      ---> MMS2 FPI/DES electron number density error during this survey [mms2_des_numberdensity_err_fast]
      
      
      MMS2 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms2_des_densityextrapolation_low_fast]
      
      
      MMS2 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms2_des_densityextrapolation_high_fast]
      
      
      MMS2 FPI/DES electron bulk-velocity DBCS vector during this survey [mms2_des_bulkv_dbcs_fast]
      
      
      MMS2 FPI/DES electron bulk-velocity estimated spintone vector in DBCS during this survey [mms2_des_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS2 FPI/DES electron bulk-velocity DBCS vector during this survey [mms2_des_bulkv_dbcs_fast_noerr]
      
      
      MMS2 FPI/DES electron bulk-velocity GSE vector during this survey [mms2_des_bulkv_gse_fast]
      
      
      MMS2 FPI/DES electron bulk-velocity estimated spintone vector in GSE during this survey [mms2_des_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS2 FPI/DES electron bulk-velocity GSE vector during this survey [mms2_des_bulkv_gse_fast_noerr]
      
      
      MMS2 FPI/DES electron bulk-velocity spintone vector in DBCS during this survey [mms2_des_bulkv_spin_dbcs_fast]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS2 FPI/DES electron bulk-velocity spintone vector in GSE during this survey [mms2_des_bulkv_spin_gse_fast]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS2 FPI/DES electron pressure tensor DBCS matrix during this survey [mms2_des_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES electron pressure tensor GSE matrix during this survey [mms2_des_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES electron temperature tensor DBCS matrix during this survey [mms2_des_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES electron temperature tensor GSE matrix during this survey [mms2_des_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES electron heat-flux DBCS vector during this survey [mms2_des_heatq_dbcs_fast]
      
      
      MMS2 FPI/DES electron heat-flux GSE vector during this survey [mms2_des_heatq_gse_fast]
      
      
      MMS2 FPI/DES electron parallel temperature during this BP [mms2_des_temppara_fast]
      
      
      MMS2 FPI/DES electron perpendicular temperature during this BP [mms2_des_tempperp_fast]
      
      
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MMS2_FPI_FAST_L2_DES-MOMSAUX
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DES vector of data-quality indicators at survey-start time [mms2_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only)
      
      MMS2 FPI/DES partial electron number density during this survey [mms2_des_numberdensity_part_fast]
      
      
      MMS2 FPI/DES partial electron bulk-velocity vector in DBCS during this survey [mms2_des_bulkv_part_dbcs_fast]
      
      
      MMS2 FPI/DES partial electron bulk-velocity vector in GSE during this survey [mms2_des_bulkv_part_gse_fast]
      
      
      MMS2 FPI/DES partial electron pressure tensor in DBCS during this survey [mms2_des_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES partial electron pressure tensor in GSE during this survey [mms2_des_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES partial electron temperature tensor in DBCS during this survey [mms2_des_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES partial electron temperature tensor in GSE during this survey [mms2_des_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES partial electron parallel temperature during this survey [mms2_des_temppara_part_fast]
      
      
      MMS2 FPI/DES partial electron perpendicular temperature during this survey [mms2_des_tempperp_part_fast]
      
      
      MMS2 FPI/DES recommended energy index for partial moments during this survey [mms2_des_part_index_fast]
      Recommended energy index during this survey
      
      MMS2 FPI/DES compression lossless/lossy indicator at survey-start time [mms2_des_compressionloss_fast]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS2 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms2_des_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS2 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms2_des_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS2 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms2_des_pitchangdist_lowen_fast]
      Low energy bin: energy steps 0-10 (of total steps 0-31). Pitch-angle bin size: 6
      deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS2 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms2_des_pitchangdist_miden_fast]
      Mid energy bin: energy steps 11-20 (of total steps 0-31). Pitch-angle bin size:
      6 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS2 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms2_des_pitchangdist_highen_fast]
      High energy bin: energy steps 21-31 (of total steps 0-31). Pitch-angle bin size:
      6 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS2 FPI/DES electron energy spectrum "near" +X_DBCS during this survey [mms2_des_energyspectr_px_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS2 FPI/DES electron energy spectrum "near" -X_DBCS during this survey [mms2_des_energyspectr_mx_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS2 FPI/DES electron energy spectrum "near" +Y_DBCS during this survey [mms2_des_energyspectr_py_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS2 FPI/DES electron energy spectrum "near" -Y_DBCS during this survey [mms2_des_energyspectr_my_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS2 FPI/DES electron energy spectrum "near" +Z_DBCS during this survey [mms2_des_energyspectr_pz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS2 FPI/DES electron energy spectrum "near" -Z_DBCS during this survey [mms2_des_energyspectr_mz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS2 FPI/DES electron energy parallel to the magnetic field direction during this survey [mms2_des_energyspectr_par_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within 30
      degrees of the magnetic field direction.
      
      MMS2 FPI/DES electron energy anti-parallel to the magnetic field direction during this survey [mms2_des_energyspectr_anti_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      150 degrees of the magnetic field direction.
      
      MMS2 FPI/DES electron energy perpendicular to the magnetic field direction during this survey [mms2_des_energyspectr_perp_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      60-120 degrees of the magnetic field direction.
      
      MMS2 FPI/DES omni-directional electron energy spectrum during this survey [mms2_des_energyspectr_omni_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS2 FPI/DES electron number density during this survey [mms2_des_numberdensity_fast]
      
      
      MMS2 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms2_des_densityextrapolation_low_fast]
      
      
      MMS2 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms2_des_densityextrapolation_high_fast]
      
      
      MMS2 FPI/DES electron bulk-velocity vector in DBCS during this survey [mms2_des_bulkv_dbcs_fast]
      
      
      MMS2 FPI/DES electron bulk-velocity estimated spintone vector in DBCS during this survey [mms2_des_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS2 FPI/DES electron bulk-velocity vector in GSE during this survey [mms2_des_bulkv_gse_fast]
      
      
      MMS2 FPI/DES electron bulk-velocity estimated spintone vector in GSE during this survey [mms2_des_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS2 FPI/DES electron pressure tensor in DBCS during this survey [mms2_des_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES electron pressure tensor in GSE during this survey [mms2_des_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES electron temperature tensor in DBCS during this survey [mms2_des_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES electron temperature tensor in GSE during this survey [mms2_des_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES electron heat-flux vector in DBCS during this survey [mms2_des_heatq_dbcs_fast]
      
      
      MMS2 FPI/DES electron heat-flux vector in GSE during this survey [mms2_des_heatq_gse_fast]
      
      
      MMS2 FPI/DES electron parallel temperature during this BP [mms2_des_temppara_fast]
      
      
      MMS2 FPI/DES electron perpendicular temperature during this BP [mms2_des_tempperp_fast]
      
      
      MMS2 FPI/DES S/C potential mean [mms2_des_scpot_mean_fast]
      Average spacecraft potential during this FP used to shift the measure energies.
      
      MMS2 FPI/DES S/C potential max [mms2_des_scpot_max_fast]
      Maximum spacecraft potential during this FP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      MMS2 FPI/DES Mag data X,Y,Z,Norm DSC components [nT] at survey-start time [mms2_des_fpibentpipe_dsc_fast]
      X, Y, Z are unit vector components.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms2_des_fpib_gse_srvy_fast]
      Averaged survey magnetic field data during this FP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms2_des_fpib_dmpa_srvy_fast]
      Averaged survey magnetic field data during this FP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms2_des_pos_gse_fast]
      
      
      Position in GSM coordinates, 30 second [mms2_des_pos_gsm_fast]
      
      
      MMS2 number density integrands [mms2_des_numberdensity_int_fast]
      Integrand terms used in normalized energy integration for number density
      
      number flux [mms2_des_numberflux_int_dbcs_fast]
      Integrand terms used in normalized energy integration for number flux
      
      MMS2 pressure tensor integrands [mms2_des_prestensor_int_dbcs_fast]
      Integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms2_des_ugrid_int_fast]
      
      
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MMS2_FPI_FAST_L2_DES-PARTMOMS (spase://NASA/NumericalData/MMS/2/FastPlasmaInvestigation/DES/Fast/Level2/PartialMoments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DES vector of data-quality indicators at survey-start time [mms2_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only)
      
      MMS2 FPI/DES partial electron number density during this survey [mms2_des_numberdensity_part_fast]
      
      
      MMS2 FPI/DES partial electron bulk-velocity vector in DBCS during this survey [mms2_des_bulkv_part_dbcs_fast]
      
      
      MMS2 FPI/DES partial electron bulk-velocity vector in GSE during this survey [mms2_des_bulkv_part_gse_fast]
      
      
      MMS2 FPI/DES partial electron pressure tensor in DBCS during this survey [mms2_des_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES partial electron pressure tensor in GSE during this survey [mms2_des_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES partial electron temperature tensor in DBCS during this survey [mms2_des_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES partial electron temperature tensor in GSE during this survey [mms2_des_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES partial electron parallel temperature during this survey [mms2_des_temppara_part_fast]
      
      
      MMS2 FPI/DES partial electron perpendicular temperature during this survey [mms2_des_tempperp_part_fast]
      
      
      MMS2 FPI/DES recommended energy index during this survey [mms2_des_part_index_fast]
      Recommended energy index during this survey
      
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MMS2_FPI_FAST_L2_DIS-DIST (spase://NASA/NumericalData/MMS/2/FastPlasmaInvestigation/DIS/Fast/Level2/Distribution/PT4.5S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data taken at burst (30/150 ms for DES/DIS)
resolution are aggregated on board and made available at survey (4.5 s)
resolution in this mode.  This product contains phase-space distribution maps of
results from surveying the high-resolution observations during each 4.5 s
period.  In particular, the (highest possible quality at the time of release)
corrected/converted "Fast Survey SkyMap" distributions are reported with
time-stamps and other annotation characterizing the state of the instrument
system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DIS fast sky-map instrument distribution - 11.3 eV (E1) using averaged even/odd steps [mms2_dis_dist_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 11.3 eV [mms2_dis_dist_fast1_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS fast sky-map instrument distribution - 39.6 eV (E6) using averaged even/odd steps [mms2_dis_dist_fast6]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 39.6 eV [mms2_dis_dist_fast6_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS fast sky-map instrument distribution - 83.9 eV (E9 using averaged even/odd steps) [mms2_dis_dist_fast9]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 83.9 eV [mms2_dis_dist_fast9_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS fast sky-map instrument distribution - 178 eV (E12) using averaged even/odd steps [mms2_dis_dist_fast12]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 178 eV [mms2_dis_dist_fast12_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS fast sky-map instrument distribution - 293 eV (E14) using averaged even/odd steps [mms2_dis_dist_fast14]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 293 eV [mms2_dis_dist_fast14_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS fast sky-map instrument distribution - 484 eV (E16) using averaged even/odd steps [mms2_dis_dist_fast16]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 484 eV [mms2_dis_dist_fast16_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS fast sky-map instrument distribution - 799 eV (E18) using averaged even/odd steps [mms2_dis_dist_fast18]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 799 eV [mms2_dis_dist_fast18_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS fast sky-map instrument distribution - 1320 eV (E20) using averaged even/odd steps [mms2_dis_dist_fast20]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1320 eV [mms2_dis_dist_fast20_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS fast sky-map instrument distribution - 2800 eV (E23) using averaged even/odd steps [mms2_dis_dist_fast23]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2800 eV [mms2_dis_dist_fast23_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS fast sky-map instrument distribution - 5920 eV (E26) using averaged even/odd steps [mms2_dis_dist_fast26]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5920 eV [mms2_dis_dist_fast26_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS fast sky-map instrument distribution - 26600 eV (E32) using averaged even/odd steps [mms2_dis_dist_fast32]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 26600 eV [mms2_dis_dist_fast32_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [Only List/Create in CDAWeb] MMS2 FPI/DIS fast sky-map instrument distribution 1-sigma error [mms2_dis_disterr_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS vector of data-quality indicators at fast survey-start time - 32-bit error flags [mms2_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS2 FPI/DIS compression lossless/lossy indicator at survey-start time [mms2_dis_compressionloss_fast]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS2 FPI/DIS Del-Phi (obs spin-phase) count at fast survey-start time [mms2_dis_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS2 FPI/DIS Del-Phi (obs spin-phase) angle at fast survey-start time [mms2_dis_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS2 FPI/DIS fast survey average f1 count values [mms2_dis_avgf1counts_fast]
      Average f1-count level as a function of energy
      
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MMS2_FPI_FAST_L2_DIS-MOMS (spase://NASA/NumericalData/MMS/2/FastPlasmaInvestigation/DIS/Fast/Level2/Moments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution.  Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This moments product
contains results from integrating the standard moments of phase-space
distributions formed from the indicated data type (DES/DIS burst, FS or SS). For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotation characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DIS vector of data-quality indicators at survey-start time [mms2_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation, Bit-14 =
      high MMS3 spintone due to DIS008 anomaly
      
      ---> MMS2 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms2_dis_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      ---> MMS2 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms2_dis_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS2 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms2_dis_energyspectr_px_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      ---> MMS2 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms2_dis_energyspectr_mx_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      ---> MMS2 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms2_dis_energyspectr_py_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      ---> MMS2 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms2_dis_energyspectr_my_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      ---> MMS2 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms2_dis_energyspectr_pz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      ---> MMS2 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms2_dis_energyspectr_mz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS2 FPI/DIS omni-directional ion energy spectrum during this survey [mms2_dis_energyspectr_omni_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS2 FPI/DIS ion background energy during this survey [mms2_dis_spectr_bg_fast]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS2 FPI/DIS ion background number density during this survey [mms2_dis_numberdensity_bg_fast]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS2 FPI/DIS ion number density during this survey [mms2_dis_numberdensity_fast]
      
      
      ---> (no error bars displayed) MMS2 FPI/DIS ion number density during this survey [mms2_dis_numberdensity_fast_noerr]
      
      
      MMS2 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms2_dis_densityextrapolation_low_fast]
      
      
      MMS2 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms2_dis_densityextrapolation_high_fast]
      
      
      MMS2 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms2_dis_bulkv_dbcs_fast]
      
      
      ---> (no error bars displayed) MMS2 FPI/DIS ion bulk-velocity DBCS vector during this survey [mms2_dis_bulkv_dbcs_fast_noerr]
      
      
      MMS2 FPI/DIS ion bulk-velocity estimated spintone vector in DBCS during this survey [mms2_dis_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS2 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms2_dis_bulkv_gse_fast]
      
      
      MMS2 FPI/DIS ion bulk-velocity estimated spintone vector in GSE during this survey [mms2_dis_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS2 FPI/DIS ion bulk-velocity GSE vector during this survey [mms2_dis_bulkv_gse_fast_noerr]
      
      
      MMS2 FPI/DIS ion pressure tensor in DBCS during this survey [mms2_dis_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS ion pressure tensor in GSE during this survey [mms2_dis_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS ion background pressure during this survey [mms2_dis_pres_bg_fast]
      
      
      MMS2 FPI/DIS ion temperature tensor in DBCS during this survey [mms2_dis_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS ion temperature tensor in GSE during this survey [mms2_dis_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS ion heat-flux vector in DBCS during this survey [mms2_dis_heatq_dbcs_fast]
      
      
      MMS2 FPI/DIS ion heat-flux vector in GSE during this survey [mms2_dis_heatq_gse_fast]
      
      
      MMS2 FPI/DIS ion parallel temperature during this BP [mms2_dis_temppara_fast]
      
      
      MMS2 FPI/DIS ion perpendicular temperature during this BP [mms2_dis_tempperp_fast]
      
      
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MMS2_FPI_FAST_L2_DIS-MOMSAUX
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DIS vector of data-quality indicators at survey-start time [mms2_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation
      
      MMS2 FPI/DIS partial ion number density during this survey [mms2_dis_numberdensity_part_fast]
      
      
      MMS2 FPI/DIS partial ion bulk-velocity vector in DBCS during this survey [mms2_dis_bulkv_part_dbcs_fast]
      
      
      MMS2 FPI/DIS partial ion bulk-velocity vector in GSE during this survey [mms2_dis_bulkv_part_gse_fast]
      
      
      MMS2 FPI/DIS partial ion pressure tensor in DBCS during this survey [mms2_dis_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS partial ion pressure tensor in GSE during this survey [mms2_dis_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS partial ion temperature tensor in DBCS during this survey [mms2_dis_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS partial ion temperature tensor in GSE during this survey [mms2_dis_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS partial ion parallel temperature during this survey [mms2_dis_temppara_part_fast]
      
      
      MMS2 FPI/DIS partial ion perpendicular temperature during this survey [mms2_dis_tempperp_part_fast]
      
      
      MMS2 FPI/DIS recommended energy index for partial moments during this survey [mms2_dis_part_index_fast]
      Recommended energy index during this survey
      
      MMS2 FPI/DIS compression lossless/lossy indicator at survey-start time [mms2_dis_compressionloss_fast]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS2 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms2_dis_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS2 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms2_dis_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS2 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms2_dis_energyspectr_px_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms2_dis_energyspectr_mx_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms2_dis_energyspectr_py_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms2_dis_energyspectr_my_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms2_dis_energyspectr_pz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms2_dis_energyspectr_mz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS2 FPI/DIS omni-directional ion energy spectrum during this survey [mms2_dis_energyspectr_omni_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS2 FPI/DIS ion background energy during this survey [mms2_dis_spectr_bg_fast]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS2 FPI/DIS ion background number density during this survey [mms2_dis_numberdensity_bg_fast]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS2 FPI/DIS ion number density during this survey [mms2_dis_numberdensity_fast]
      
      
      MMS2 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms2_dis_densityextrapolation_low_fast]
      
      
      MMS2 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms2_dis_densityextrapolation_high_fast]
      
      
      MMS2 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms2_dis_bulkv_dbcs_fast]
      
      
      MMS2 FPI/DIS ion bulk-velocity estimated spintone vector in DBCS during this survey [mms2_dis_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS2 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms2_dis_bulkv_gse_fast]
      
      
      MMS2 FPI/DIS ion bulk-velocity estimated spintone vector in GSE during this survey [mms2_dis_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS2 FPI/DIS ion pressure tensor in DBCS during this survey [mms2_dis_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS ion pressure tensor in GSE during this survey [mms2_dis_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS ion background pressure during this survey [mms2_dis_pres_bg_fast]
      
      
      MMS2 FPI/DIS ion temperature tensor in DBCS during this survey [mms2_dis_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS ion temperature tensor in GSE during this survey [mms2_dis_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS ion heat-flux vector in DBCS during this survey [mms2_dis_heatq_dbcs_fast]
      
      
      MMS2 FPI/DIS ion heat-flux vector in GSE during this survey [mms2_dis_heatq_gse_fast]
      
      
      MMS2 FPI/DIS ion parallel temperature during this BP [mms2_dis_temppara_fast]
      
      
      MMS2 FPI/DIS ion perpendicular temperature during this BP [mms2_dis_tempperp_fast]
      
      
      MMS2 FPI/DIS S/C potential mean [mms2_dis_scpot_mean_fast]
      Average spacecraft potential during this FP used to shift the measure energies.
      
      MMS2 FPI/DIS S/C potential max [mms2_dis_scpot_max_fast]
      Maximum spacecraft potential during this FP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      MMS2 FPI/DIS Mag data X,Y,Z,Norm DSC components [nT] at survey-start time [mms2_dis_fpibentpipe_dsc_fast]
      X, Y, Z are unit vector components.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms2_dis_fpib_gse_srvy_fast]
      Averaged survey magnetic field data during this FP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms2_dis_fpib_dmpa_srvy_fast]
      Averaged survey magnetic field data during this FP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms2_dis_pos_gse_fast]
      
      
      Position in GSM coordinates, 30 second [mms2_dis_pos_gsm_fast]
      
      
      MMS2 number density integrands [mms2_dis_numberdensity_int_fast]
      integrand terms used in normalized energy integration for number density
      
      number flux [mms2_dis_numberflux_int_dbcs_fast]
      integrand terms used in normalized energy integration for number flux
      
      MMS2 pressure tensor integrands [mms2_dis_prestensor_int_dbcs_fast]
      integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms2_dis_ugrid_int_fast]
      
      
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MMS2_FPI_FAST_L2_DIS-PARTMOMS (spase://NASA/NumericalData/MMS/2/FastPlasmaInvestigation/DIS/Fast/Level2/PartialMoments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DIS vector of data-quality indicators at survey-start time [mms2_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation
      
      MMS2 FPI/DIS partial ion number density during this survey [mms2_dis_numberdensity_part_fast]
      
      
      MMS2 FPI/DIS partial ion bulk-velocity vector in DBCS during this survey [mms2_dis_bulkv_part_dbcs_fast]
      
      
      MMS2 FPI/DIS partial ion bulk-velocity vector in GSE during this survey [mms2_dis_bulkv_part_gse_fast]
      
      
      MMS2 FPI/DIS partial ion pressure tensor in DBCS during this survey [mms2_dis_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS partial ion pressure tensor in GSE during this survey [mms2_dis_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS partial ion temperature tensor in DBCS during this survey [mms2_dis_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS partial ion temperature tensor in GSE during this survey [mms2_dis_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS partial ion parallel temperature during this survey [mms2_dis_temppara_part_fast]
      
      
      MMS2 FPI/DIS partial ion perpendicular temperature during this survey [mms2_dis_tempperp_part_fast]
      
      
      MMS2 FPI/DIS recommended energy index during this survey [mms2_dis_part_index_fast]
      Recommended energy index during this survey
      
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MMS2_FPI_SLOW_L2_DES-DIST
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode.  This product contains phase-space distribution maps of those
survey-resolution data from Slow Mode.  In particular, the (highest possible
quality at the time of release) corrected/converted "Slow Survey SkyMap"
distributions are reported with time-stamps and other annotation characterizing
the state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DES vector of data-quality indicators at survey-start time [mms2_des_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = compression pipeline error
      
      MMS2 FPI/DES compression lossless/lossy indicator at survey-start time [mms2_des_compressionloss_slow]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS2 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms2_des_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS2 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms2_des_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS2 FPI/DES Slow Survey sky-map instrument distribution [mms2_des_dist_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES Slow Survey sky-map instrument distribution 1-sigma error [mms2_des_disterr_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DES slow survey average f1 count values [mms2_des_avgf1counts_slow]
      Average f1-count level as a function of energy
      
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MMS2_FPI_SLOW_L2_DES-MOMS
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DES vector of data-quality indicators at survey-start time [mms2_des_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only)
      
      MMS2 FPI/DES compression lossless/lossy indicator at survey-start time [mms2_des_compressionloss_slow]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS2 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms2_des_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS2 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms2_des_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS2 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms2_des_pitchangdist_lowen_slow]
      Low energy bin: energy steps 0-10 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS2 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms2_des_pitchangdist_miden_slow]
      Mid energy bin: energy steps 11-20 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS2 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms2_des_pitchangdist_highen_slow]
      High energy bin: energy steps 21-31 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS2 FPI/DES electron energy spectrum "near" +X_DBCS during this survey [mms2_des_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS2 FPI/DES electron energy spectrum "near" -X_DBCS during this survey [mms2_des_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS2 FPI/DES electron energy spectrum "near" +Y_DBCS during this survey [mms2_des_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS2 FPI/DES electron energy spectrum "near" -Y_DBCS during this survey [mms2_des_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS2 FPI/DES electron energy spectrum "near" +Z_DBCS during this survey [mms2_des_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS2 FPI/DES electron energy spectrum "near" -Z_DBCS during this survey [mms2_des_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS2 FPI/DES electron energy parallel to the magnetic field direction during this survey [mms2_des_energyspectr_par_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within 30
      degrees of the magnetic field direction.
      
      MMS2 FPI/DES electron energy anti-parallel to the magnetic field direction during this survey [mms2_des_energyspectr_anti_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      150 degrees of the magnetic field direction.
      
      MMS2 FPI/DES electron energy perpendicular to the magnetic field direction during this survey [mms2_des_energyspectr_perp_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      60-120 degrees of the magnetic field direction.
      
      MMS2 FPI/DES omni-directional electron energy spectrum during this survey [mms2_des_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS2 FPI/DES electron number density during this survey [mms2_des_numberdensity_slow]
      
      
      MMS2 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms2_des_densityextrapolation_low_slow]
      
      
      MMS2 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms2_des_densityextrapolation_high_slow]
      
      
      MMS2 FPI/DES electron bulk-velocity vector in DBCS during this survey [mms2_des_bulkv_dbcs_slow]
      
      
      MMS2 FPI/DES electron bulk-velocity vector in GSE during this survey [mms2_des_bulkv_gse_slow]
      
      
      MMS2 FPI/DES electron pressure tensor in DBCS during this survey [mms2_des_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES electron pressure tensor in GSE during this survey [mms2_des_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES electron temperature tensor in DBCS during this survey [mms2_des_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES electron temperature tensor in GSE during this survey [mms2_des_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES electron heat-flux vector in DBCS during this survey [mms2_des_heatq_dbcs_slow]
      
      
      MMS2 FPI/DES electron heat-flux vector in GSE during this survey [mms2_des_heatq_gse_slow]
      
      
      MMS2 FPI/DES electron parallel temperature during this BP [mms2_des_temppara_slow]
      
      
      MMS2 FPI/DES electron perpendicular temperature during this BP [mms2_des_tempperp_slow]
      
      
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MMS2_FPI_SLOW_L2_DES-MOMSAUX
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DES vector of data-quality indicators at survey-start time [mms2_des_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only)
      
      MMS2 FPI/DES partial electron number density during this survey [mms2_des_numberdensity_part_slow]
      
      
      MMS2 FPI/DES partial electron bulk-velocity vector in DBCS during this survey [mms2_des_bulkv_part_dbcs_slow]
      
      
      MMS2 FPI/DES partial electron bulk-velocity vector in GSE during this survey [mms2_des_bulkv_part_gse_slow]
      
      
      MMS2 FPI/DES partial electron pressure tensor in DBCS during this survey [mms2_des_prestensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES partial electron pressure tensor in GSE during this survey [mms2_des_prestensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES partial electron temperature tensor in DBCS during this survey [mms2_des_temptensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES partial electron temperature tensor in GSE during this survey [mms2_des_temptensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES partial electron parallel temperature during this survey [mms2_des_temppara_part_slow]
      
      
      MMS2 FPI/DES partial electron perpendicular temperature during this survey [mms2_des_tempperp_part_slow]
      
      
      MMS2 FPI/DES recommended energy index for partial moments during this survey [mms2_des_part_index_slow]
      Recommended energy index during this survey
      
      MMS2 FPI/DES compression lossless/lossy indicator at survey-start time [mms2_des_compressionloss_slow]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS2 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms2_des_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS2 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms2_des_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS2 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms2_des_pitchangdist_lowen_slow]
      Low energy bin: energy steps 0-10 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS2 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms2_des_pitchangdist_miden_slow]
      Mid energy bin: energy steps 11-20 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS2 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms2_des_pitchangdist_highen_slow]
      High energy bin: energy steps 21-31 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS2 FPI/DES electron energy spectrum "near" +X_DBCS during this survey [mms2_des_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS2 FPI/DES electron energy spectrum "near" -X_DBCS during this survey [mms2_des_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS2 FPI/DES electron energy spectrum "near" +Y_DBCS during this survey [mms2_des_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS2 FPI/DES electron energy spectrum "near" -Y_DBCS during this survey [mms2_des_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS2 FPI/DES electron energy spectrum "near" +Z_DBCS during this survey [mms2_des_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS2 FPI/DES electron energy spectrum "near" -Z_DBCS during this survey [mms2_des_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS2 FPI/DES electron energy parallel to the magnetic field direction during this survey [mms2_des_energyspectr_par_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within 30
      degrees of the magnetic field direction.
      
      MMS2 FPI/DES electron energy anti-parallel to the magnetic field direction during this survey [mms2_des_energyspectr_anti_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      150 degrees of the magnetic field direction.
      
      MMS2 FPI/DES electron energy perpendicular to the magnetic field direction during this survey [mms2_des_energyspectr_perp_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      60-120 degrees of the magnetic field direction.
      
      MMS2 FPI/DES omni-directional electron energy spectrum during this survey [mms2_des_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS2 FPI/DES electron number density during this survey [mms2_des_numberdensity_slow]
      
      
      MMS2 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms2_des_densityextrapolation_low_slow]
      
      
      MMS2 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms2_des_densityextrapolation_high_slow]
      
      
      MMS2 FPI/DES electron bulk-velocity vector in DBCS during this survey [mms2_des_bulkv_dbcs_slow]
      
      
      MMS2 FPI/DES electron bulk-velocity vector in GSE during this survey [mms2_des_bulkv_gse_slow]
      
      
      MMS2 FPI/DES electron pressure tensor in DBCS during this survey [mms2_des_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES electron pressure tensor in GSE during this survey [mms2_des_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DES electron temperature tensor in DBCS during this survey [mms2_des_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES electron temperature tensor in GSE during this survey [mms2_des_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DES electron heat-flux vector in DBCS during this survey [mms2_des_heatq_dbcs_slow]
      
      
      MMS2 FPI/DES electron heat-flux vector in GSE during this survey [mms2_des_heatq_gse_slow]
      
      
      MMS2 FPI/DES electron parallel temperature during this BP [mms2_des_temppara_slow]
      
      
      MMS2 FPI/DES electron perpendicular temperature during this BP [mms2_des_tempperp_slow]
      
      
      MMS2 FPI/DES S/C potential mean [mms2_des_scpot_mean_slow]
      Average spacecraft potential during this SP used to shift the measure energies.
      
      MMS2 FPI/DES S/C potential max [mms2_des_scpot_max_slow]
      Maximum spacecraft potential during this SP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms2_des_fpib_gse_srvy_slow]
      Averaged survey magnetic field data during this SP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms2_des_fpib_dmpa_srvy_slow]
      Averaged survey magnetic field data during this SP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms2_des_pos_gse_slow]
      
      
      Position in GSM coordinates, 30 second [mms2_des_pos_gsm_slow]
      
      
      MMS2 number density integrands [mms2_des_numberdensity_int_slow]
      integrand terms used in normalized energy integration for number density
      
      number flux [mms2_des_numberflux_int_dbcs_slow]
      integrand terms used in normalized energy integration for number flux
      
      MMS2 pressure tensor integrands [mms2_des_prestensor_int_dbcs_slow]
      integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms2_des_ugrid_int_slow]
      
      
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MMS2_FPI_SLOW_L2_DIS-DIST
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode.  This product contains phase-space distribution maps of those
survey-resolution data from Slow Mode.  In particular, the (highest possible
quality at the time of release) corrected/converted "Slow Survey SkyMap"
distributions are reported with time-stamps and other annotation characterizing
the state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DIS vector of data-quality indicators at survey-start time [mms2_dis_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = compression pipeline error
      
      MMS2 FPI/DIS compression lossless/lossy indicator at survey-start time [mms2_dis_compressionloss_slow]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS2 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms2_dis_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS2 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms2_dis_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS2 FPI/DIS Slow Survey sky-map instrument distribution [mms2_dis_dist_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS Slow Survey sky-map instrument distribution 1-sigma error [mms2_dis_disterr_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS2 FPI/DIS slow survey average f1 count values [mms2_dis_avgf1counts_slow]
      Average f1-count level as a function of energy
      
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MMS2_FPI_SLOW_L2_DIS-MOMS
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DIS vector of data-quality indicators at survey-start time [mms2_dis_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only), Bit-13 =
      significant (>=20%) penetrating radiation, Bit-14 = high MMS3 spintone due to
      DIS008 anomaly
      
      MMS2 FPI/DIS compression lossless/lossy indicator at survey-start time [mms2_dis_compressionloss_slow]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS2 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms2_dis_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS2 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms2_dis_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS2 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms2_dis_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms2_dis_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms2_dis_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms2_dis_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms2_dis_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms2_dis_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS2 FPI/DIS omni-directional ion energy spectrum during this survey [mms2_dis_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS2 FPI/DIS ion background energy during this survey [mms2_dis_spectr_bg_slow]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS2 FPI/DIS ion background number density during this survey [mms2_dis_numberdensity_bg_slow]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS2 FPI/DIS ion number density during this survey [mms2_dis_numberdensity_slow]
      
      
      MMS2 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms2_dis_densityextrapolation_low_slow]
      
      
      MMS2 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms2_dis_densityextrapolation_high_slow]
      
      
      MMS2 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms2_dis_bulkv_dbcs_slow]
      
      
      MMS2 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms2_dis_bulkv_gse_slow]
      
      
      MMS2 FPI/DIS ion pressure tensor in DBCS during this survey [mms2_dis_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS ion pressure tensor in GSE during this survey [mms2_dis_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS ion background pressure during this survey [mms2_dis_pres_bg_slow]
      
      
      MMS2 FPI/DIS ion temperature tensor in DBCS during this survey [mms2_dis_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS ion temperature tensor in GSE during this survey [mms2_dis_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS ion heat-flux vector in DBCS during this survey [mms2_dis_heatq_dbcs_slow]
      
      
      MMS2 FPI/DIS ion heat-flux vector in GSE during this survey [mms2_dis_heatq_gse_slow]
      
      
      MMS2 FPI/DIS ion parallel temperature during this BP [mms2_dis_temppara_slow]
      
      
      MMS2 FPI/DIS ion perpendicular temperature during this BP [mms2_dis_tempperp_slow]
      
      
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MMS2_FPI_SLOW_L2_DIS-MOMSAUX
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS2 FPI/DIS vector of data-quality indicators at survey-start time [mms2_dis_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only), Bit-13 =
      significant (>=20%) penetrating radiation, Bit-14 = high MMS3 spintone due to
      DIS008 anomaly
      
      MMS2 FPI/DIS partial ion number density during this survey [mms2_dis_numberdensity_part_slow]
      
      
      MMS2 FPI/DIS partial ion bulk-velocity vector in DBCS during this survey [mms2_dis_bulkv_part_dbcs_slow]
      
      
      MMS2 FPI/DIS partial ion bulk-velocity vector in GSE during this survey [mms2_dis_bulkv_part_gse_slow]
      
      
      MMS2 FPI/DIS partial ion pressure tensor in DBCS during this survey [mms2_dis_prestensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS partial ion pressure tensor in GSE during this survey [mms2_dis_prestensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS partial ion temperature tensor in DBCS during this survey [mms2_dis_temptensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS partial ion temperature tensor in GSE during this survey [mms2_dis_temptensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS partial ion parallel temperature during this survey [mms2_dis_temppara_part_slow]
      
      
      MMS2 FPI/DIS partial ion perpendicular temperature during this survey [mms2_dis_tempperp_part_slow]
      
      
      MMS2 FPI/DIS recommended energy index for partial moments during this survey [mms2_dis_part_index_slow]
      Recommended energy index during this survey
      
      MMS2 FPI/DIS compression lossless/lossy indicator at survey-start time [mms2_dis_compressionloss_slow]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS2 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms2_dis_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS2 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms2_dis_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS2 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms2_dis_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms2_dis_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms2_dis_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms2_dis_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms2_dis_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS2 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms2_dis_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS2 FPI/DIS omni-directional ion energy spectrum during this survey [mms2_dis_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS2 FPI/DIS ion background energy during this survey [mms2_dis_spectr_bg_slow]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS2 FPI/DIS ion background number density during this survey [mms2_dis_numberdensity_bg_slow]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS2 FPI/DIS ion number density during this survey [mms2_dis_numberdensity_slow]
      
      
      MMS2 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms2_dis_densityextrapolation_low_slow]
      
      
      MMS2 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms2_dis_densityextrapolation_high_slow]
      
      
      MMS2 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms2_dis_bulkv_dbcs_slow]
      
      
      MMS2 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms2_dis_bulkv_gse_slow]
      
      
      MMS2 FPI/DIS ion pressure tensor in DBCS during this survey [mms2_dis_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS ion pressure tensor in GSE during this survey [mms2_dis_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS2 FPI/DIS ion background pressure during this survey [mms2_dis_pres_bg_slow]
      
      
      MMS2 FPI/DIS ion temperature tensor in DBCS during this survey [mms2_dis_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS ion temperature tensor in GSE during this survey [mms2_dis_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS2 FPI/DIS ion heat-flux vector in DBCS during this survey [mms2_dis_heatq_dbcs_slow]
      
      
      MMS2 FPI/DIS ion heat-flux vector in GSE during this survey [mms2_dis_heatq_gse_slow]
      
      
      MMS2 FPI/DIS ion parallel temperature during this BP [mms2_dis_temppara_slow]
      
      
      MMS2 FPI/DIS ion perpendicular temperature during this BP [mms2_dis_tempperp_slow]
      
      
      MMS2 FPI/DIS S/C potential mean [mms2_dis_scpot_mean_slow]
      Average spacecraft potential during this SP used to shift the measure energies.
      
      MMS2 FPI/DIS S/C potential max [mms2_dis_scpot_max_slow]
      Maximum spacecraft potential during this SP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms2_dis_fpib_gse_srvy_slow]
      Averaged survey magnetic field data during this SP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms2_dis_fpib_dmpa_srvy_slow]
      Averaged survey magnetic field data during this SP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms2_dis_pos_gse_slow]
      
      
      Position in GSM coordinates, 30 second [mms2_dis_pos_gsm_slow]
      
      
      MMS2 number density integrands [mms2_dis_numberdensity_int_slow]
      integrand terms used in normalized energy integration for number density
      
      number flux [mms2_dis_numberflux_int_dbcs_slow]
      integrand terms used in normalized energy integration for number flux
      
      MMS2 pressure tensor integrands [mms2_dis_prestensor_int_dbcs_slow]
      integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms2_dis_ugrid_int_slow]
      
      
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MMS2_HPCA_BRST_L2_ION (spase://NASA/NumericalData/MMS/2/HotPlasmaCompositionAnalyzer/Burst/Level2/Ion/PT0.625S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Start Azimuth [mms2_hpca_start_azimuth]
      
      
      Science Mode Value as defined in the HPCA Science Algorithm Document [mms2_hpca_science_mode]
      
      
      H+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms2_hpca_hplus_data_quality]
      
      
      Hydrogen+ Flux for all Elevation Anodes across all energies [mms2_hpca_hplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_hplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_hplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_hplus_flux_byAnode_atE]
      
      
      Hydrogen+ Phase Space Density for all Elevation Anodes across all energies [mms2_hpca_hplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_hplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anodes [mms2_hpca_hplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_hplus_phase_space_density_byAnode_atE]
      
      
      He+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms2_hpca_heplus_data_quality]
      
      
      Helium+ Flux for all Elevation Anodes across all energies [mms2_hpca_heplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_heplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_heplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_heplus_flux_byAnode_atE]
      
      
      Helium+ Phase Space Density for all Elevation Anodes across all energies [mms2_hpca_heplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_heplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_heplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_heplus_phase_space_density_byAnode_atE]
      
      
      He++ per sweep status (0=bad): see Data_Quality_Key global attribute [mms2_hpca_heplusplus_data_quality]
      
      
      Helium++ Flux for all Elevation Anodes across all energies [mms2_hpca_heplusplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_heplusplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_heplusplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_heplusplus_flux_byAnode_atE]
      
      
      Helium++ Phase Space Density for all Elevation Anodes across all energies [mms2_hpca_heplusplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_heplusplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_heplusplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_heplusplus_phase_space_density_byAnode_atE]
      
      
      O+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms2_hpca_oplus_data_quality]
      
      
      Oxygen+ Flux for all Elevation Anodes across all energies [mms2_hpca_oplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_oplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_oplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_oplus_flux_byAnode_atE]
      
      
      Oxygen+ Phase Space Density for all Elevation Anodes across all energies [mms2_hpca_oplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_oplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_oplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_oplus_phase_space_density_byAnode_atE]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s), Despun MPA-aligned cartesian coordinates [mms2_hpca_B_GSE_sweep_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s), Geocentric Solar Magnetospheric (GSM) cartesian coordinates [mms2_hpca_B_GSM_sweep_avg]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms2_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms2_hpca_TOF_VMON_MIN_converted]
      
      
      Decimation Factor Index from mode config file [mms2_hpca_decimation_factor_index]
      
      
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MMS2_HPCA_BRST_L2_MOMENTS (spase://NASA/NumericalData/MMS/2/HotPlasmaCompositionAnalyzer/Burst/Level2/Moments/PT10S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Number Density Hydrogen+ for each HPCA half-spin [mms2_hpca_hplus_number_density]
      
      
      ---> Ion Bulk Velocity Hydrogen+ for each HPCA half-spin (x, y, z) [mms2_hpca_hplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Hydrogen+ for each HPCA half-spin [mms2_hpca_hplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_hplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_hplus_temperature_tensor]
      
      
      Number Density Helium+ for each HPCA half-spin [mms2_hpca_heplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium+ for each HPCA half-spin (x, y, z) [mms2_hpca_heplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium+ for each HPCA half-spin [mms2_hpca_heplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_heplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_heplus_temperature_tensor]
      
      
      Number Density Helium++ for each HPCA half-spin [mms2_hpca_heplusplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium++ for each HPCA half-spin (x, y, z) [mms2_hpca_heplusplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium++ for each HPCA half-spin [mms2_hpca_heplusplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_heplusplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_heplusplus_temperature_tensor]
      
      
      Number Density Oxygen+ for each HPCA half-spin [mms2_hpca_oplus_number_density]
      
      
      ---> Ion Bulk Velocity Oxygen+ for each HPCA half-spin (x, y, z) [mms2_hpca_oplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Oxygen+ for each HPCA half-spin [mms2_hpca_oplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_oplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_oplus_temperature_tensor]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms2_hpca_B_GSE_spin_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms2_hpca_B_GSM_spin_avg]
      
      
      Bulk Velocity in GSM for H+ for each HPCA half-spin (x, y, z) [mms2_hpca_hplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp H+ for each HPCA half-spin [mms2_hpca_hplus_tperp]
      
      
      ---> Tparallel H+ for each HPCA half-spin [mms2_hpca_hplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_hplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_hplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_hplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_hplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He+ for each HPCA half-spin (x, y, z) [mms2_hpca_heplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He+ for each HPCA half-spin [mms2_hpca_heplus_tperp]
      
      
      ---> Tparallel He+ for each HPCA half-spin [mms2_hpca_heplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He++ for each HPCA half-spin (x, y, z) [mms2_hpca_heplusplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He++ for each HPCA half-spin [mms2_hpca_heplusplus_tperp]
      
      
      ---> Tparallel He++ for each HPCA half-spin [mms2_hpca_heplusplus_tparallel]
      
      
      Vperp vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplusplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplusplus_vparallel]
      
      
      Vperp vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplusplus_vperp_GSM]
      
      
      Vparallel vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplusplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for O+ for each HPCA half-spin (x, y, z) [mms2_hpca_oplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp O+ for each HPCA half-spin [mms2_hpca_oplus_tperp]
      
      
      ---> Tparallel O+ for each HPCA half-spin [mms2_hpca_oplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_oplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_oplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_oplus_vperp_GSM]
      
      
      --->Vparallel vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_oplus_vparallel_GSM]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms2_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms2_hpca_TOF_VMON_MIN_converted]
      
      
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MMS2_HPCA_SRVY_L2_ION (spase://NASA/NumericalData/MMS/2/HotPlasmaCompositionAnalyzer/Survey/Level2/Ion/PT0.625S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Start Azimuth [mms2_hpca_start_azimuth]
      
      
      Science Mode Value as defined in the HPCA Science Algorithm Document [mms2_hpca_science_mode]
      
      
      H+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms2_hpca_hplus_data_quality]
      
      
      Hydrogen+ Flux for all Elevation Anodes across all energies [mms2_hpca_hplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_hplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_hplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_hplus_flux_byAnode_atE]
      
      
      Hydrogen+ Phase Space Density for all Elevation Anodes across all energies [mms2_hpca_hplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_hplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anodes [mms2_hpca_hplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_hplus_phase_space_density_byAnode_atE]
      
      
      He+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms2_hpca_heplus_data_quality]
      
      
      Helium+ Flux for all Elevation Anodes across all energies [mms2_hpca_heplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_heplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_heplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_heplus_flux_byAnode_atE]
      
      
      Helium+ Phase Space Density for all Elevation Anodes across all energies [mms2_hpca_heplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_heplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_heplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_heplus_phase_space_density_byAnode_atE]
      
      
      He++ per sweep status (0=bad): see Data_Quality_Key global attribute [mms2_hpca_heplusplus_data_quality]
      
      
      Helium++ Flux for all Elevation Anodes across all energies [mms2_hpca_heplusplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_heplusplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_heplusplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_heplusplus_flux_byAnode_atE]
      
      
      Helium++ Phase Space Density for all Elevation Anodes across all energies [mms2_hpca_heplusplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_heplusplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_heplusplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_heplusplus_phase_space_density_byAnode_atE]
      
      
      O+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms2_hpca_oplus_data_quality]
      
      
      Oxygen+ Flux for all Elevation Anodes across all energies [mms2_hpca_oplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_oplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_oplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_oplus_flux_byAnode_atE]
      
      
      Oxygen+ Phase Space Density for all Elevation Anodes across all energies [mms2_hpca_oplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms2_hpca_oplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms2_hpca_oplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms2_hpca_oplus_phase_space_density_byAnode_atE]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s), Despun MPA-aligned cartesian coordinates [mms2_hpca_B_GSE_sweep_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s), Geocentric Solar Magnetospheric (GSM) cartesian coordinates [mms2_hpca_B_GSM_sweep_avg]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms2_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms2_hpca_TOF_VMON_MIN_converted]
      
      
      Decimation Factor Index from mode config file [mms2_hpca_decimation_factor_index]
      
      
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MMS2_HPCA_SRVY_L2_MOMENTS (spase://NASA/NumericalData/MMS/2/HotPlasmaCompositionAnalyzer/Survey/Level2/Moments/PT10S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Number Density Hydrogen+ for each HPCA half-spin [mms2_hpca_hplus_number_density]
      
      
      ---> Ion Bulk Velocity Hydrogen+ for each HPCA half-spin (x, y, z) [mms2_hpca_hplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Hydrogen+ for each HPCA half-spin [mms2_hpca_hplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_hplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_hplus_temperature_tensor]
      
      
      Number Density Helium+ for each HPCA half-spin [mms2_hpca_heplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium+ for each HPCA half-spin (x, y, z) [mms2_hpca_heplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium+ for each HPCA half-spin [mms2_hpca_heplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_heplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_heplus_temperature_tensor]
      
      
      Number Density Helium++ for each HPCA half-spin [mms2_hpca_heplusplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium++ for each HPCA half-spin (x, y, z) [mms2_hpca_heplusplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium++ for each HPCA half-spin [mms2_hpca_heplusplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_heplusplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_heplusplus_temperature_tensor]
      
      
      Number Density Oxygen+ for each HPCA half-spin [mms2_hpca_oplus_number_density]
      
      
      ---> Ion Bulk Velocity Oxygen+ for each HPCA half-spin (x, y, z) [mms2_hpca_oplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Oxygen+ for each HPCA half-spin [mms2_hpca_oplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_oplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms2_hpca_oplus_temperature_tensor]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms2_hpca_B_GSE_spin_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms2_hpca_B_GSM_spin_avg]
      
      
      Bulk Velocity in GSM for H+ for each HPCA half-spin (x, y, z) [mms2_hpca_hplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp H+ for each HPCA half-spin [mms2_hpca_hplus_tperp]
      
      
      ---> Tparallel H+ for each HPCA half-spin [mms2_hpca_hplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_hplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_hplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_hplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_hplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He+ for each HPCA half-spin (x, y, z) [mms2_hpca_heplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He+ for each HPCA half-spin [mms2_hpca_heplus_tperp]
      
      
      ---> Tparallel He+ for each HPCA half-spin [mms2_hpca_heplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He++ for each HPCA half-spin (x, y, z) [mms2_hpca_heplusplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He++ for each HPCA half-spin [mms2_hpca_heplusplus_tperp]
      
      
      ---> Tparallel He++ for each HPCA half-spin [mms2_hpca_heplusplus_tparallel]
      
      
      Vperp vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplusplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplusplus_vparallel]
      
      
      Vperp vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplusplus_vperp_GSM]
      
      
      Vparallel vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms2_hpca_heplusplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for O+ for each HPCA half-spin (x, y, z) [mms2_hpca_oplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp O+ for each HPCA half-spin [mms2_hpca_oplus_tperp]
      
      
      ---> Tparallel O+ for each HPCA half-spin [mms2_hpca_oplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_oplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_oplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_oplus_vperp_GSM]
      
      
      --->Vparallel vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms2_hpca_oplus_vparallel_GSM]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms2_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms2_hpca_TOF_VMON_MIN_converted]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS2_HPCA_SRVY_L2_TOF-COUNTS (spase://NASA/NumericalData/MMS/2/HotPlasmaCompositionAnalyzer/Survey/Level2/TimeOfFlight/Counts/PT0.625S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      TOF Counts for all angles, across all energies [mms2_hpca_tof_counts]
      
      
      ---> Spectrograms all angles, at selected energies [mms2_hpca_tof_counts_allA_atE]
      
      
      ---> Spectrograms at select angles, for all energies [mms2_hpca_tof_counts_allE_atA]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS2_MEC_BRST_L2_EPHT89D (spase://NASA/NumericalData/MMS/2/Ephemeris/Burst/Level2/Tsyganenko_89_Dynamic/PT0.030S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms2_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms2_mec_gmst]
      
      
      Magnetic Latitude. [mms2_mec_mlat]
      
      
      Magnetic Local Time. [mms2_mec_mlt]
      
      
      Dipole L-shell value. [mms2_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms2_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms2_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms2_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms2_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms2_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms2_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms2_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms2_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms2_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms2_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms2 (km) [mms2_mec_r_eci]
      
      
      Velocity of mms2 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms2_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms2 (km) [mms2_mec_r_gsm]
      
      
      Velocity of mms2 spacecraft in GSM coordinates (km/s) [mms2_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms2 (km) [mms2_mec_r_geo]
      
      
      Velocity of mms2 spacecraft in GEO coordinates (km/s) [mms2_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms2 (km) [mms2_mec_r_sm]
      
      
      Velocity of mms2 spacecraft in SM coordinates (km/s) [mms2_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms2 (km) [mms2_mec_r_gse]
      
      
      Velocity of mms2 spacecraft in GSE coordinates (km/s) [mms2_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms2 (km) [mms2_mec_r_gse2000]
      
      
      Velocity of mms2 spacecraft in GSE2000 coordinates (km/s) [mms2_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms2 spacecraft [mms2_mec_geod_lat]
      
      
      Geodetic longitude of mms2 spacecraft [mms2_mec_geod_lon]
      
      
      Geodetic height of mms2 spacecraft. (Height above WGS84 Spheroid.) [mms2_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms2_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms2_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms2_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms2 spacecraft [mms2_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms2_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms2_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms2 spacecraft [mms2_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms2 spacecraft [mms2_mec_bmin_gsm]
      
      
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MMS2_MEC_BRST_L2_EPHT89Q (spase://NASA/NumericalData/MMS/2/Ephemeris/Burst/Level2/Tsyganenko_89_Quiet/PT0.030S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms2_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms2_mec_gmst]
      
      
      Magnetic Latitude. [mms2_mec_mlat]
      
      
      Magnetic Local Time. [mms2_mec_mlt]
      
      
      Dipole L-shell value. [mms2_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms2_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms2_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms2_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms2_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms2_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms2_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms2_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms2_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms2_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms2_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms2 (km) [mms2_mec_r_eci]
      
      
      Velocity of mms2 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms2_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms2 (km) [mms2_mec_r_gsm]
      
      
      Velocity of mms2 spacecraft in GSM coordinates (km/s) [mms2_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms2 (km) [mms2_mec_r_geo]
      
      
      Velocity of mms2 spacecraft in GEO coordinates (km/s) [mms2_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms2 (km) [mms2_mec_r_sm]
      
      
      Velocity of mms2 spacecraft in SM coordinates (km/s) [mms2_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms2 (km) [mms2_mec_r_gse]
      
      
      Velocity of mms2 spacecraft in GSE coordinates (km/s) [mms2_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms2 (km) [mms2_mec_r_gse2000]
      
      
      Velocity of mms2 spacecraft in GSE2000 coordinates (km/s) [mms2_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms2 spacecraft [mms2_mec_geod_lat]
      
      
      Geodetic longitude of mms2 spacecraft [mms2_mec_geod_lon]
      
      
      Geodetic height of mms2 spacecraft. (Height above WGS84 Spheroid.) [mms2_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms2_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms2_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms2_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms2 spacecraft [mms2_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms2_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms2_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms2 spacecraft [mms2_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms2 spacecraft [mms2_mec_bmin_gsm]
      
      
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MMS2_MEC_BRST_L2_EPHTS04D (spase://NASA/NumericalData/MMS/2/Ephemeris/Burst/Level2/Tsyganenko_04_Dynamic/PT0.030S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms2_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms2_mec_gmst]
      
      
      Magnetic Latitude. [mms2_mec_mlat]
      
      
      Magnetic Local Time. [mms2_mec_mlt]
      
      
      Dipole L-shell value. [mms2_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms2_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms2_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms2_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms2_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms2_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms2_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms2_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms2_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms2_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms2_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms2 (km) [mms2_mec_r_eci]
      
      
      Velocity of mms2 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms2_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms2 (km) [mms2_mec_r_gsm]
      
      
      Velocity of mms2 spacecraft in GSM coordinates (km/s) [mms2_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms2 (km) [mms2_mec_r_geo]
      
      
      Velocity of mms2 spacecraft in GEO coordinates (km/s) [mms2_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms2 (km) [mms2_mec_r_sm]
      
      
      Velocity of mms2 spacecraft in SM coordinates (km/s) [mms2_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms2 (km) [mms2_mec_r_gse]
      
      
      Velocity of mms2 spacecraft in GSE coordinates (km/s) [mms2_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms2 (km) [mms2_mec_r_gse2000]
      
      
      Velocity of mms2 spacecraft in GSE2000 coordinates (km/s) [mms2_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms2 spacecraft [mms2_mec_geod_lat]
      
      
      Geodetic longitude of mms2 spacecraft [mms2_mec_geod_lon]
      
      
      Geodetic height of mms2 spacecraft. (Height above WGS84 Spheroid.) [mms2_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms2_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms2_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms2_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms2 spacecraft [mms2_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms2_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms2_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms2 spacecraft [mms2_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms2 spacecraft [mms2_mec_bmin_gsm]
      
      
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MMS2_MEC_SRVY_L2_EPHT89D (spase://NASA/NumericalData/MMS/2/Ephemeris/Survey/Level2/Tsyganenko_89_Dynamic/PT30S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms2_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms2_mec_gmst]
      
      
      Magnetic Latitude. [mms2_mec_mlat]
      
      
      Magnetic Local Time. [mms2_mec_mlt]
      
      
      Dipole L-shell value. [mms2_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms2_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms2_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms2_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms2_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms2_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms2_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms2_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms2_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms2_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms2_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms2 (km) [mms2_mec_r_eci]
      
      
      Velocity of mms2 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms2_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms2 (km) [mms2_mec_r_gsm]
      
      
      Velocity of mms2 spacecraft in GSM coordinates (km/s) [mms2_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms2 (km) [mms2_mec_r_geo]
      
      
      Velocity of mms2 spacecraft in GEO coordinates (km/s) [mms2_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms2 (km) [mms2_mec_r_sm]
      
      
      Velocity of mms2 spacecraft in SM coordinates (km/s) [mms2_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms2 (km) [mms2_mec_r_gse]
      
      
      Velocity of mms2 spacecraft in GSE coordinates (km/s) [mms2_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms2 (km) [mms2_mec_r_gse2000]
      
      
      Velocity of mms2 spacecraft in GSE2000 coordinates (km/s) [mms2_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms2 spacecraft [mms2_mec_geod_lat]
      
      
      Geodetic longitude of mms2 spacecraft [mms2_mec_geod_lon]
      
      
      Geodetic height of mms2 spacecraft. (Height above WGS84 Spheroid.) [mms2_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms2_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms2_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms2_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms2 spacecraft [mms2_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms2_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms2_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms2 spacecraft [mms2_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms2 spacecraft [mms2_mec_bmin_gsm]
      
      
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MMS2_MEC_SRVY_L2_EPHT89Q (spase://NASA/NumericalData/MMS/2/Ephemeris/Survey/Level2/Tsyganenko_89_Quiet/PT30S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms2_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms2_mec_gmst]
      
      
      Magnetic Latitude. [mms2_mec_mlat]
      
      
      Magnetic Local Time. [mms2_mec_mlt]
      
      
      Dipole L-shell value. [mms2_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms2_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms2_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms2_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms2_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms2_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms2_mec_P_phase]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms2_mec_ang_mom_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms2_mec_ang_mom_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms2_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms2_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms2_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms2_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms2 (km) [mms2_mec_r_eci]
      
      
      Velocity of mms2 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms2_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms2 (km) [mms2_mec_r_gsm]
      
      
      Velocity of mms2 spacecraft in GSM coordinates (km/s) [mms2_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms2 (km) [mms2_mec_r_geo]
      
      
      Velocity of mms2 spacecraft in GEO coordinates (km/s) [mms2_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms2 (km) [mms2_mec_r_sm]
      
      
      Velocity of mms2 spacecraft in SM coordinates (km/s) [mms2_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms2 (km) [mms2_mec_r_gse]
      
      
      Velocity of mms2 spacecraft in GSE coordinates (km/s) [mms2_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms2 (km) [mms2_mec_r_gse2000]
      
      
      Velocity of mms2 spacecraft in GSE2000 coordinates (km/s) [mms2_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms2 spacecraft [mms2_mec_geod_lat]
      
      
      Geodetic longitude of mms2 spacecraft [mms2_mec_geod_lon]
      
      
      Geodetic height of mms2 spacecraft. (Height above WGS84 Spheroid.) [mms2_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms2_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms2_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms2_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms2 spacecraft [mms2_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms2_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms2_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms2 spacecraft [mms2_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms2 spacecraft [mms2_mec_bmin_gsm]
      
      
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MMS2_MEC_SRVY_L2_EPHTS04D (spase://NASA/NumericalData/MMS/2/Ephemeris/Survey/Level2/Tsyganenko_04_Dynamic/PT30S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms2_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms2_mec_gmst]
      
      
      Magnetic Latitude. [mms2_mec_mlat]
      
      
      Magnetic Local Time. [mms2_mec_mlt]
      
      
      Dipole L-shell value. [mms2_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms2_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms2_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms2_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms2_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms2_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms2_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms2_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms2_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms2_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms2_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms2 (km) [mms2_mec_r_eci]
      
      
      Velocity of mms2 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms2_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms2 (km) [mms2_mec_r_gsm]
      
      
      Velocity of mms2 spacecraft in GSM coordinates (km/s) [mms2_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms2 (km) [mms2_mec_r_geo]
      
      
      Velocity of mms2 spacecraft in GEO coordinates (km/s) [mms2_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms2 (km) [mms2_mec_r_sm]
      
      
      Velocity of mms2 spacecraft in SM coordinates (km/s) [mms2_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms2 (km) [mms2_mec_r_gse]
      
      
      Velocity of mms2 spacecraft in GSE coordinates (km/s) [mms2_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms2 (km) [mms2_mec_r_gse2000]
      
      
      Velocity of mms2 spacecraft in GSE2000 coordinates (km/s) [mms2_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms2_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms2 spacecraft [mms2_mec_geod_lat]
      
      
      Geodetic longitude of mms2 spacecraft [mms2_mec_geod_lon]
      
      
      Geodetic height of mms2 spacecraft. (Height above WGS84 Spheroid.) [mms2_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms2_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms2_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms2_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms2 spacecraft [mms2_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms2_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms2_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms2 spacecraft [mms2_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms2 spacecraft [mms2_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms2 spacecraft [mms2_mec_bmin_gsm]
      
      
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MMS2_R0_SUMMARY
Description
Pre-generated MMS Quicklook Summary Plots
File location: https://cdaweb.gsfc.nasa.gov/pub/data/mms/ql_plots/all_mms2_summ 
 
  • Data Variable Descriptions
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MMS2_SCM_BRST_L2_SCB (spase://NASA/NumericalData/MMS/2/FIELDS/SCM/Burst/Level2/PT0.0001220703125S)
Description
The tri-axial search-coil magnetometer (SCM) with its associated preamplifier
provides the three-dimensional measurement of the magnetic field fluctuations.
The analog magnetic waveforms measured by the SCM are digitized and processed
inside the digital signal processor (DSP), collected and stored by the central
instrument data processor (CIDP) via the Fields central electronics box (CEB).
Prior to launch, all SCM Flight models were calibrated by LPP at the National
Magnetic Observatory at Chambon-la-Foret (Orleans). Once per orbit, each SCM
transfer function is checked thanks to the onboard calibration signal provided
by DSP. SCM is operated for the entire MMS orbit in survey mode. Within the ROI,
burst mode data are also acquired as well as high burst mode data. 
SCM data set corresponds to the AC magnetic field waveforms in nanoTesla and in
the GSE frame.
The instrument paper for SCM can be found at
https://urldefense.proofpoint.com/v2/url?u=http-3A__link.springer.com_article_10
.1007_s11214-2D014-2D0096-2D9&d=DwIFAg&c=c6MrceVCY5m5A_KAUkrdoA&r=bjziExGTRYoZgE
2xb_dDSm9NxNIo0lG6Q-rB0Y6rHS4&m=CMzo0Vv9zPtWSdbdY1Wq9-jIkYS2cOMV9JYZsMV10y0&s=Xb
P9PiEAswHGl5lqgsDVI6zs8ivJx7yek9i2undKl10&e= 
Modification History
unpack telemetry, assign sample times
2026-07-10T20:11:42.00002789497058Z - [L1A->L1B (step 1/1)] Calibration
(TMcounts->nT). See CALIBRATION_PARAMETERS for details.
2026-07-16T12:36:37.00003266334522Z - [L1B->L2 (step 1/2)] Coordinate transform
(SCM123->GSE). See COORD_TRANS_PARAMETERS for details.
2026-07-16T12:36:43.00004035234439Z - [L1B->L2 (step 2/2)] Frequency filtering.
See FREQUENCY_FILTER for details.
 
  • Data Variable Descriptions
      L2 AC magnetic field in GSE frame [mms2_scm_acb_gse_scb_brst_l2]
      These calibrated (nT) AC magnetic field waveform data are sampled at 8192S/s.
      They are high-pass filtered above 1.00Hz but not low-pass filtered. See global
      attributes for details. For more information, please have a look at the SCM Data
      Products Guide.
      
      (List/Create Only) Quality Factor (one letter per antenna, G=good) [mms2_scm_qf_scm123_scb_brst_l2]
      Each letter refers to one SCM physical antenna in the SCM123 order. 'G' stands
      for good data, 'Z' for data that are affected or set to zero by convolution
      boundary effect, 'S' for saturated data, 'X' for out of range data, 'B' for
      fillvalue/bad data.
      
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MMS2_SCM_BRST_L2_SCHB (spase://NASA/NumericalData/MMS/2/FIELDS/SCM/Burst/Level2/PT0.00006101515625S)
Description
The tri-axial search-coil magnetometer (SCM) with its associated preamplifier
provides the three-dimensional measurement of the magnetic field fluctuations.
The analog magnetic waveforms measured by the SCM are digitized and processed
inside the digital signal processor (DSP), collected and stored by the central
instrument data processor (CIDP) via the Fields central electronics box (CEB).
Prior to launch, all SCM Flight models were calibrated by LPP at the National
Magnetic Observatory at Chambon-la-Foret (Orleans). Once per orbit, each SCM
transfer function is checked thanks to the onboard calibration signal provided
by DSP. SCM is operated for the entire MMS orbit in survey mode. Within the ROI,
burst mode data are also acquired as well as high burst mode data. 
SCM data set corresponds to the AC magnetic field waveforms in nanoTesla and in
the GSE frame.
The instrument paper for SCM can be found at
http://link.springer.com/article/10.1007/s11214-014-0096-9
Modification History
unpack telemetry, assign sample times
2026-07-10T20:12:08.00004780292192Z - [L1A->L1B (step 1/1)] Calibration
(TMcounts->nT). See CALIBRATION_PARAMETERS for details.
2026-07-16T12:41:12.00002968311314Z - [L1B->L2 (step 1/2)] Coordinate transform
(SCM123->GSE). See COORD_TRANS_PARAMETERS for details.
2026-07-16T12:41:17.00004279613499Z - [L1B->L2 (step 2/2)] Frequency filtering.
See FREQUENCY_FILTER for details.
 
  • Data Variable Descriptions
      L2 AC magnetic field in GSE frame [mms2_scm_acb_gse_schb_brst_l2]
      These calibrated (nT) AC magnetic field waveform data are sampled at 16384S/s.
      They are high-pass filtered above 32.00Hz but not low-pass filtered. See global
      attributes for details. For more information, please have a look at the SCM Data
      Products Guide
      (https://lasp.colorado.edu/mms/sdc/public/datasets/fields/Science_Data_Products_ 
      Guide_vol2_SCM_v11_20160301.pdf).
      
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MMS2_SCM_SRVY_L2_SCSRVY (spase://NASA/NumericalData/MMS/2/FIELDS/SCM/Survey/Level2/PT0.03125S)
Description
The tri-axial search-coil magnetometer (SCM) with its associated preamplifier
provides the three-dimensional measurement of the magnetic field fluctuations.
The analog magnetic waveforms measured by the SCM are digitized and processed
inside the digital signal processor (DSP), collected and stored by the central
instrument data processor (CIDP) via the Fields central electronics box (CEB).
Prior to launch, all SCM Flight models were calibrated by LPP at the National
Magnetic Observatory at Chambon-la-Foret (Orleans). Once per orbit, each SCM
transfer function is checked thanks to the onboard calibration signal provided
by DSP. SCM is operated for the entire MMS orbit in survey mode. Within the ROI,
burst mode data are also acquired as well as high burst mode data. 
SCM data set corresponds to the AC magnetic field waveforms in nanoTesla and in
the GSE frame.
The instrument paper for SCM can be found at
http://link.springer.com/article/10.1007/s11214-014-0096-9
Modification History
unpack telemetry, assign sample times
2026-07-02T23:56:41.00003331899318Z - [L1A->L1B (step 1/1)] Calibration
(TMcounts->nT). See CALIBRATION_PARAMETERS for details.
2026-07-15T23:55:18.0000409483875Z - [L1B->L2 (step 1/2)] Coordinate transform
(SCM123->GSE). See COORD_TRANS_PARAMETERS for details.
2026-07-15T23:56:09.00004595517787Z - [L1B->L2 (step 2/2)] Frequency filtering.
See FREQUENCY_FILTER for details.
 
  • Data Variable Descriptions
      L2 AC magnetic field in GSE frame [mms2_scm_acb_gse_scsrvy_srvy_l2]
      These calibrated (nT) AC magnetic field waveform data are sampled at 32S/s. They
      are high-pass filtered above 0.50Hz but not low-pass filtered. See global
      attributes for details. For more information, please have a look at the SCM Data
      Products Guide
      (https://lasp.colorado.edu/mms/sdc/public/datasets/fields/Science_Data_Products_ 
      Guide_vol2_SCM_v11_20160301.pdf).
      
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MMS3_ASPOC_SRVY_L2 (spase://NASA/NumericalData/MMS/3/ASPOC/Survey/Level2/PT1S)
Description
K. Torkar et al, Active Spacecraft Potential Control Investigation
Space Science Reviews, 2014, DOI: 10.1007/s11214-014-0049-3
Further information:
- http://www.iwf.oeaw.ac.at/en/research/near-earth-space/mms/ 
- http://mms.space.swri.edu/ 
Modification History
150224 Initial version
150831 Minor updates and fixes
160205 CDF file format guide compliant
 
  • Data Variable Descriptions
      ASPOC Ion Emission Current Sum, 1s resolution [mms3_aspoc_ionc]
      
      
      ASPOC Unit 1 Ion Emission Current, 1s resolution [mms3_asp1_ionc]
      
      
      ASPOC Unit 2 Ion Emission Current, 1s resolution [mms3_asp2_ionc]
      
      
      ASPOC Unit 1 Emitted Beam Energy, 1s resolution [mms3_asp1_energy]
      
      
      ASPOC Unit 2 Emitted Beam Energy, 1s resolution [mms3_asp2_energy]
      
      
      ASPOC Data Quality and Instrument Status, 1s resolution [mms3_aspoc_status]
      
      
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MMS3_DSP_FAST_L2_BPSD (spase://NASA/NumericalData/MMS/3/FIELDS/DSP/Fast/Level2/MagneticFieldPowerSpectralDensity/PT2S)
Description
BPSD is the low frequency B spectral density covering the frequency range of .2
to 6000 Hz.
 
  • Data Variable Descriptions
      SCM Axis 1 (X) component magnetic power spectral density [mms3_dsp_bpsd_scm1_fast_l2]
      
      
      SCM Axis 2 (Y, ~direction of S/C Z) component magnetic power spectral density [mms3_dsp_bpsd_scm2_fast_l2]
      
      
      SCM Axis 3 (Z) component magnetic power spectral density [mms3_dsp_bpsd_scm3_fast_l2]
      
      
      Omni-directional magnetic power spectral density: square root of the sum of the squares of 3 components [mms3_dsp_bpsd_omni_fast_l2]
      
      
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MMS3_DSP_FAST_L2_EPSD (spase://NASA/NumericalData/MMS/3/FIELDS/DSP/Fast/Level2/ElectricFieldPowerSpectralDensity/PT2S)
Description
EPSD combines the low frequency E spectral density covering the frequency range
of 1 to 8000 Hz and the  medium frequency E spectral density covering the
frequency range of .25 to 100 kHz.
 
  • Data Variable Descriptions
      null [mms3_dsp_epsd_x]
      
      
      null [mms3_dsp_epsd_y]
      
      
      null [mms3_dsp_epsd_z]
      
      
      null [mms3_dsp_epsd_omni]
      
      
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MMS3_DSP_SLOW_L2_BPSD (spase://NASA/NumericalData/MMS/3/FIELDS/DSP/Slow/Level2/MagneticFieldPowerSpectralDensity/PT16S)
Description
search coil magnetometer spectral density
 
  • Data Variable Descriptions
      SCM1 component magnetic power spectral density [mms3_dsp_bpsd_scm1_slow_l2]
      
      
      SCM2 component magnetic power spectral density - NO DATA in Slow Survey [mms3_dsp_bpsd_scm2_slow_l2]
      
      
      SCM3 component magnetic power spectral density [mms3_dsp_bpsd_scm3_slow_l2]
      
      
      Omni-directional magnetic power spectral density: square root of the sum of the squares of 2 components [mms3_dsp_bpsd_omni_slow_l2]
      
      
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MMS3_DSP_SLOW_L2_EPSD (spase://NASA/NumericalData/MMS/3/FIELDS/DSP/Slow/Level2/ElectricFieldPowerSpectralDensity/PT16S)
Description
electric spectral density
 
  • Data Variable Descriptions
      null [mms3_dsp_epsd_x]
      
      
      null [mms3_dsp_epsd_y]
      
      
      null [mms3_dsp_epsd_z]
      
      
      null [mms3_dsp_epsd_omni]
      
      
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MMS3_EDI_BRST_L2_AMB (spase://NASA/NumericalData/MMS/3/FIELDS/EDI/Burst/Level2/ElectronFluxAmbient/ProjectionMethod1/PT0.0009765625S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - Original version.
v1.0.0 - Include trajectory vectors and optics state.
v1.1.0 - Update metadata: counts -> flux.
v1.2.0 - Added flux error.
v1.3.0 - Trajectory vector errors are now deltas.
v1.4.0 - Fixed dead-time correction and error values.
v1.5.0 - Factor of 2 for accumulation time & 2 for abscal factor in srvy mode.
v1.6.0 - No factor of 2 for accumulation time in srvy mode.
v2.0.0 - Reduced file size with scalar errors. Update metadata.
v2.1.0 - Correct fill value for fluxes.
v3.0.0 - Omni-directional error for trajectories. Y-Version linked to cal file.
Single epoch for counts.
v4.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
 
  • Data Variable Descriptions
      Optics state [mms3_edi_optics_state_brst_l2]
      
      
      ---> GDU1 energy [mms3_edi_energy_gdu1_brst_l2]
      
      
      ---> GDU2 energy [mms3_edi_energy_gdu2_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-1 0PA [mms3_edi_flux1_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-1 0PA [mms3_edi_flux1_0_brst_l2_noerr]
      
      
      ---> Error for flux1 0-degree pitch angle electron flux. [mms3_edi_flux1_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-2 0PA [mms3_edi_flux2_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-2 0PA [mms3_edi_flux2_0_brst_l2_noerr]
      
      
      ---> Error for flux2 0-degree pitch angle electron flux. [mms3_edi_flux2_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-3 0PA [mms3_edi_flux3_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-3 0PA [mms3_edi_flux3_0_brst_l2_noerr]
      
      
      ---> Error for flux3 0-degree pitch angle electron flux. [mms3_edi_flux3_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-4 0PA [mms3_edi_flux4_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-4 0PA [mms3_edi_flux4_0_brst_l2_noerr]
      
      
      ---> Error for flux4 0-degree pitch angle electron flux. [mms3_edi_flux4_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-1 180PA [mms3_edi_flux1_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-1 180PA [mms3_edi_flux1_180_brst_l2_noerr]
      
      
      ---> Error for flux1 180-degree pitch angle electron flux. [mms3_edi_flux1_180_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by traj2 180PA [mms3_edi_flux2_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-2 180PA [mms3_edi_flux2_180_brst_l2_noerr]
      
      
      ---> Error for flux2 180-degree pitch angle electron flux. [mms3_edi_flux2_180_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by traj3 180PA [mms3_edi_flux3_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-3 180PA [mms3_edi_flux3_180_brst_l2_noerr]
      
      
      ---> Error for flux3 180-degree pitch angle electron flux. [mms3_edi_flux3_180_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by traj4 180PA [mms3_edi_flux4_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-4 180PA [mms3_edi_flux4_180_brst_l2_noerr]
      
      
      ---> Error for flux4 180-degree pitch angle electron flux. [mms3_edi_flux4_180_delta_brst_l2]
      
      
      Trajectory of flux1 0-degree pitch angle electrons in GSE coordinates. [mms3_edi_traj1_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 0-degree pitch angle electrons in GSE coordinates. [mms3_edi_traj2_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 0-degree pitch angle electrons in GSE coordinates. [mms3_edi_traj3_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 0-degree pitch angle electrons in GSE coordinates. [mms3_edi_traj4_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of flux1 180-degree pitch angle electrons in GSE coordinates. [mms3_edi_traj1_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 180-degree pitch angle electrons in GSE coordinates. [mms3_edi_traj2_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 180-degree pitch angle electrons in GSE coordinates. [mms3_edi_traj3_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 180-degree pitch angle electrons in GSE coordinates. [mms3_edi_traj4_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj1_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 0-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj2_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 0-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj3_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 0-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj4_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj1_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 180-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj2_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 180-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj3_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 180-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj4_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms3_edi_traj1_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms3_edi_traj2_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms3_edi_traj3_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms3_edi_traj4_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms3_edi_traj1_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms3_edi_traj2_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms3_edi_traj3_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms3_edi_traj4_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS3_EDI_BRST_L2_AMB-PM2 (spase://NASA/NumericalData/MMS/3/FIELDS/EDI/Burst/Level2/AmbientElectronFlux/ProjectionMethod2/PT0.0009765625S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v1.0.0 - Original version.
v1.1.0 - Correct fill value for fluxes.
v2.0.0 - Omni-directional error for trajectories. Y-Version linked to cal file.
Single epoch for counts.
v3.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
v4.0.0 - Each trajectory has its own LABL_PTR_1 variable.
 
  • Data Variable Descriptions
      Optics state [mms3_edi_optics_state_brst_l2]
      
      
      ---> GDU1 energy [mms3_edi_energy_gdu1_brst_l2]
      
      
      ---> GDU2 energy [mms3_edi_energy_gdu2_brst_l2]
      
      
      Field-aligned electron flux from channel 1 of both GDUs [mms3_edi_flux1_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 1 of both GDUs [mms3_edi_flux1_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 1 of both GDUs. [mms3_edi_flux1_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 1 of both GDUs [mms3_edi_flux1_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 1 of both GDUs [mms3_edi_flux1_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 1 of both GDUs. [mms3_edi_flux1_180_delta_brst_l2]
      
      
      Field-aligned electron flux from channel 2 of both GDUs [mms3_edi_flux2_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 2 of both GDUs [mms3_edi_flux2_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 2 of both GDUs. [mms3_edi_flux2_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 2 of both GDUs [mms3_edi_flux2_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 2 of both GDUs [mms3_edi_flux2_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 2 of both GDUs. [mms3_edi_flux2_180_delta_brst_l2]
      
      
      Field-aligned electron flux from channel 3 of both GDUs [mms3_edi_flux3_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 3 of both GDUs [mms3_edi_flux3_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 3 of both GDUs. [mms3_edi_flux3_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 3 of both GDUs [mms3_edi_flux3_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 3 of both GDUs [mms3_edi_flux3_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 3 of both GDUs. [mms3_edi_flux3_180_delta_brst_l2]
      
      
      Field-aligned electron flux from channel 4 of both GDUs [mms3_edi_flux4_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 4 of both GDUs [mms3_edi_flux4_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 4 of both GDUs. [mms3_edi_flux4_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 4 of both GDUs [mms3_edi_flux4_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 4 of both GDUs [mms3_edi_flux4_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 4 of both GDUs. [mms3_edi_flux4_180_delta_brst_l2]
      
      
      Trajectory of field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms3_edi_traj1_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms3_edi_traj1_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 1 of both GDUs in GSE coordinates. [mms3_edi_traj1_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 1 of both GDUs, in GSE coordinates. [mms3_edi_traj1_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms3_edi_traj2_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms3_edi_traj2_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 2 of both GDUs in GSE coordinates. [mms3_edi_traj2_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 2 of both GDUs, in GSE coordinates. [mms3_edi_traj2_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms3_edi_traj3_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms3_edi_traj3_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 3 of both GDUs in GSE coordinates. [mms3_edi_traj3_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 3 of both GDUs, in GSE coordinates. [mms3_edi_traj3_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms3_edi_traj4_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms3_edi_traj4_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 4 of both GDUs in GSE coordinates. [mms3_edi_traj4_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 4 of both GDUs, in GSE coordinates. [mms3_edi_traj4_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj1_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj1_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS3_EDI_BRST_L2_EFIELD (spase://NASA/NumericalData/MMS/3/FIELDS/EDI/Burst/Level2/ElectricField/PT0.0009765625S)
Description
EDI electric field data. Instrument papers for EDI can be found at:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7
Modification History
v1.0.0 - First version. TRI-TOF selection based on smallest error.
v1.1.0 - TRI-TOF merged by weighted average.
v1.2.0 - Fixed t_delta_plus/minus CDF_type.
v1.3.0 - Fixed Fixed vdrift SI conversion.
v1.4.0 - Fixed data duplication caused by multiple l2pre file locations.
v1.5.0 - Inplemented baseline*beams*Bmag filter for triangulation.
v1.6.0 - Inplemented null files for no or low quality data.
 
  • Data Variable Descriptions
      ExB drift velocity in DSL coordinates. [mms3_edi_vdrift_dsl_brst_l2]
      
      
      ---> ExB drift velocity in DSL coordinates (no error bars) [mms3_edi_vdrift_dsl_brst_l2_noerr]
      
      
      ExB drift velocity in GSE coordinates. [mms3_edi_vdrift_gse_brst_l2]
      
      
      ---> ExB drift velocity in GSE coordinates (no error bars) [mms3_edi_vdrift_gse_brst_l2_noerr]
      
      
      ExB drift velocity in GSM coordinates. [mms3_edi_vdrift_gsm_brst_l2]
      
      
      ---> ExB drift velocity in GSM coordinates (no error bars) [mms3_edi_vdrift_gsm_brst_l2_noerr]
      
      
      Electric field in DSL coordinates. [mms3_edi_e_dsl_brst_l2]
      
      
      ---> Electric field in DSL coordinates (no error bars) [mms3_edi_e_dsl_brst_l2_noerr]
      
      
      Electric field in GSE coordinates. [mms3_edi_e_gse_brst_l2]
      
      
      ---> Electric field in GSE coordinates (no error bars) [mms3_edi_e_gse_brst_l2_noerr]
      
      
      Electric field in GSM coordinates. [mms3_edi_e_gsm_brst_l2]
      
      
      ---> Electric field in GSM coordinates (no error bars) [mms3_edi_e_gsm_brst_l2_noerr]
      
      
      Weighted use of TRI method in L2 results. [mms3_edi_tri_weight_brst_l2]
      
      
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MMS3_EDI_BRST_L2_Q0 (spase://NASA/NumericalData/MMS/3/FIELDS/EDI/Burst/Level2/QualityZero/PT0.0078125S)
Description
EDI Q0 data. The EDI instrument paper and data products guidescan be found at
the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - First version.
v0.0.1 - Filled energy variables.
v0.0.2 - Energy written properly.
v1.0.0 - Update variable names.
v1.1.0 - Added optics state.
v2.0.0 - Added electron trajectories.
v2.1.0 - Deltas on trajectory vectors are now deltas.
v3.0.0 - Reduced file size with scalar errors. Add VAR_NOTES.
v3.1.0 - Fixed optics datatype.
v4.0.0 - Removed unused Epoch variable.
v5.0.0 - Trajectories are provided in DBCS coordinates.
 
  • Data Variable Descriptions
      Optics state [mms3_edi_optics_state_brst_l2]
      
      
      ---> GDU1 energy [mms3_edi_energy_gdu1_brst_l2]
      
      
      ---> GDU2 energy [mms3_edi_energy_gdu2_brst_l2]
      
      
      GDU1 quality 0 counts. [mms3_edi_counts_gdu1_brst_l2]
      Q0 data consists of raw electron counts. The error at any one time is the
      square-root of the counts. Note that there may be contamination from the EDI
      electron beams. See the data products guide or contact an EDI team member to
      learn about beam contamination.
      
      GDU2 quality 0 counts. [mms3_edi_counts_gdu2_brst_l2]
      
      
      GDU1 electron incident trajectory vectors in spherical BCS coordinates. [mms3_edi_traj_bcs_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical BCS coordinates. [mms3_edi_traj_bcs_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical DBCS coordinates. [mms3_edi_traj_dbcs_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical DBCS coordinates. [mms3_edi_traj_dbcs_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSE coordinates. [mms3_edi_traj_gse_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSE coordinates. [mms3_edi_traj_gse_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSM coordinates. [mms3_edi_traj_gsm_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSM coordinates. [mms3_edi_traj_gsm_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS3_EDI_SRVY_L2_AMB (spase://NASA/NumericalData/MMS/3/FIELDS/EDI/Survey/Level2/ElectronFluxAmbient/ProjectionMethod1/PT0.03125S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - Original version.
v1.0.0 - Include trajectory vectors and optics state.
v1.1.0 - Update metadata: counts -> flux.
v1.2.0 - Added flux error.
v1.3.0 - Trajectory vector errors are now deltas.
v1.4.0 - Fixed dead-time correction and error values.
v1.5.0 - Factor of 2 for accumulation time & 2 for abscal factor in srvy mode.
v1.6.0 - No factor of 2 for accumulation time in srvy mode.
v2.0.0 - Reduced file size with scalar errors. Update metadata.
v2.1.0 - Correct fill value for fluxes.
v3.0.0 - Omni-directional error for trajectories. Correct time deltas. Y-Version
linked to cal file. Single epoch for counts.
v4.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
 
  • Data Variable Descriptions
      Optics state [mms3_edi_optics_state_srvy_l2]
      
      
      ---> GDU1 energy [mms3_edi_energy_gdu1_srvy_l2]
      
      
      ---> GDU2 energy [mms3_edi_energy_gdu2_srvy_l2]
      
      
      Field-aligned electron flux from both GDUs [mms3_edi_flux1_0_srvy_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from both GDUs [mms3_edi_flux1_0_srvy_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from both GDUs. [mms3_edi_flux1_0_delta_srvy_l2]
      
      
      Anti-field-aligned electron flux from both GDUs [mms3_edi_flux1_180_srvy_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from both GDUs [mms3_edi_flux1_180_srvy_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from both GDUs. [mms3_edi_flux1_180_delta_srvy_l2]
      
      
      Trajectory of field-aligned electrons from both GDUs in DBCS coordinates. [mms3_edi_traj1_dbcs_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs in DBCS coordinates. [mms3_edi_traj1_dbcs_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from both GDUs in GSE coordinates. [mms3_edi_traj1_gse_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs, in GSE coordinates. [mms3_edi_traj1_gse_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj1_gsm_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj1_gsm_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS3_EDI_SRVY_L2_AMB-PM2 (spase://NASA/NumericalData/MMS/3/FIELDS/EDI/Survey/Level2/ElectronFluxAmbient/ProjectionMethod2/PT0.03125S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v1.0.0 - Original version.
v1.1.0 - Correct fill value for fluxes.
v2.0.0 - Omni-directional error for trajectories. Y-Version linked to cal file.
Single epoch for counts.
v3.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
v4.0.0 - Each trajectory has its own LABL_PTR_1 variable.
 
  • Data Variable Descriptions
      Optics state [mms3_edi_optics_state_srvy_l2]
      
      
      ---> GDU1 energy [mms3_edi_energy_gdu1_srvy_l2]
      
      
      ---> GDU2 energy [mms3_edi_energy_gdu2_srvy_l2]
      
      
      Field-aligned electron flux from both GDUs [mms3_edi_flux1_0_srvy_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from both GDUs [mms3_edi_flux1_0_srvy_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from both GDUs. [mms3_edi_flux1_0_delta_srvy_l2]
      
      
      Anti-field-aligned electron flux from both GDUs [mms3_edi_flux1_180_srvy_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from both GDUs [mms3_edi_flux1_180_srvy_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from both GDUs. [mms3_edi_flux1_180_delta_srvy_l2]
      
      
      Trajectory of field-aligned electrons from both GDUs in DBCS coordinates. [mms3_edi_traj1_dbcs_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs in DBCS coordinates. [mms3_edi_traj1_dbcs_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from both GDUs in GSE coordinates. [mms3_edi_traj1_gse_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs, in GSE coordinates. [mms3_edi_traj1_gse_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj1_gsm_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms3_edi_traj1_gsm_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS3_EDI_SRVY_L2_EFIELD (spase://NASA/NumericalData/MMS/3/FIELDS/EDI/Survey/Level2/ElectricField/PT5S)
Description
EDI electric field data. Instrument papers for EDI can be found at:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7
Modification History
v1.0.0 - First version. TRI-TOF selection based on smallest error.
v1.1.0 - TRI-TOF merged by weighted average.
v1.2.0 - Fixed t_delta_plus/minus CDF_type.
v1.3.0 - Fixed Fixed vdrift SI conversion.
v1.4.0 - Fixed data duplication caused by multiple l2pre file locations.
v1.5.0 - Inplemented baseline*beams*Bmag filter for triangulation.
v1.6.0 - Inplemented null files for no or low quality data.
 
  • Data Variable Descriptions
      ExB drift velocity in DSL coordinates. [mms3_edi_vdrift_dsl_srvy_l2]
      
      
      ---> ExB drift velocity in DSL coordinates (no error bars) [mms3_edi_vdrift_dsl_srvy_l2_noerr]
      
      
      ExB drift velocity in GSE coordinates. [mms3_edi_vdrift_gse_srvy_l2]
      
      
      ---> ExB drift velocity in GSE coordinates (no error bars) [mms3_edi_vdrift_gse_srvy_l2_noerr]
      
      
      ExB drift velocity in GSM coordinates. [mms3_edi_vdrift_gsm_srvy_l2]
      
      
      ---> ExB drift velocity in GSM coordinates (no error bars) [mms3_edi_vdrift_gsm_srvy_l2_noerr]
      
      
      Electric field in DSL coordinates. [mms3_edi_e_dsl_srvy_l2]
      
      
      ---> Electric field in DSL coordinates (no error bars) [mms3_edi_e_dsl_srvy_l2_noerr]
      
      
      Electric field in GSE coordinates. [mms3_edi_e_gse_srvy_l2]
      
      
      ---> Electric field in GSE coordinates (no error bars) [mms3_edi_e_gse_srvy_l2_noerr]
      
      
      Electric field in GSM coordinates. [mms3_edi_e_gsm_srvy_l2]
      
      
      ---> Electric field in GSM coordinates (no error bars) [mms3_edi_e_gsm_srvy_l2_noerr]
      
      
      Weighted use of TRI method in L2 results. [mms3_edi_tri_weight_srvy_l2]
      
      
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MMS3_EDI_SRVY_L2_Q0 (spase://NASA/NumericalData/MMS/3/FIELDS/EDI/Survey/Level2/QualityZero/PT0.125S)
Description
EDI Q0 data. The EDI instrument paper and data products guidescan be found at
the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - First version.
v0.0.1 - Filled energy variables.
v0.0.2 - Energy written properly.
v1.0.0 - Update variable names.
v1.1.0 - Added optics state.
v2.0.0 - Added electron trajectories.
v2.1.0 - Deltas on trajectory vectors are now deltas.
v3.0.0 - Reduced file size with scalar errors. Add VAR_NOTES.
v4.0.0 - Removed unused Epoch variable.
v5.0.0 - Trajectories are provided in DBCS coordinates.
 
  • Data Variable Descriptions
      Optics state [mms3_edi_optics_state_srvy_l2]
      
      
      ---> GDU1 energy [mms3_edi_energy_gdu1_srvy_l2]
      
      
      ---> GDU2 energy [mms3_edi_energy_gdu2_srvy_l2]
      
      
      GDU1 quality 0 counts. [mms3_edi_counts_gdu1_srvy_l2]
      Q0 data consists of raw electron counts. The error at any one time is the
      square-root of the counts. Note that there may be contamination from the EDI
      electron beams. See the data products guide or contact an EDI team member to
      learn about beam contamination.
      
      GDU2 quality 0 counts. [mms3_edi_counts_gdu2_srvy_l2]
      
      
      GDU1 electron incident trajectory vectors in spherical BCS coordinates. [mms3_edi_traj_bcs_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical BCS coordinates. [mms3_edi_traj_bcs_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical DBCS coordinates. [mms3_edi_traj_dbcs_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical DBCS coordinates. [mms3_edi_traj_dbcs_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSE coordinates. [mms3_edi_traj_gse_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSE coordinates. [mms3_edi_traj_gse_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSM coordinates. [mms3_edi_traj_gsm_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSM coordinates. [mms3_edi_traj_gsm_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS3_EDP_BRST_L2_DCE (spase://NASA/NumericalData/MMS/3/FIELDS/EDP/Burst/Level2/DCElectricField/PT0.0001220703125S)
Description
http://mms.gsfc.nasa.gov/
Modification History
V.0. Initial release.
 
  • Data Variable Descriptions
      L2 DC E Field (GSE coords) calibrated for SDP and ADP, all flag values included [mms3_edp_dce_gse_brst_l2]
      
      
      L2 DC E Field (DSL coords) calibrated for SDP and ADP, all flag values included [mms3_edp_dce_dsl_brst_l2]
      
      
      L2 DC E Parallel Field calibrated for SDP and ADP [mms3_edp_dce_par_epar_brst_l2]
      
      
      Quality indicator (3 good), (2 ok data, use with some caution), (1 bad data, use with caution), (0 Really bad data or no data at all) [mms3_edp_quality_brst_l2]
      
      
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MMS3_EDP_BRST_L2_HMFE (spase://NASA/NumericalData/MMS/3/FIELDS/EDP/Burst/Level2Pre/HMFE/PT0.00001525878906S)
Description
 d
 
  • Data Variable Descriptions
      DC E Field calibrated for SDP and ADP [mms3_edp_hmfe_dsl_brst_l2]
      
      
      DC E parallel Field from calibrated SDP and ADP [mms3_edp_hmfe_par_epar_brst_l2]
      
      
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MMS3_EDP_BRST_L2_SCPOT doi:10.48322/x3td-gh63
Proper citations should include the "Accessed on date" in the form .
Description
http://mms.gsfc.nasa.gov/
The full name of PI affiliations: SWRI - Southwest Research Institute. LASP -
Laboratory for Atmospheric and Space Physics. KTH - Kungliga Tekniska Hogskolan
(Swedish Royal Institute of Technology). 
Modification History
V.0. Initial release.
V.1. QL (v1.0.z), SCPOT (v1.0.z), L2A (v0.1.z) now uses ASPOC srvy l2 and
DEFATT, if these are available. Brst QL uses intermediate L2A file from Fast
mode for delta offsets. Bitmask changed to uint16 and Quality to uint8.
V.2. SCPOT (v2.0.z), L2A (v1.0.z) now uses variable names in accordance with new
recommended standard for FIELDS, All products change shortening factor to 1.25
on SDP, offsets applied indicated by GlobalAttribute Calibration_file.
V.2. L2a (v2.0.z), QL (v1.6.z) now try to remove solar wind wake which
previously left a clear sinusodial signal in the data.
V.3. L2a (v3.0.z) Slow Mode probe Gain set to 1.0 when orbital radius less than
5 RE (1.25 otherwise), L2pre (v2.0.z) DSL offsets removed from field is now
included in the file as the Slow mode is dependent on scpot product (Fast/Brst
is simply based on offset in Calibration_file).
 
  • Data Variable Descriptions
      Spacecraft potential [mms3_edp_scpot_brst_l2]
      
      
      Probe to spacecraft potential, averaged [mms3_edp_psp_brst_l2]
      
      
      Probe to spacecraft potential, individual probes [mms3_edp_dcv_brst_l2]
      
      
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MMS3_EDP_FAST_L2_DCE (spase://NASA/NumericalData/MMS/3/FIELDS/EDP/Fast/Level2/DCElectricField/PT0.03125S)
Description
http://mms.gsfc.nasa.gov/
Modification History
V.0. Initial release.
 
  • Data Variable Descriptions
      L2 DC E Field (GSE coords) calibrated for SDP and ADP, all flag values included [mms3_edp_dce_gse_fast_l2]
      
      
      L2 DC E Field (DSL coords) calibrated for SDP and ADP, all flag values included [mms3_edp_dce_dsl_fast_l2]
      
      
      L2 DC E Parallel Field with error calibrated for SDP and ADP [mms3_edp_dce_par_epar_fast_l2]
      
      
      Approximate DC E field error derived from SDP (quality and bitmask) and ADP (residue) [mms3_edp_dce_err_fast_l2]
      
      
      Quality indicator (3 good), (2 ok data, use with some caution), (1 bad data, use with caution), (0 Really bad data or no data at all) [mms3_edp_quality_fast_l2]
      
      
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MMS3_EDP_FAST_L2_SCPOT doi:10.48322/kzh6-vf67
Proper citations should include the "Accessed on date" in the form .
Description
http://mms.gsfc.nasa.gov/
The full name of PI affiliations: SWRI - Southwest Research Institute. LASP -
Laboratory for Atmospheric and Space Physics. KTH - Kungliga Tekniska Hogskolan
(Swedish Royal Institute of Technology). 
Modification History
V.0. Initial release.
V.1. QL (v1.0.z), SCPOT (v1.0.z), L2A (v0.1.z) now uses ASPOC srvy l2 and
DEFATT, if these are available. Brst QL uses intermediate L2A file from Fast
mode for delta offsets. Bitmask changed to uint16 and Quality to uint8.
V.2. SCPOT (v2.0.z), L2A (v1.0.z) now uses variable names in accordance with new
recommended standard for FIELDS, All products change shortening factor to 1.25
on SDP, offsets applied indicated by GlobalAttribute Calibration_file.
V.2. L2a (v2.0.z), QL (v1.6.z) now try to remove solar wind wake which
previously left a clear sinusodial signal in the data.
V.3. L2a (v3.0.z) Slow Mode probe Gain set to 1.0 when orbital radius less than
5 RE (1.25 otherwise), L2pre (v2.0.z) DSL offsets removed from field is now
included in the file as the Slow mode is dependent on scpot product (Fast/Brst
is simply based on offset in Calibration_file).
 
  • Data Variable Descriptions
      Spacecraft potential [mms3_edp_scpot_fast_l2]
      
      
      Probe to spacecraft potential, averaged [mms3_edp_psp_fast_l2]
      
      
      Probe to spacecraft potential, individual probes [mms3_edp_dcv_fast_l2]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS3_EDP_SLOW_L2_DCE (spase://NASA/NumericalData/MMS/3/FIELDS/EDP/Slow/Level2/DCElectricField/PT0.125S)
Description
http://mms.gsfc.nasa.gov/
Modification History
V.0. Initial release.
 
  • Data Variable Descriptions
      L2 DC E Field (GSE coords) calibrated for SDP and ADP, all flag values included [mms3_edp_dce_gse_slow_l2]
      
      
      L2 DC E Field (DSL coords) calibrated for SDP and ADP, all flag values included [mms3_edp_dce_dsl_slow_l2]
      
      
      L2 DC E Parallel Field with error calibrated for SDP and ADP [mms3_edp_dce_par_epar_slow_l2]
      
      
      Approximate DC E field error derived from SDP (quality and bitmask) and ADP (residue) [mms3_edp_dce_err_slow_l2]
      
      
      Quality indicator (3 good), (2 ok data, use with some caution), (1 bad data, use with caution), (0 Really bad data or no data at all) [mms3_edp_quality_slow_l2]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS3_EDP_SLOW_L2_SCPOT doi:10.48322/5vc4-ys82
Proper citations should include the "Accessed on date" in the form .
Description
http://mms.gsfc.nasa.gov/
The full name of PI affiliations: SWRI - Southwest Research Institute. LASP -
Laboratory for Atmospheric and Space Physics. KTH - Kungliga Tekniska Hogskolan
(Swedish Royal Institute of Technology). 
Modification History
V.0. Initial release.
V.1. QL (v1.0.z), SCPOT (v1.0.z), L2A (v0.1.z) now uses ASPOC srvy l2 and
DEFATT, if these are available. Brst QL uses intermediate L2A file from Fast
mode for delta offsets. Bitmask changed to uint16 and Quality to uint8.
V.2. SCPOT (v2.0.z), L2A (v1.0.z) now uses variable names in accordance with new
recommended standard for FIELDS, All products change shortening factor to 1.25
on SDP, offsets applied indicated by GlobalAttribute Calibration_file.
V.2. L2a (v2.0.z), QL (v1.6.z) now try to remove solar wind wake which
previously left a clear sinusodial signal in the data.
V.3. L2a (v3.0.z) Slow Mode probe Gain set to 1.0 when orbital radius less than
5 RE (1.25 otherwise), L2pre (v2.0.z) DSL offsets removed from field is now
included in the file as the Slow mode is dependent on scpot product (Fast/Brst
is simply based on offset in Calibration_file).
 
  • Data Variable Descriptions
      Spacecraft potential [mms3_edp_scpot_slow_l2]
      
      
      Probe to spacecraft potential, averaged [mms3_edp_psp_slow_l2]
      
      
      Probe to spacecraft potential, individual probes [mms3_edp_dcv_slow_l2]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS3_EDP_SRVY_L2_HFESP (spase://NASA/NumericalData/MMS/3/FIELDS/EDP/Survey/Level2/HighFrequencyElectricFieldSpectra/PT16S)
Description
 AC Electric Field
 
  • Data Variable Descriptions
      HF ACE E Field Spectral Density [mms3_edp_hfesp_srvy_l2]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS3_EPD-EIS_BRST_L2_EXTOF (spase://NASA/NumericalData/MMS/3/EnergeticParticleDetector/EIS/Burst/Level2/EnergyByTimeOfFlight/PT0.605S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms3_epd_eis_brst_l2_extof_duration]
      
      
      ---> Instrument Deadtime [mms3_epd_eis_brst_l2_extof_deadtime]
      
      
      ---> Instrument Large Pixel in Use [mms3_epd_eis_brst_l2_extof_largepixel]
      
      
      ---> Spin [mms3_epd_eis_brst_l2_extof_spin]
      
      
      ---> Sector [mms3_epd_eis_brst_l2_extof_sector]
      
      
      ---> Quality Word [mms3_epd_eis_brst_l2_extof_quality]
      
      
      MMS3 ExTOF-Burst proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_extof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms3_epd_eis_brst_l2_extof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms3_epd_eis_brst_l2_extof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms3_epd_eis_brst_l2_extof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms3_epd_eis_brst_l2_extof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms3_epd_eis_brst_l2_extof_proton_P6_counts_t5]
      
      
      MMS3 ExTOF-Burst proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_extof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms3_epd_eis_brst_l2_extof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms3_epd_eis_brst_l2_extof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms3_epd_eis_brst_l2_extof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms3_epd_eis_brst_l2_extof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms3_epd_eis_brst_l2_extof_proton_P6_cps_t5]
      
      
      MMS3 ExTOF-Burst proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_extof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms3_epd_eis_brst_l2_extof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms3_epd_eis_brst_l2_extof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms3_epd_eis_brst_l2_extof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms3_epd_eis_brst_l2_extof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms3_epd_eis_brst_l2_extof_proton_P6_flux_t5]
      
      
      MMS3 ExTOF-Burst helium_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_extof_helium_P6_counts_t0]
      
      
      ---> helium_P6_counts_t1 [mms3_epd_eis_brst_l2_extof_helium_P6_counts_t1]
      
      
      ---> helium_P6_counts_t2 [mms3_epd_eis_brst_l2_extof_helium_P6_counts_t2]
      
      
      ---> helium_P6_counts_t3 [mms3_epd_eis_brst_l2_extof_helium_P6_counts_t3]
      
      
      ---> helium_P6_counts_t4 [mms3_epd_eis_brst_l2_extof_helium_P6_counts_t4]
      
      
      ---> helium_P6_counts_t5 [mms3_epd_eis_brst_l2_extof_helium_P6_counts_t5]
      
      
      MMS3 ExTOF-Burst helium_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_extof_helium_P6_cps_t0]
      
      
      ---> helium_P6_cps_t1 [mms3_epd_eis_brst_l2_extof_helium_P6_cps_t1]
      
      
      ---> helium_P6_cps_t2 [mms3_epd_eis_brst_l2_extof_helium_P6_cps_t2]
      
      
      ---> helium_P6_cps_t3 [mms3_epd_eis_brst_l2_extof_helium_P6_cps_t3]
      
      
      ---> helium_P6_cps_t4 [mms3_epd_eis_brst_l2_extof_helium_P6_cps_t4]
      
      
      ---> helium_P6_cps_t5 [mms3_epd_eis_brst_l2_extof_helium_P6_cps_t5]
      
      
      MMS3 ExTOF-Burst helium_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_extof_helium_P6_flux_t0]
      
      
      ---> helium_P6_flux_t1 [mms3_epd_eis_brst_l2_extof_helium_P6_flux_t1]
      
      
      ---> helium_P6_flux_t2 [mms3_epd_eis_brst_l2_extof_helium_P6_flux_t2]
      
      
      ---> helium_P6_flux_t3 [mms3_epd_eis_brst_l2_extof_helium_P6_flux_t3]
      
      
      ---> helium_P6_flux_t4 [mms3_epd_eis_brst_l2_extof_helium_P6_flux_t4]
      
      
      ---> helium_P6_flux_t5 [mms3_epd_eis_brst_l2_extof_helium_P6_flux_t5]
      
      
      MMS3 ExTOF-Burst oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_extof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms3_epd_eis_brst_l2_extof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms3_epd_eis_brst_l2_extof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms3_epd_eis_brst_l2_extof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms3_epd_eis_brst_l2_extof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms3_epd_eis_brst_l2_extof_oxygen_P6_counts_t5]
      
      
      MMS3 ExTOF-Burst oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_extof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms3_epd_eis_brst_l2_extof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms3_epd_eis_brst_l2_extof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms3_epd_eis_brst_l2_extof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms3_epd_eis_brst_l2_extof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms3_epd_eis_brst_l2_extof_oxygen_P6_cps_t5]
      
      
      MMS3 ExTOF-Burst oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_extof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms3_epd_eis_brst_l2_extof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms3_epd_eis_brst_l2_extof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms3_epd_eis_brst_l2_extof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms3_epd_eis_brst_l2_extof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms3_epd_eis_brst_l2_extof_oxygen_P6_flux_t5]
      
      
      MMS3 ExTOF-Burst dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_extof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms3_epd_eis_brst_l2_extof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms3_epd_eis_brst_l2_extof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms3_epd_eis_brst_l2_extof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms3_epd_eis_brst_l2_extof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms3_epd_eis_brst_l2_extof_dump_P6_counts_t5]
      
      
      MMS3 ExTOF-Burst dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_extof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms3_epd_eis_brst_l2_extof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms3_epd_eis_brst_l2_extof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms3_epd_eis_brst_l2_extof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms3_epd_eis_brst_l2_extof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms3_epd_eis_brst_l2_extof_dump_P6_cps_t5]
      
      
      MMS3 ExTOF-Burst dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_extof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms3_epd_eis_brst_l2_extof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms3_epd_eis_brst_l2_extof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms3_epd_eis_brst_l2_extof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms3_epd_eis_brst_l2_extof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms3_epd_eis_brst_l2_extof_dump_P6_flux_t5]
      
      
      MMS3 ExTOF-Burst proton_P5_counts_t0 [data available from 2020/09/24 to 2025/01/06] [mms3_epd_eis_brst_l2_extof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms3_epd_eis_brst_l2_extof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms3_epd_eis_brst_l2_extof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms3_epd_eis_brst_l2_extof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms3_epd_eis_brst_l2_extof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms3_epd_eis_brst_l2_extof_proton_P5_counts_t5]
      
      
      MMS3 ExTOF-Burst proton_P5_cps_t0 [data available from 2020/09/24 to 2025/01/06] [mms3_epd_eis_brst_l2_extof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms3_epd_eis_brst_l2_extof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms3_epd_eis_brst_l2_extof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms3_epd_eis_brst_l2_extof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms3_epd_eis_brst_l2_extof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms3_epd_eis_brst_l2_extof_proton_P5_cps_t5]
      
      
      MMS3 ExTOF-Burst proton_P5_flux_t0 [data available from 2020/09/24 to 2025/01/06] [mms3_epd_eis_brst_l2_extof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms3_epd_eis_brst_l2_extof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms3_epd_eis_brst_l2_extof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms3_epd_eis_brst_l2_extof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms3_epd_eis_brst_l2_extof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms3_epd_eis_brst_l2_extof_proton_P5_flux_t5]
      
      
      MMS3 ExTOF-Burst oxygen_P5_counts_t0 [data available from 2020/09/24 to 2025/01/06] [mms3_epd_eis_brst_l2_extof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms3_epd_eis_brst_l2_extof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms3_epd_eis_brst_l2_extof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms3_epd_eis_brst_l2_extof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms3_epd_eis_brst_l2_extof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms3_epd_eis_brst_l2_extof_oxygen_P5_counts_t5]
      
      
      MMS3 ExTOF-Burst oxygen_P5_cps_t0 [data available from 2020/09/24 to 2025/01/06] [mms3_epd_eis_brst_l2_extof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms3_epd_eis_brst_l2_extof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms3_epd_eis_brst_l2_extof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms3_epd_eis_brst_l2_extof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms3_epd_eis_brst_l2_extof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms3_epd_eis_brst_l2_extof_oxygen_P5_cps_t5]
      
      
      MMS3 ExTOF-Burst oxygen_P5_flux_t0 [data available from 2020/09/24 to 2025/01/06] [mms3_epd_eis_brst_l2_extof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms3_epd_eis_brst_l2_extof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms3_epd_eis_brst_l2_extof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms3_epd_eis_brst_l2_extof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms3_epd_eis_brst_l2_extof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms3_epd_eis_brst_l2_extof_oxygen_P5_flux_t5]
      
      
      MMS3 ExTOF-Burst helium_P5_counts_t0 [data available from 2020/09/24 to 2025/01/06] [mms3_epd_eis_brst_l2_extof_helium_P5_counts_t0]
      
      
      ---> helium_P5_counts_t1 [mms3_epd_eis_brst_l2_extof_helium_P5_counts_t1]
      
      
      ---> helium_P5_counts_t2 [mms3_epd_eis_brst_l2_extof_helium_P5_counts_t2]
      
      
      ---> helium_P5_counts_t3 [mms3_epd_eis_brst_l2_extof_helium_P5_counts_t3]
      
      
      ---> helium_P5_counts_t4 [mms3_epd_eis_brst_l2_extof_helium_P5_counts_t4]
      
      
      ---> helium_P5_counts_t5 [mms3_epd_eis_brst_l2_extof_helium_P5_counts_t5]
      
      
      MMS3 ExTOF-Burst helium_P5_cps_t0 [data available from 2020/09/24 to 2025/01/06] [mms3_epd_eis_brst_l2_extof_helium_P5_cps_t0]
      
      
      ---> helium_P5_cps_t1 [mms3_epd_eis_brst_l2_extof_helium_P5_cps_t1]
      
      
      ---> helium_P5_cps_t2 [mms3_epd_eis_brst_l2_extof_helium_P5_cps_t2]
      
      
      ---> helium_P5_cps_t3 [mms3_epd_eis_brst_l2_extof_helium_P5_cps_t3]
      
      
      ---> helium_P5_cps_t4 [mms3_epd_eis_brst_l2_extof_helium_P5_cps_t4]
      
      
      ---> helium_P5_cps_t5 [mms3_epd_eis_brst_l2_extof_helium_P5_cps_t5]
      
      
      MMS3 ExTOF-Burst helium_P5_flux_t0 [data available from 2020/09/24 to 2025/01/06] [mms3_epd_eis_brst_l2_extof_helium_P5_flux_t0]
      
      
      ---> helium_P5_flux_t1 [mms3_epd_eis_brst_l2_extof_helium_P5_flux_t1]
      
      
      ---> helium_P5_flux_t2 [mms3_epd_eis_brst_l2_extof_helium_P5_flux_t2]
      
      
      ---> helium_P5_flux_t3 [mms3_epd_eis_brst_l2_extof_helium_P5_flux_t3]
      
      
      ---> helium_P5_flux_t4 [mms3_epd_eis_brst_l2_extof_helium_P5_flux_t4]
      
      
      ---> helium_P5_flux_t5 [mms3_epd_eis_brst_l2_extof_helium_P5_flux_t5]
      
      
      MMS3 ExTOF-Burst proton_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_extof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms3_epd_eis_brst_l2_extof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms3_epd_eis_brst_l2_extof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms3_epd_eis_brst_l2_extof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms3_epd_eis_brst_l2_extof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms3_epd_eis_brst_l2_extof_proton_P4_counts_t5]
      
      
      MMS3 ExTOF-Burst proton_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_extof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms3_epd_eis_brst_l2_extof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms3_epd_eis_brst_l2_extof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms3_epd_eis_brst_l2_extof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms3_epd_eis_brst_l2_extof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms3_epd_eis_brst_l2_extof_proton_P4_cps_t5]
      
      
      MMS3 ExTOF-Burst proton_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_extof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms3_epd_eis_brst_l2_extof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms3_epd_eis_brst_l2_extof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms3_epd_eis_brst_l2_extof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms3_epd_eis_brst_l2_extof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms3_epd_eis_brst_l2_extof_proton_P4_flux_t5]
      
      
      MMS3 ExTOF-Burst alpha_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_extof_helium_P4_counts_t0]
      
      
      ---> alpha_P4_counts_t1 [mms3_epd_eis_brst_l2_extof_helium_P4_counts_t1]
      
      
      ---> alpha_P4_counts_t2 [mms3_epd_eis_brst_l2_extof_helium_P4_counts_t2]
      
      
      ---> alpha_P4_counts_t3 [mms3_epd_eis_brst_l2_extof_helium_P4_counts_t3]
      
      
      ---> alpha_P4_counts_t4 [mms3_epd_eis_brst_l2_extof_helium_P4_counts_t4]
      
      
      ---> alpha_P4_counts_t5 [mms3_epd_eis_brst_l2_extof_helium_P4_counts_t5]
      
      
      MMS3 ExTOF-Burst alpha_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_extof_helium_P4_cps_t0]
      
      
      ---> alpha_P4_cps_t1 [mms3_epd_eis_brst_l2_extof_helium_P4_cps_t1]
      
      
      ---> alpha_P4_cps_t2 [mms3_epd_eis_brst_l2_extof_helium_P4_cps_t2]
      
      
      ---> alpha_P4_cps_t3 [mms3_epd_eis_brst_l2_extof_helium_P4_cps_t3]
      
      
      ---> alpha_P4_cps_t4 [mms3_epd_eis_brst_l2_extof_helium_P4_cps_t4]
      
      
      ---> alpha_P4_cps_t5 [mms3_epd_eis_brst_l2_extof_helium_P4_cps_t5]
      
      
      MMS3 ExTOF-Burst alpha_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_extof_helium_P4_flux_t0]
      
      
      ---> alpha_P4_flux_t1 [mms3_epd_eis_brst_l2_extof_helium_P4_flux_t1]
      
      
      ---> alpha_P4_flux_t2 [mms3_epd_eis_brst_l2_extof_helium_P4_flux_t2]
      
      
      ---> alpha_P4_flux_t3 [mms3_epd_eis_brst_l2_extof_helium_P4_flux_t3]
      
      
      ---> alpha_P4_flux_t4 [mms3_epd_eis_brst_l2_extof_helium_P4_flux_t4]
      
      
      ---> alpha_P4_flux_t5 [mms3_epd_eis_brst_l2_extof_helium_P4_flux_t5]
      
      
      MMS3 ExTOF-Burst oxygen_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_extof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms3_epd_eis_brst_l2_extof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms3_epd_eis_brst_l2_extof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms3_epd_eis_brst_l2_extof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms3_epd_eis_brst_l2_extof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms3_epd_eis_brst_l2_extof_oxygen_P4_counts_t5]
      
      
      MMS3 ExTOF-Burst oxygen_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_extof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms3_epd_eis_brst_l2_extof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms3_epd_eis_brst_l2_extof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms3_epd_eis_brst_l2_extof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms3_epd_eis_brst_l2_extof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms3_epd_eis_brst_l2_extof_oxygen_P4_cps_t5]
      
      
      MMS3 ExTOF-Burst oxygen_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_extof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms3_epd_eis_brst_l2_extof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms3_epd_eis_brst_l2_extof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms3_epd_eis_brst_l2_extof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms3_epd_eis_brst_l2_extof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms3_epd_eis_brst_l2_extof_oxygen_P4_flux_t5]
      
      
      MMS3 ExTOF-Burst proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_extof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms3_epd_eis_brst_l2_extof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms3_epd_eis_brst_l2_extof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms3_epd_eis_brst_l2_extof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms3_epd_eis_brst_l2_extof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms3_epd_eis_brst_l2_extof_proton_P3_counts_t5]
      
      
      MMS3 ExTOF-Burst proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_extof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms3_epd_eis_brst_l2_extof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms3_epd_eis_brst_l2_extof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms3_epd_eis_brst_l2_extof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms3_epd_eis_brst_l2_extof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms3_epd_eis_brst_l2_extof_proton_P3_cps_t5]
      
      
      MMS3 ExTOF-Burst proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_extof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms3_epd_eis_brst_l2_extof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms3_epd_eis_brst_l2_extof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms3_epd_eis_brst_l2_extof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms3_epd_eis_brst_l2_extof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms3_epd_eis_brst_l2_extof_proton_P3_flux_t5]
      
      
      MMS3 ExTOF-Burst alpha_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_extof_helium_P3_counts_t0]
      
      
      ---> alpha_P3_counts_t1 [mms3_epd_eis_brst_l2_extof_helium_P3_counts_t1]
      
      
      ---> alpha_P3_counts_t2 [mms3_epd_eis_brst_l2_extof_helium_P3_counts_t2]
      
      
      ---> alpha_P3_counts_t3 [mms3_epd_eis_brst_l2_extof_helium_P3_counts_t3]
      
      
      ---> alpha_P3_counts_t4 [mms3_epd_eis_brst_l2_extof_helium_P3_counts_t4]
      
      
      ---> alpha_P3_counts_t5 [mms3_epd_eis_brst_l2_extof_helium_P3_counts_t5]
      
      
      MMS3 ExTOF-Burst alpha_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_extof_helium_P3_cps_t0]
      
      
      ---> alpha_P3_cps_t1 [mms3_epd_eis_brst_l2_extof_helium_P3_cps_t1]
      
      
      ---> alpha_P3_cps_t2 [mms3_epd_eis_brst_l2_extof_helium_P3_cps_t2]
      
      
      ---> alpha_P3_cps_t3 [mms3_epd_eis_brst_l2_extof_helium_P3_cps_t3]
      
      
      ---> alpha_P3_cps_t4 [mms3_epd_eis_brst_l2_extof_helium_P3_cps_t4]
      
      
      ---> alpha_P3_cps_t5 [mms3_epd_eis_brst_l2_extof_helium_P3_cps_t5]
      
      
      MMS3 ExTOF-Burst alpha_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_extof_helium_P3_flux_t0]
      
      
      ---> alpha_P3_flux_t1 [mms3_epd_eis_brst_l2_extof_helium_P3_flux_t1]
      
      
      ---> alpha_P3_flux_t2 [mms3_epd_eis_brst_l2_extof_helium_P3_flux_t2]
      
      
      ---> alpha_P3_flux_t3 [mms3_epd_eis_brst_l2_extof_helium_P3_flux_t3]
      
      
      ---> alpha_P3_flux_t4 [mms3_epd_eis_brst_l2_extof_helium_P3_flux_t4]
      
      
      ---> alpha_P3_flux_t5 [mms3_epd_eis_brst_l2_extof_helium_P3_flux_t5]
      
      
      MMS3 ExTOF-Burst oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_extof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms3_epd_eis_brst_l2_extof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms3_epd_eis_brst_l2_extof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms3_epd_eis_brst_l2_extof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms3_epd_eis_brst_l2_extof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms3_epd_eis_brst_l2_extof_oxygen_P3_counts_t5]
      
      
      MMS3 ExTOF-Burst oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_extof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms3_epd_eis_brst_l2_extof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms3_epd_eis_brst_l2_extof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms3_epd_eis_brst_l2_extof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms3_epd_eis_brst_l2_extof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms3_epd_eis_brst_l2_extof_oxygen_P3_cps_t5]
      
      
      MMS3 ExTOF-Burst oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_extof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms3_epd_eis_brst_l2_extof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms3_epd_eis_brst_l2_extof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms3_epd_eis_brst_l2_extof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms3_epd_eis_brst_l2_extof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms3_epd_eis_brst_l2_extof_oxygen_P3_flux_t5]
      
      
      MMS3 ExTOF-Burst dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_extof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms3_epd_eis_brst_l2_extof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms3_epd_eis_brst_l2_extof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms3_epd_eis_brst_l2_extof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms3_epd_eis_brst_l2_extof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms3_epd_eis_brst_l2_extof_dump_P3_counts_t5]
      
      
      MMS3 ExTOF-Burst dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_extof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms3_epd_eis_brst_l2_extof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms3_epd_eis_brst_l2_extof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms3_epd_eis_brst_l2_extof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms3_epd_eis_brst_l2_extof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms3_epd_eis_brst_l2_extof_dump_P4_counts_t5]
      
      
      MMS3 ExTOF-Burst dump_P5_counts_t0 [data available from 2020/09/24 to 2025/01/06] [mms3_epd_eis_brst_l2_extof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms3_epd_eis_brst_l2_extof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms3_epd_eis_brst_l2_extof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms3_epd_eis_brst_l2_extof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms3_epd_eis_brst_l2_extof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms3_epd_eis_brst_l2_extof_dump_P5_counts_t5]
      
      
      MMS3 ExTOF-Burst dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_extof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms3_epd_eis_brst_l2_extof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms3_epd_eis_brst_l2_extof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms3_epd_eis_brst_l2_extof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms3_epd_eis_brst_l2_extof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms3_epd_eis_brst_l2_extof_dump_P3_cps_t5]
      
      
      MMS3 ExTOF-Burst dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_extof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms3_epd_eis_brst_l2_extof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms3_epd_eis_brst_l2_extof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms3_epd_eis_brst_l2_extof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms3_epd_eis_brst_l2_extof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms3_epd_eis_brst_l2_extof_dump_P4_cps_t5]
      
      
      MMS3 ExTOF-Burst dump_P5_cps_t0 [data available from 2020/09/24 to 2025/01/06] [mms3_epd_eis_brst_l2_extof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms3_epd_eis_brst_l2_extof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms3_epd_eis_brst_l2_extof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms3_epd_eis_brst_l2_extof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms3_epd_eis_brst_l2_extof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms3_epd_eis_brst_l2_extof_dump_P5_cps_t5]
      
      
      MMS3 ExTOF-Burst dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_extof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms3_epd_eis_brst_l2_extof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms3_epd_eis_brst_l2_extof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms3_epd_eis_brst_l2_extof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms3_epd_eis_brst_l2_extof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms3_epd_eis_brst_l2_extof_dump_P3_flux_t5]
      
      
      MMS3 ExTOF-Burst dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_extof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms3_epd_eis_brst_l2_extof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms3_epd_eis_brst_l2_extof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms3_epd_eis_brst_l2_extof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms3_epd_eis_brst_l2_extof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms3_epd_eis_brst_l2_extof_dump_P4_flux_t5]
      
      
      MMS3 ExTOF-Burst dump_P5_flux_t0 [data available from 2020/09/24 to 2025/01/06] [mms3_epd_eis_brst_l2_extof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms3_epd_eis_brst_l2_extof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms3_epd_eis_brst_l2_extof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms3_epd_eis_brst_l2_extof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms3_epd_eis_brst_l2_extof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms3_epd_eis_brst_l2_extof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS3 [mms3_epd_eis_brst_l2_extof_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS3 [mms3_epd_eis_brst_l2_extof_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS3 [mms3_epd_eis_brst_l2_extof_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS3 [mms3_epd_eis_brst_l2_extof_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS3 [mms3_epd_eis_brst_l2_extof_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS3 [mms3_epd_eis_brst_l2_extof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS3 [mms3_epd_eis_brst_l2_extof_look_t0]
      
      
      Look Direction for Telescope 1 MMS3 [mms3_epd_eis_brst_l2_extof_look_t1]
      
      
      Look Direction for Telescope 2 MMS3 [mms3_epd_eis_brst_l2_extof_look_t2]
      
      
      Look Direction for Telescope 3 MMS3 [mms3_epd_eis_brst_l2_extof_look_t3]
      
      
      Look Direction for Telescope 4 MMS3 [mms3_epd_eis_brst_l2_extof_look_t4]
      
      
      Look Direction for Telescope 5 MMS3 [mms3_epd_eis_brst_l2_extof_look_t5]
      
      
      Magnetic Field BCS MMS3 [mms3_epd_eis_brst_l2_extof_b]
      
      
      Spacecraft position GSE MMS3 [mms3_epd_eis_brst_l2_extof_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS3 [mms3_epd_eis_brst_l2_extof_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS3 [mms3_epd_eis_brst_l2_extof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS3 [mms3_epd_eis_brst_l2_extof_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS3 [mms3_epd_eis_brst_l2_extof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS3 [mms3_epd_eis_brst_l2_extof_r]
      
      
      Dipole L-shell MMS3 [mms3_epd_eis_brst_l2_extof_l]
      
      
      Latitude in GSE Frame MMS3 [mms3_epd_eis_brst_l2_extof_gse_lat]
      
      
      Longitude in GSE Frame MMS3 [mms3_epd_eis_brst_l2_extof_gse_lon]
      
      
      Latitude in GSM Frame MMS3 [mms3_epd_eis_brst_l2_extof_gsm_lat]
      
      
      Longitude in GSM Frame MMS3 [mms3_epd_eis_brst_l2_extof_gsm_lon]
      
      
      Latitude in SM Frame MMS3 [mms3_epd_eis_brst_l2_extof_sm_lat]
      
      
      Longitude in SM Frame MMS3 [mms3_epd_eis_brst_l2_extof_sm_lon]
      
      
      Orbit number MMS3 [mms3_epd_eis_brst_l2_extof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS3 [mms3_epd_eis_brst_l2_extof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS3 [mms3_epd_eis_brst_l2_extof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS3 [mms3_epd_eis_brst_l2_extof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS3 [mms3_epd_eis_brst_l2_extof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS3 [mms3_epd_eis_brst_l2_extof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS3 [mms3_epd_eis_brst_l2_extof_ssd5]
      
      
      Valid Events Processed per second MMS3 [mms3_epd_eis_brst_l2_extof_vep]
      
      
      Start 0 Anode Count Rate MMS3 [mms3_epd_eis_brst_l2_extof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS3 [mms3_epd_eis_brst_l2_extof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS3 [mms3_epd_eis_brst_l2_extof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS3 [mms3_epd_eis_brst_l2_extof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS3 [mms3_epd_eis_brst_l2_extof_vtofxphe]
      
      
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MMS3_EPD-EIS_BRST_L2_PHXTOF (spase://NASA/NumericalData/MMS/3/EnergeticParticleDetector/EIS/Burst/Level2/PulseHeightByTimeOfFlight/PT0.605S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms3_epd_eis_brst_l2_phxtof_duration]
      
      
      ---> Instrument Deadtime [mms3_epd_eis_brst_l2_phxtof_deadtime]
      
      
      ---> Instrument Large Pixel in Use [mms3_epd_eis_brst_l2_phxtof_largepixel]
      
      
      ---> Spin [mms3_epd_eis_brst_l2_phxtof_spin]
      
      
      ---> Sector [mms3_epd_eis_brst_l2_phxtof_sector]
      
      
      ---> Quality Word [mms3_epd_eis_brst_l2_phxtof_quality]
      
      
      MMS3 PhxTOF-Burst proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms3_epd_eis_brst_l2_phxtof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms3_epd_eis_brst_l2_phxtof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms3_epd_eis_brst_l2_phxtof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms3_epd_eis_brst_l2_phxtof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms3_epd_eis_brst_l2_phxtof_proton_P6_counts_t5]
      
      
      MMS3 PhxTOF-Burst proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms3_epd_eis_brst_l2_phxtof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms3_epd_eis_brst_l2_phxtof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms3_epd_eis_brst_l2_phxtof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms3_epd_eis_brst_l2_phxtof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms3_epd_eis_brst_l2_phxtof_proton_P6_cps_t5]
      
      
      MMS3 PhxTOF-Burst proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms3_epd_eis_brst_l2_phxtof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms3_epd_eis_brst_l2_phxtof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms3_epd_eis_brst_l2_phxtof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms3_epd_eis_brst_l2_phxtof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms3_epd_eis_brst_l2_phxtof_proton_P6_flux_t5]
      
      
      MMS3 PhxTOF-Burst oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t5]
      
      
      MMS3 PhxTOF-Burst oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t5]
      
      
      MMS3 PhxTOF-Burst oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms3_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t5]
      
      
      MMS3 PhxTOF-Burst dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms3_epd_eis_brst_l2_phxtof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms3_epd_eis_brst_l2_phxtof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms3_epd_eis_brst_l2_phxtof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms3_epd_eis_brst_l2_phxtof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms3_epd_eis_brst_l2_phxtof_dump_P6_counts_t5]
      
      
      MMS3 PhxTOF-Burst dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms3_epd_eis_brst_l2_phxtof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms3_epd_eis_brst_l2_phxtof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms3_epd_eis_brst_l2_phxtof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms3_epd_eis_brst_l2_phxtof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms3_epd_eis_brst_l2_phxtof_dump_P6_cps_t5]
      
      
      MMS3 PhxTOF-Burst dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms3_epd_eis_brst_l2_phxtof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms3_epd_eis_brst_l2_phxtof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms3_epd_eis_brst_l2_phxtof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms3_epd_eis_brst_l2_phxtof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms3_epd_eis_brst_l2_phxtof_dump_P6_flux_t5]
      
      
      MMS3 PhxTOF-Burst proton_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms3_epd_eis_brst_l2_phxtof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms3_epd_eis_brst_l2_phxtof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms3_epd_eis_brst_l2_phxtof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms3_epd_eis_brst_l2_phxtof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms3_epd_eis_brst_l2_phxtof_proton_P5_counts_t5]
      
      
      MMS3 PhxTOF-Burst proton_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms3_epd_eis_brst_l2_phxtof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms3_epd_eis_brst_l2_phxtof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms3_epd_eis_brst_l2_phxtof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms3_epd_eis_brst_l2_phxtof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms3_epd_eis_brst_l2_phxtof_proton_P5_cps_t5]
      
      
      MMS3 PhxTOF-Burst proton_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms3_epd_eis_brst_l2_phxtof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms3_epd_eis_brst_l2_phxtof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms3_epd_eis_brst_l2_phxtof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms3_epd_eis_brst_l2_phxtof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms3_epd_eis_brst_l2_phxtof_proton_P5_flux_t5]
      
      
      MMS3 PhxTOF-Burst oxygen_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t5]
      
      
      MMS3 PhxTOF-Burst oxygen_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t5]
      
      
      MMS3 PhxTOF-Burst oxygen_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms3_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t5]
      
      
      MMS3 PhxTOF-Burst proton_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_phxtof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms3_epd_eis_brst_l2_phxtof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms3_epd_eis_brst_l2_phxtof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms3_epd_eis_brst_l2_phxtof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms3_epd_eis_brst_l2_phxtof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms3_epd_eis_brst_l2_phxtof_proton_P4_counts_t5]
      
      
      MMS3 PhxTOF-Burst proton_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_phxtof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms3_epd_eis_brst_l2_phxtof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms3_epd_eis_brst_l2_phxtof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms3_epd_eis_brst_l2_phxtof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms3_epd_eis_brst_l2_phxtof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms3_epd_eis_brst_l2_phxtof_proton_P4_cps_t5]
      
      
      MMS3 PhxTOF-Burst proton_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_phxtof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms3_epd_eis_brst_l2_phxtof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms3_epd_eis_brst_l2_phxtof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms3_epd_eis_brst_l2_phxtof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms3_epd_eis_brst_l2_phxtof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms3_epd_eis_brst_l2_phxtof_proton_P4_flux_t5]
      
      
      MMS3 PhxTOF-Burst oxygen_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t5]
      
      
      MMS3 PhxTOF-Burst oxygen_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t5]
      
      
      MMS3 PhxTOF-Burst oxygen_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms3_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t5]
      
      
      MMS3 PhxTOF-Burst proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_phxtof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms3_epd_eis_brst_l2_phxtof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms3_epd_eis_brst_l2_phxtof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms3_epd_eis_brst_l2_phxtof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms3_epd_eis_brst_l2_phxtof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms3_epd_eis_brst_l2_phxtof_proton_P3_counts_t5]
      
      
      MMS3 PhxTOF-Burst proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_phxtof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms3_epd_eis_brst_l2_phxtof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms3_epd_eis_brst_l2_phxtof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms3_epd_eis_brst_l2_phxtof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms3_epd_eis_brst_l2_phxtof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms3_epd_eis_brst_l2_phxtof_proton_P3_cps_t5]
      
      
      MMS3 PhxTOF-Burst proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_phxtof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms3_epd_eis_brst_l2_phxtof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms3_epd_eis_brst_l2_phxtof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms3_epd_eis_brst_l2_phxtof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms3_epd_eis_brst_l2_phxtof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms3_epd_eis_brst_l2_phxtof_proton_P3_flux_t5]
      
      
      MMS3 PhxTOF-Burst oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t5]
      
      
      MMS3 PhxTOF-Burst oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t5]
      
      
      MMS3 PhxTOF-Burst oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms3_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t5]
      
      
      MMS3 PhxTOF-Burst dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_phxtof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms3_epd_eis_brst_l2_phxtof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms3_epd_eis_brst_l2_phxtof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms3_epd_eis_brst_l2_phxtof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms3_epd_eis_brst_l2_phxtof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms3_epd_eis_brst_l2_phxtof_dump_P3_counts_t5]
      
      
      MMS3 PhxTOF-Burst dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_phxtof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms3_epd_eis_brst_l2_phxtof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms3_epd_eis_brst_l2_phxtof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms3_epd_eis_brst_l2_phxtof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms3_epd_eis_brst_l2_phxtof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms3_epd_eis_brst_l2_phxtof_dump_P4_counts_t5]
      
      
      MMS3 PhxTOF-Burst dump_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms3_epd_eis_brst_l2_phxtof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms3_epd_eis_brst_l2_phxtof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms3_epd_eis_brst_l2_phxtof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms3_epd_eis_brst_l2_phxtof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms3_epd_eis_brst_l2_phxtof_dump_P5_counts_t5]
      
      
      MMS3 PhxTOF-Burst dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_phxtof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms3_epd_eis_brst_l2_phxtof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms3_epd_eis_brst_l2_phxtof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms3_epd_eis_brst_l2_phxtof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms3_epd_eis_brst_l2_phxtof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms3_epd_eis_brst_l2_phxtof_dump_P3_cps_t5]
      
      
      MMS3 PhxTOF-Burst dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_phxtof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms3_epd_eis_brst_l2_phxtof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms3_epd_eis_brst_l2_phxtof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms3_epd_eis_brst_l2_phxtof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms3_epd_eis_brst_l2_phxtof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms3_epd_eis_brst_l2_phxtof_dump_P4_cps_t5]
      
      
      MMS3 PhxTOF-Burst dump_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms3_epd_eis_brst_l2_phxtof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms3_epd_eis_brst_l2_phxtof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms3_epd_eis_brst_l2_phxtof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms3_epd_eis_brst_l2_phxtof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms3_epd_eis_brst_l2_phxtof_dump_P5_cps_t5]
      
      
      MMS3 PhxTOF-Burst dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_brst_l2_phxtof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms3_epd_eis_brst_l2_phxtof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms3_epd_eis_brst_l2_phxtof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms3_epd_eis_brst_l2_phxtof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms3_epd_eis_brst_l2_phxtof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms3_epd_eis_brst_l2_phxtof_dump_P3_flux_t5]
      
      
      MMS3 PhxTOF-Burst dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_brst_l2_phxtof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms3_epd_eis_brst_l2_phxtof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms3_epd_eis_brst_l2_phxtof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms3_epd_eis_brst_l2_phxtof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms3_epd_eis_brst_l2_phxtof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms3_epd_eis_brst_l2_phxtof_dump_P4_flux_t5]
      
      
      MMS3 PhxTOF-Burst dump_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_brst_l2_phxtof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms3_epd_eis_brst_l2_phxtof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms3_epd_eis_brst_l2_phxtof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms3_epd_eis_brst_l2_phxtof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms3_epd_eis_brst_l2_phxtof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms3_epd_eis_brst_l2_phxtof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS3 [mms3_epd_eis_brst_l2_phxtof_pitch_angle_t0]
      
      
      ---> Pitch Angle for Telescope 1 MMS3 [mms3_epd_eis_brst_l2_phxtof_pitch_angle_t1]
      
      
      ---> Pitch Angle for Telescope 2 MMS3 [mms3_epd_eis_brst_l2_phxtof_pitch_angle_t2]
      
      
      ---> Pitch Angle for Telescope 3 MMS3 [mms3_epd_eis_brst_l2_phxtof_pitch_angle_t3]
      
      
      ---> Pitch Angle for Telescope 4 MMS3 [mms3_epd_eis_brst_l2_phxtof_pitch_angle_t4]
      
      
      ---> Pitch Angle for Telescope 5 MMS3 [mms3_epd_eis_brst_l2_phxtof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS3 [mms3_epd_eis_brst_l2_phxtof_look_t0]
      
      
      ---> Look Direction for Telescope 1 MMS3 [mms3_epd_eis_brst_l2_phxtof_look_t1]
      
      
      ---> Look Direction for Telescope 2 MMS3 [mms3_epd_eis_brst_l2_phxtof_look_t2]
      
      
      ---> Look Direction for Telescope 3 MMS3 [mms3_epd_eis_brst_l2_phxtof_look_t3]
      
      
      ---> Look Direction for Telescope 4 MMS3 [mms3_epd_eis_brst_l2_phxtof_look_t4]
      
      
      ---> Look Direction for Telescope 5 MMS3 [mms3_epd_eis_brst_l2_phxtof_look_t5]
      
      
      Magnetic Field BCS MMS3 [mms3_epd_eis_brst_l2_phxtof_b]
      
      
      Spacecraft position GSE MMS3 [mms3_epd_eis_brst_l2_phxtof_position_gse]
      
      
      ---> Spacecraft position in GSM coordinates MMS3 [mms3_epd_eis_brst_l2_phxtof_position_gsm]
      
      
      ---> Spacecraft-Moon vector in GSE coordinates MMS3 [mms3_epd_eis_brst_l2_phxtof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS3 [mms3_epd_eis_brst_l2_phxtof_sc_to_gse]
      
      
      ---> Transformation Matrix GSE to GSM Frame MMS3 [mms3_epd_eis_brst_l2_phxtof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS3 [mms3_epd_eis_brst_l2_phxtof_r]
      
      
      Dipole L-shell MMS3 [mms3_epd_eis_brst_l2_phxtof_l]
      
      
      Latitude in GSE Frame MMS3 [mms3_epd_eis_brst_l2_phxtof_gse_lat]
      
      
      Longitude in GSE Frame MMS3 [mms3_epd_eis_brst_l2_phxtof_gse_lon]
      
      
      Latitude in GSM Frame MMS3 [mms3_epd_eis_brst_l2_phxtof_gsm_lat]
      
      
      Longitude in GSM Frame MMS3 [mms3_epd_eis_brst_l2_phxtof_gsm_lon]
      
      
      Latitude in SM Frame MMS3 [mms3_epd_eis_brst_l2_phxtof_sm_lat]
      
      
      Longitude in SM Frame MMS3 [mms3_epd_eis_brst_l2_phxtof_sm_lon]
      
      
      Orbit number MMS3 [mms3_epd_eis_brst_l2_phxtof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS3 [mms3_epd_eis_brst_l2_phxtof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS3 [mms3_epd_eis_brst_l2_phxtof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS3 [mms3_epd_eis_brst_l2_phxtof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS3 [mms3_epd_eis_brst_l2_phxtof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS3 [mms3_epd_eis_brst_l2_phxtof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS3 [mms3_epd_eis_brst_l2_phxtof_ssd5]
      
      
      Valid Events Processed per second MMS3 [mms3_epd_eis_brst_l2_phxtof_vep]
      
      
      Start 0 Anode Count Rate MMS3 [mms3_epd_eis_brst_l2_phxtof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS3 [mms3_epd_eis_brst_l2_phxtof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS3 [mms3_epd_eis_brst_l2_phxtof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS3 [mms3_epd_eis_brst_l2_phxtof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS3 [mms3_epd_eis_brst_l2_phxtof_vtofxphe]
      
      
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MMS3_EPD-EIS_SRVY_L2_ELECTRONENERGY (spase://NASA/NumericalData/MMS/3/EnergeticParticleDetector/EIS/Survey/Level2/ElectronEnergySpectra/PT2.42S)
Description
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Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms3_epd_eis_srvy_l2_electronenergy_duration]
      
      
      Instrument Deadtime [mms3_epd_eis_srvy_l2_electronenergy_deadtime]
      
      
      Instrument Large Pixel in Use [mms3_epd_eis_srvy_l2_electronenergy_largepixel]
      
      
      Spin [mms3_epd_eis_srvy_l2_electronenergy_spin]
      
      
      Sector [mms3_epd_eis_srvy_l2_electronenergy_sector]
      
      
      Quality Word [mms3_epd_eis_srvy_l2_electronenergy_quality]
      
      
      MMS3 ElectronEnergy-Survey electron_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t0]
      
      
      ---> electron_P6_counts_t1 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t1]
      
      
      ---> electron_P6_counts_t2 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t2]
      
      
      ---> electron_P6_counts_t3 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t3]
      
      
      ---> electron_P6_counts_t4 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t4]
      
      
      ---> electron_P6_counts_t5 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t5]
      
      
      MMS3 ElectronEnergy-Survey electron_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t0]
      
      
      ---> electron_P6_cps_t1 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t1]
      
      
      ---> electron_P6_cps_t2 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t2]
      
      
      ---> electron_P6_cps_t3 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t3]
      
      
      ---> electron_P6_cps_t4 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t4]
      
      
      ---> electron_P6_cps_t5 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t5]
      
      
      MMS3 ElectronEnergy-Survey electron_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t0]
      
      
      ---> electron_P6_flux_t1 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t1]
      
      
      ---> electron_P6_flux_t2 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t2]
      
      
      ---> electron_P6_flux_t3 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t3]
      
      
      ---> electron_P6_flux_t4 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t4]
      
      
      ---> electron_P6_flux_t5 [mms3_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t5]
      
      
      MMS3 ElectronEnergy-Survey dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t5]
      
      
      MMS3 ElectronEnergy-Survey dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t5]
      
      
      MMS3 ElectronEnergy-Survey dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms3_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t5]
      
      
      MMS3 ElectronEnergy-Survey electron_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t0]
      
      
      ---> electron_P5_counts_t1 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t1]
      
      
      ---> electron_P5_counts_t2 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t2]
      
      
      ---> electron_P5_counts_t3 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t3]
      
      
      ---> electron_P5_counts_t4 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t4]
      
      
      ---> electron_P5_counts_t5 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t5]
      
      
      MMS3 ElectronEnergy-Survey electron_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t0]
      
      
      ---> electron_P5_cps_t1 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t1]
      
      
      ---> electron_P5_cps_t2 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t2]
      
      
      ---> electron_P5_cps_t3 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t3]
      
      
      ---> electron_P5_cps_t4 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t4]
      
      
      ---> electron_P5_cps_t5 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t5]
      
      
      MMS3 ElectronEnergy-Survey electron_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t0]
      
      
      ---> electron_P5_flux_t1 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t1]
      
      
      ---> electron_P5_flux_t2 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t2]
      
      
      ---> electron_P5_flux_t3 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t3]
      
      
      ---> electron_P5_flux_t4 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t4]
      
      
      ---> electron_P5_flux_t5 [mms3_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t5]
      
      
      MMS3 ElectronEnergy-Survey electron_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t0]
      
      
      ---> electron_P4_counts_t1 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t1]
      
      
      ---> electron_P4_counts_t2 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t2]
      
      
      ---> electron_P4_counts_t3 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t3]
      
      
      ---> electron_P4_counts_t4 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t4]
      
      
      ---> electron_P4_counts_t5 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t5]
      
      
      MMS3 ElectronEnergy-Survey electron_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t0]
      
      
      ---> electron_P4_cps_t1 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t1]
      
      
      ---> electron_P4_cps_t2 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t2]
      
      
      ---> electron_P4_cps_t3 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t3]
      
      
      ---> electron_P4_cps_t4 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t4]
      
      
      ---> electron_P4_cps_t5 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t5]
      
      
      MMS3 ElectronEnergy-Survey electron_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t0]
      
      
      ---> electron_P4_flux_t1 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t1]
      
      
      ---> electron_P4_flux_t2 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t2]
      
      
      ---> electron_P4_flux_t3 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t3]
      
      
      ---> electron_P4_flux_t4 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t4]
      
      
      ---> electron_P4_flux_t5 [mms3_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t5]
      
      
      MMS3 ElectronEnergy-Survey electron_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t0]
      
      
      ---> electron_P3_counts_t1 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t1]
      
      
      ---> electron_P3_counts_t2 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t2]
      
      
      ---> electron_P3_counts_t3 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t3]
      
      
      ---> electron_P3_counts_t4 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t4]
      
      
      ---> electron_P3_counts_t5 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t5]
      
      
      MMS3 ElectronEnergy-Survey electron_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t0]
      
      
      ---> electron_P3_cps_t1 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t1]
      
      
      ---> electron_P3_cps_t2 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t2]
      
      
      ---> electron_P3_cps_t3 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t3]
      
      
      ---> electron_P3_cps_t4 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t4]
      
      
      ---> electron_P3_cps_t5 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t5]
      
      
      MMS3 ElectronEnergy-Survey electron_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t0]
      
      
      ---> electron_P3_flux_t1 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t1]
      
      
      ---> electron_P3_flux_t2 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t2]
      
      
      ---> electron_P3_flux_t3 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t3]
      
      
      ---> electron_P3_flux_t4 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t4]
      
      
      ---> electron_P3_flux_t5 [mms3_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t5]
      
      
      MMS3 ElectronEnergy-Survey dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t5]
      
      
      MMS3 ElectronEnergy-Survey dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t5]
      
      
      MMS3 ElectronEnergy-Survey dump_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t5]
      
      
      MMS3 ElectronEnergy-Survey dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t5]
      
      
      MMS3 ElectronEnergy-Survey dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t5]
      
      
      MMS3 ElectronEnergy-Survey dump_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t5]
      
      
      MMS3 ElectronEnergy-Survey dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms3_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t5]
      
      
      MMS3 ElectronEnergy-Survey dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms3_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t5]
      
      
      MMS3 ElectronEnergy-Survey dump_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms3_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS3 [mms3_epd_eis_srvy_l2_electronenergy_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS3 [mms3_epd_eis_srvy_l2_electronenergy_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS3 [mms3_epd_eis_srvy_l2_electronenergy_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS3 [mms3_epd_eis_srvy_l2_electronenergy_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS3 [mms3_epd_eis_srvy_l2_electronenergy_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS3 [mms3_epd_eis_srvy_l2_electronenergy_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS3 [mms3_epd_eis_srvy_l2_electronenergy_look_t0]
      
      
      Look Direction for Telescope 1 MMS3 [mms3_epd_eis_srvy_l2_electronenergy_look_t1]
      
      
      Look Direction for Telescope 2 MMS3 [mms3_epd_eis_srvy_l2_electronenergy_look_t2]
      
      
      Look Direction for Telescope 3 MMS3 [mms3_epd_eis_srvy_l2_electronenergy_look_t3]
      
      
      Look Direction for Telescope 4 MMS3 [mms3_epd_eis_srvy_l2_electronenergy_look_t4]
      
      
      Look Direction for Telescope 5 MMS3 [mms3_epd_eis_srvy_l2_electronenergy_look_t5]
      
      
      Magnetic Field BCS MMS3 [mms3_epd_eis_srvy_l2_electronenergy_b]
      
      
      Spacecraft position GSE MMS3 [mms3_epd_eis_srvy_l2_electronenergy_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS3 [mms3_epd_eis_srvy_l2_electronenergy_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS3 [mms3_epd_eis_srvy_l2_electronenergy_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS3 [mms3_epd_eis_srvy_l2_electronenergy_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS3 [mms3_epd_eis_srvy_l2_electronenergy_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS3 [mms3_epd_eis_srvy_l2_electronenergy_r]
      
      
      Dipole L-shell MMS3 [mms3_epd_eis_srvy_l2_electronenergy_l]
      
      
      Latitude in GSE Frame MMS3 [mms3_epd_eis_srvy_l2_electronenergy_gse_lat]
      
      
      Longitude in GSE Frame MMS3 [mms3_epd_eis_srvy_l2_electronenergy_gse_lon]
      
      
      Latitude in GSM Frame MMS3 [mms3_epd_eis_srvy_l2_electronenergy_gsm_lat]
      
      
      Longitude in GSM Frame MMS3 [mms3_epd_eis_srvy_l2_electronenergy_gsm_lon]
      
      
      Latitude in SM Frame MMS3 [mms3_epd_eis_srvy_l2_electronenergy_sm_lat]
      
      
      Longitude in SM Frame MMS3 [mms3_epd_eis_srvy_l2_electronenergy_sm_lon]
      
      
      Orbit number MMS3 [mms3_epd_eis_srvy_l2_electronenergy_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS3 [mms3_epd_eis_srvy_l2_electronenergy_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS3 [mms3_epd_eis_srvy_l2_electronenergy_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS3 [mms3_epd_eis_srvy_l2_electronenergy_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS3 [mms3_epd_eis_srvy_l2_electronenergy_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS3 [mms3_epd_eis_srvy_l2_electronenergy_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS3 [mms3_epd_eis_srvy_l2_electronenergy_ssd5]
      
      
      Valid Events Processed per second MMS3 [mms3_epd_eis_srvy_l2_electronenergy_vep]
      
      
      Valid Electron Events per second MMS3 [mms3_epd_eis_srvy_l2_electronenergy_vee]
      
      
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MMS3_EPD-EIS_SRVY_L2_EXTOF (spase://NASA/NumericalData/MMS/3/EnergeticParticleDetector/EIS/Survey/Level2/EnergyByTimeOfFlight/PT2.42S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms3_epd_eis_srvy_l2_extof_duration]
      
      
      ---> Instrument Deadtime [mms3_epd_eis_srvy_l2_extof_deadtime]
      
      
      ---> Instrument Large Pixel in Use [mms3_epd_eis_srvy_l2_extof_largepixel]
      
      
      ---> Spin [mms3_epd_eis_srvy_l2_extof_spin]
      
      
      ---> Sector [mms3_epd_eis_srvy_l2_extof_sector]
      
      
      ---> Quality Word [mms3_epd_eis_srvy_l2_extof_quality]
      
      
      MMS3 ExTOF-Survey proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_extof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms3_epd_eis_srvy_l2_extof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms3_epd_eis_srvy_l2_extof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms3_epd_eis_srvy_l2_extof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms3_epd_eis_srvy_l2_extof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms3_epd_eis_srvy_l2_extof_proton_P6_counts_t5]
      
      
      MMS3 ExTOF-Survey proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_extof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms3_epd_eis_srvy_l2_extof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms3_epd_eis_srvy_l2_extof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms3_epd_eis_srvy_l2_extof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms3_epd_eis_srvy_l2_extof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms3_epd_eis_srvy_l2_extof_proton_P6_cps_t5]
      
      
      MMS3 ExTOF-Survey proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_extof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms3_epd_eis_srvy_l2_extof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms3_epd_eis_srvy_l2_extof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms3_epd_eis_srvy_l2_extof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms3_epd_eis_srvy_l2_extof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms3_epd_eis_srvy_l2_extof_proton_P6_flux_t5]
      
      
      MMS3 ExTOF-Survey helium_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_extof_helium_P6_counts_t0]
      
      
      ---> helium_P6_counts_t1 [mms3_epd_eis_srvy_l2_extof_helium_P6_counts_t1]
      
      
      ---> helium_P6_counts_t2 [mms3_epd_eis_srvy_l2_extof_helium_P6_counts_t2]
      
      
      ---> helium_P6_counts_t3 [mms3_epd_eis_srvy_l2_extof_helium_P6_counts_t3]
      
      
      ---> helium_P6_counts_t4 [mms3_epd_eis_srvy_l2_extof_helium_P6_counts_t4]
      
      
      ---> helium_P6_counts_t5 [mms3_epd_eis_srvy_l2_extof_helium_P6_counts_t5]
      
      
      MMS3 ExTOF-Survey helium_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_extof_helium_P6_cps_t0]
      
      
      ---> helium_P6_cps_t1 [mms3_epd_eis_srvy_l2_extof_helium_P6_cps_t1]
      
      
      ---> helium_P6_cps_t2 [mms3_epd_eis_srvy_l2_extof_helium_P6_cps_t2]
      
      
      ---> helium_P6_cps_t3 [mms3_epd_eis_srvy_l2_extof_helium_P6_cps_t3]
      
      
      ---> helium_P6_cps_t4 [mms3_epd_eis_srvy_l2_extof_helium_P6_cps_t4]
      
      
      ---> helium_P6_cps_t5 [mms3_epd_eis_srvy_l2_extof_helium_P6_cps_t5]
      
      
      MMS3 ExTOF-Survey helium_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_extof_helium_P6_flux_t0]
      
      
      ---> helium_P6_flux_t1 [mms3_epd_eis_srvy_l2_extof_helium_P6_flux_t1]
      
      
      ---> helium_P6_flux_t2 [mms3_epd_eis_srvy_l2_extof_helium_P6_flux_t2]
      
      
      ---> helium_P6_flux_t3 [mms3_epd_eis_srvy_l2_extof_helium_P6_flux_t3]
      
      
      ---> helium_P6_flux_t4 [mms3_epd_eis_srvy_l2_extof_helium_P6_flux_t4]
      
      
      ---> helium_P6_flux_t5 [mms3_epd_eis_srvy_l2_extof_helium_P6_flux_t5]
      
      
      MMS3 ExTOF-Survey oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_extof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_counts_t5]
      
      
      MMS3 ExTOF-Survey oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_extof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_cps_t5]
      
      
      MMS3 ExTOF-Survey oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_extof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms3_epd_eis_srvy_l2_extof_oxygen_P6_flux_t5]
      
      
      MMS3 ExTOF-Survey dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_extof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms3_epd_eis_srvy_l2_extof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms3_epd_eis_srvy_l2_extof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms3_epd_eis_srvy_l2_extof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms3_epd_eis_srvy_l2_extof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms3_epd_eis_srvy_l2_extof_dump_P6_counts_t5]
      
      
      MMS3 ExTOF-Survey dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_extof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms3_epd_eis_srvy_l2_extof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms3_epd_eis_srvy_l2_extof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms3_epd_eis_srvy_l2_extof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms3_epd_eis_srvy_l2_extof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms3_epd_eis_srvy_l2_extof_dump_P6_cps_t5]
      
      
      MMS3 ExTOF-Survey dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_extof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms3_epd_eis_srvy_l2_extof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms3_epd_eis_srvy_l2_extof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms3_epd_eis_srvy_l2_extof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms3_epd_eis_srvy_l2_extof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms3_epd_eis_srvy_l2_extof_dump_P6_flux_t5]
      
      
      MMS3 ExTOF-Survey proton_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms3_epd_eis_srvy_l2_extof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms3_epd_eis_srvy_l2_extof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms3_epd_eis_srvy_l2_extof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms3_epd_eis_srvy_l2_extof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms3_epd_eis_srvy_l2_extof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms3_epd_eis_srvy_l2_extof_proton_P5_counts_t5]
      
      
      MMS3 ExTOF-Survey proton_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms3_epd_eis_srvy_l2_extof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms3_epd_eis_srvy_l2_extof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms3_epd_eis_srvy_l2_extof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms3_epd_eis_srvy_l2_extof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms3_epd_eis_srvy_l2_extof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms3_epd_eis_srvy_l2_extof_proton_P5_cps_t5]
      
      
      MMS3 ExTOF-Survey proton_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms3_epd_eis_srvy_l2_extof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms3_epd_eis_srvy_l2_extof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms3_epd_eis_srvy_l2_extof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms3_epd_eis_srvy_l2_extof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms3_epd_eis_srvy_l2_extof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms3_epd_eis_srvy_l2_extof_proton_P5_flux_t5]
      
      
      MMS3 ExTOF-Survey oxygen_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms3_epd_eis_srvy_l2_extof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_counts_t5]
      
      
      MMS3 ExTOF-Survey oxygen_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms3_epd_eis_srvy_l2_extof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_cps_t5]
      
      
      MMS3 ExTOF-Survey oxygen_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms3_epd_eis_srvy_l2_extof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms3_epd_eis_srvy_l2_extof_oxygen_P5_flux_t5]
      
      
      MMS3 ExTOF-Survey helium_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms3_epd_eis_srvy_l2_extof_helium_P5_counts_t0]
      
      
      ---> helium_P5_counts_t1 [mms3_epd_eis_srvy_l2_extof_helium_P5_counts_t1]
      
      
      ---> helium_P5_counts_t2 [mms3_epd_eis_srvy_l2_extof_helium_P5_counts_t2]
      
      
      ---> helium_P5_counts_t3 [mms3_epd_eis_srvy_l2_extof_helium_P5_counts_t3]
      
      
      ---> helium_P5_counts_t4 [mms3_epd_eis_srvy_l2_extof_helium_P5_counts_t4]
      
      
      ---> helium_P5_counts_t5 [mms3_epd_eis_srvy_l2_extof_helium_P5_counts_t5]
      
      
      MMS3 ExTOF-Survey helium_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms3_epd_eis_srvy_l2_extof_helium_P5_cps_t0]
      
      
      ---> helium_P5_cps_t1 [mms3_epd_eis_srvy_l2_extof_helium_P5_cps_t1]
      
      
      ---> helium_P5_cps_t2 [mms3_epd_eis_srvy_l2_extof_helium_P5_cps_t2]
      
      
      ---> helium_P5_cps_t3 [mms3_epd_eis_srvy_l2_extof_helium_P5_cps_t3]
      
      
      ---> helium_P5_cps_t4 [mms3_epd_eis_srvy_l2_extof_helium_P5_cps_t4]
      
      
      ---> helium_P5_cps_t5 [mms3_epd_eis_srvy_l2_extof_helium_P5_cps_t5]
      
      
      MMS3 ExTOF-Survey helium_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms3_epd_eis_srvy_l2_extof_helium_P5_flux_t0]
      
      
      ---> helium_P5_flux_t1 [mms3_epd_eis_srvy_l2_extof_helium_P5_flux_t1]
      
      
      ---> helium_P5_flux_t2 [mms3_epd_eis_srvy_l2_extof_helium_P5_flux_t2]
      
      
      ---> helium_P5_flux_t3 [mms3_epd_eis_srvy_l2_extof_helium_P5_flux_t3]
      
      
      ---> helium_P5_flux_t4 [mms3_epd_eis_srvy_l2_extof_helium_P5_flux_t4]
      
      
      ---> helium_P5_flux_t5 [mms3_epd_eis_srvy_l2_extof_helium_P5_flux_t5]
      
      
      MMS3 ExTOF-Survey proton_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms3_epd_eis_srvy_l2_extof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms3_epd_eis_srvy_l2_extof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms3_epd_eis_srvy_l2_extof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms3_epd_eis_srvy_l2_extof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms3_epd_eis_srvy_l2_extof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms3_epd_eis_srvy_l2_extof_proton_P4_counts_t5]
      
      
      MMS3 ExTOF-Survey proton_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms3_epd_eis_srvy_l2_extof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms3_epd_eis_srvy_l2_extof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms3_epd_eis_srvy_l2_extof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms3_epd_eis_srvy_l2_extof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms3_epd_eis_srvy_l2_extof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms3_epd_eis_srvy_l2_extof_proton_P4_cps_t5]
      
      
      MMS3 ExTOF-Survey proton_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms3_epd_eis_srvy_l2_extof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms3_epd_eis_srvy_l2_extof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms3_epd_eis_srvy_l2_extof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms3_epd_eis_srvy_l2_extof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms3_epd_eis_srvy_l2_extof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms3_epd_eis_srvy_l2_extof_proton_P4_flux_t5]
      
      
      MMS3 ExTOF-Survey alpha_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms3_epd_eis_srvy_l2_extof_helium_P4_counts_t0]
      
      
      ---> alpha_P4_counts_t1 [mms3_epd_eis_srvy_l2_extof_helium_P4_counts_t1]
      
      
      ---> alpha_P4_counts_t2 [mms3_epd_eis_srvy_l2_extof_helium_P4_counts_t2]
      
      
      ---> alpha_P4_counts_t3 [mms3_epd_eis_srvy_l2_extof_helium_P4_counts_t3]
      
      
      ---> alpha_P4_counts_t4 [mms3_epd_eis_srvy_l2_extof_helium_P4_counts_t4]
      
      
      ---> alpha_P4_counts_t5 [mms3_epd_eis_srvy_l2_extof_helium_P4_counts_t5]
      
      
      MMS3 ExTOF-Survey alpha_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms3_epd_eis_srvy_l2_extof_helium_P4_cps_t0]
      
      
      ---> alpha_P4_cps_t1 [mms3_epd_eis_srvy_l2_extof_helium_P4_cps_t1]
      
      
      ---> alpha_P4_cps_t2 [mms3_epd_eis_srvy_l2_extof_helium_P4_cps_t2]
      
      
      ---> alpha_P4_cps_t3 [mms3_epd_eis_srvy_l2_extof_helium_P4_cps_t3]
      
      
      ---> alpha_P4_cps_t4 [mms3_epd_eis_srvy_l2_extof_helium_P4_cps_t4]
      
      
      ---> alpha_P4_cps_t5 [mms3_epd_eis_srvy_l2_extof_helium_P4_cps_t5]
      
      
      MMS3 ExTOF-Survey alpha_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms3_epd_eis_srvy_l2_extof_helium_P4_flux_t0]
      
      
      ---> alpha_P4_flux_t1 [mms3_epd_eis_srvy_l2_extof_helium_P4_flux_t1]
      
      
      ---> alpha_P4_flux_t2 [mms3_epd_eis_srvy_l2_extof_helium_P4_flux_t2]
      
      
      ---> alpha_P4_flux_t3 [mms3_epd_eis_srvy_l2_extof_helium_P4_flux_t3]
      
      
      ---> alpha_P4_flux_t4 [mms3_epd_eis_srvy_l2_extof_helium_P4_flux_t4]
      
      
      ---> alpha_P4_flux_t5 [mms3_epd_eis_srvy_l2_extof_helium_P4_flux_t5]
      
      
      MMS3 ExTOF-Survey oxygen_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms3_epd_eis_srvy_l2_extof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_counts_t5]
      
      
      MMS3 ExTOF-Survey oxygen_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms3_epd_eis_srvy_l2_extof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_cps_t5]
      
      
      MMS3 ExTOF-Survey oxygen_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms3_epd_eis_srvy_l2_extof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms3_epd_eis_srvy_l2_extof_oxygen_P4_flux_t5]
      
      
      MMS3 ExTOF-Survey proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_extof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms3_epd_eis_srvy_l2_extof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms3_epd_eis_srvy_l2_extof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms3_epd_eis_srvy_l2_extof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms3_epd_eis_srvy_l2_extof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms3_epd_eis_srvy_l2_extof_proton_P3_counts_t5]
      
      
      MMS3 ExTOF-Survey proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_extof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms3_epd_eis_srvy_l2_extof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms3_epd_eis_srvy_l2_extof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms3_epd_eis_srvy_l2_extof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms3_epd_eis_srvy_l2_extof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms3_epd_eis_srvy_l2_extof_proton_P3_cps_t5]
      
      
      MMS3 ExTOF-Survey proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_extof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms3_epd_eis_srvy_l2_extof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms3_epd_eis_srvy_l2_extof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms3_epd_eis_srvy_l2_extof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms3_epd_eis_srvy_l2_extof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms3_epd_eis_srvy_l2_extof_proton_P3_flux_t5]
      
      
      MMS3 ExTOF-Survey alpha_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_extof_helium_P3_counts_t0]
      
      
      ---> alpha_P3_counts_t1 [mms3_epd_eis_srvy_l2_extof_helium_P3_counts_t1]
      
      
      ---> alpha_P3_counts_t2 [mms3_epd_eis_srvy_l2_extof_helium_P3_counts_t2]
      
      
      ---> alpha_P3_counts_t3 [mms3_epd_eis_srvy_l2_extof_helium_P3_counts_t3]
      
      
      ---> alpha_P3_counts_t4 [mms3_epd_eis_srvy_l2_extof_helium_P3_counts_t4]
      
      
      ---> alpha_P3_counts_t5 [mms3_epd_eis_srvy_l2_extof_helium_P3_counts_t5]
      
      
      MMS3 ExTOF-Survey alpha_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_extof_helium_P3_cps_t0]
      
      
      ---> alpha_P3_cps_t1 [mms3_epd_eis_srvy_l2_extof_helium_P3_cps_t1]
      
      
      ---> alpha_P3_cps_t2 [mms3_epd_eis_srvy_l2_extof_helium_P3_cps_t2]
      
      
      ---> alpha_P3_cps_t3 [mms3_epd_eis_srvy_l2_extof_helium_P3_cps_t3]
      
      
      ---> alpha_P3_cps_t4 [mms3_epd_eis_srvy_l2_extof_helium_P3_cps_t4]
      
      
      ---> alpha_P3_cps_t5 [mms3_epd_eis_srvy_l2_extof_helium_P3_cps_t5]
      
      
      MMS3 ExTOF-Survey alpha_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_extof_helium_P3_flux_t0]
      
      
      ---> alpha_P3_flux_t1 [mms3_epd_eis_srvy_l2_extof_helium_P3_flux_t1]
      
      
      ---> alpha_P3_flux_t2 [mms3_epd_eis_srvy_l2_extof_helium_P3_flux_t2]
      
      
      ---> alpha_P3_flux_t3 [mms3_epd_eis_srvy_l2_extof_helium_P3_flux_t3]
      
      
      ---> alpha_P3_flux_t4 [mms3_epd_eis_srvy_l2_extof_helium_P3_flux_t4]
      
      
      ---> alpha_P3_flux_t5 [mms3_epd_eis_srvy_l2_extof_helium_P3_flux_t5]
      
      
      MMS3 ExTOF-Survey oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_extof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_counts_t5]
      
      
      MMS3 ExTOF-Survey oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_extof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_cps_t5]
      
      
      MMS3 ExTOF-Survey oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_extof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms3_epd_eis_srvy_l2_extof_oxygen_P3_flux_t5]
      
      
      MMS3 ExTOF-Survey dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_extof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms3_epd_eis_srvy_l2_extof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms3_epd_eis_srvy_l2_extof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms3_epd_eis_srvy_l2_extof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms3_epd_eis_srvy_l2_extof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms3_epd_eis_srvy_l2_extof_dump_P3_counts_t5]
      
      
      MMS3 ExTOF-Survey dump_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms3_epd_eis_srvy_l2_extof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms3_epd_eis_srvy_l2_extof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms3_epd_eis_srvy_l2_extof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms3_epd_eis_srvy_l2_extof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms3_epd_eis_srvy_l2_extof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms3_epd_eis_srvy_l2_extof_dump_P4_counts_t5]
      
      
      MMS3 ExTOF-Survey dump_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms3_epd_eis_srvy_l2_extof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms3_epd_eis_srvy_l2_extof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms3_epd_eis_srvy_l2_extof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms3_epd_eis_srvy_l2_extof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms3_epd_eis_srvy_l2_extof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms3_epd_eis_srvy_l2_extof_dump_P5_counts_t5]
      
      
      MMS3 ExTOF-Survey dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_extof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms3_epd_eis_srvy_l2_extof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms3_epd_eis_srvy_l2_extof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms3_epd_eis_srvy_l2_extof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms3_epd_eis_srvy_l2_extof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms3_epd_eis_srvy_l2_extof_dump_P3_cps_t5]
      
      
      MMS3 ExTOF-Survey dump_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms3_epd_eis_srvy_l2_extof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms3_epd_eis_srvy_l2_extof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms3_epd_eis_srvy_l2_extof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms3_epd_eis_srvy_l2_extof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms3_epd_eis_srvy_l2_extof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms3_epd_eis_srvy_l2_extof_dump_P4_cps_t5]
      
      
      MMS3 ExTOF-Survey dump_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms3_epd_eis_srvy_l2_extof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms3_epd_eis_srvy_l2_extof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms3_epd_eis_srvy_l2_extof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms3_epd_eis_srvy_l2_extof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms3_epd_eis_srvy_l2_extof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms3_epd_eis_srvy_l2_extof_dump_P5_cps_t5]
      
      
      MMS3 ExTOF-Survey dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_extof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms3_epd_eis_srvy_l2_extof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms3_epd_eis_srvy_l2_extof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms3_epd_eis_srvy_l2_extof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms3_epd_eis_srvy_l2_extof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms3_epd_eis_srvy_l2_extof_dump_P3_flux_t5]
      
      
      MMS3 ExTOF-Survey dump_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms3_epd_eis_srvy_l2_extof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms3_epd_eis_srvy_l2_extof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms3_epd_eis_srvy_l2_extof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms3_epd_eis_srvy_l2_extof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms3_epd_eis_srvy_l2_extof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms3_epd_eis_srvy_l2_extof_dump_P4_flux_t5]
      
      
      MMS3 ExTOF-Survey dump_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms3_epd_eis_srvy_l2_extof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms3_epd_eis_srvy_l2_extof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms3_epd_eis_srvy_l2_extof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms3_epd_eis_srvy_l2_extof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms3_epd_eis_srvy_l2_extof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms3_epd_eis_srvy_l2_extof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS3 [mms3_epd_eis_srvy_l2_extof_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS3 [mms3_epd_eis_srvy_l2_extof_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS3 [mms3_epd_eis_srvy_l2_extof_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS3 [mms3_epd_eis_srvy_l2_extof_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS3 [mms3_epd_eis_srvy_l2_extof_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS3 [mms3_epd_eis_srvy_l2_extof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS3 [mms3_epd_eis_srvy_l2_extof_look_t0]
      
      
      Look Direction for Telescope 1 MMS3 [mms3_epd_eis_srvy_l2_extof_look_t1]
      
      
      Look Direction for Telescope 2 MMS3 [mms3_epd_eis_srvy_l2_extof_look_t2]
      
      
      Look Direction for Telescope 3 MMS3 [mms3_epd_eis_srvy_l2_extof_look_t3]
      
      
      Look Direction for Telescope 4 MMS3 [mms3_epd_eis_srvy_l2_extof_look_t4]
      
      
      Look Direction for Telescope 5 MMS3 [mms3_epd_eis_srvy_l2_extof_look_t5]
      
      
      Magnetic Field BCS MMS3 [mms3_epd_eis_srvy_l2_extof_b]
      
      
      Spacecraft position GSE MMS3 [mms3_epd_eis_srvy_l2_extof_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS3 [mms3_epd_eis_srvy_l2_extof_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS3 [mms3_epd_eis_srvy_l2_extof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS3 [mms3_epd_eis_srvy_l2_extof_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS3 [mms3_epd_eis_srvy_l2_extof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS3 [mms3_epd_eis_srvy_l2_extof_r]
      
      
      Dipole L-shell MMS3 [mms3_epd_eis_srvy_l2_extof_l]
      
      
      Latitude in GSE Frame MMS3 [mms3_epd_eis_srvy_l2_extof_gse_lat]
      
      
      Longitude in GSE Frame MMS3 [mms3_epd_eis_srvy_l2_extof_gse_lon]
      
      
      Latitude in GSM Frame MMS3 [mms3_epd_eis_srvy_l2_extof_gsm_lat]
      
      
      Longitude in GSM Frame MMS3 [mms3_epd_eis_srvy_l2_extof_gsm_lon]
      
      
      Latitude in SM Frame MMS3 [mms3_epd_eis_srvy_l2_extof_sm_lat]
      
      
      Longitude in SM Frame MMS3 [mms3_epd_eis_srvy_l2_extof_sm_lon]
      
      
      Orbit number MMS3 [mms3_epd_eis_srvy_l2_extof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS3 [mms3_epd_eis_srvy_l2_extof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS3 [mms3_epd_eis_srvy_l2_extof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS3 [mms3_epd_eis_srvy_l2_extof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS3 [mms3_epd_eis_srvy_l2_extof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS3 [mms3_epd_eis_srvy_l2_extof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS3 [mms3_epd_eis_srvy_l2_extof_ssd5]
      
      
      Valid Events Processed per second MMS3 [mms3_epd_eis_srvy_l2_extof_vep]
      
      
      Start 0 Anode Count Rate MMS3 [mms3_epd_eis_srvy_l2_extof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS3 [mms3_epd_eis_srvy_l2_extof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS3 [mms3_epd_eis_srvy_l2_extof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS3 [mms3_epd_eis_srvy_l2_extof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS3 [mms3_epd_eis_srvy_l2_extof_vtofxphe]
      
      
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MMS3_EPD-EIS_SRVY_L2_PHXTOF (spase://NASA/NumericalData/MMS/3/EnergeticParticleDetector/EIS/Survey/Level2/PulseHeightByTimeOfFlight/PT2.42S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms3_epd_eis_srvy_l2_phxtof_duration]
      
      
      Instrument Deadtime [mms3_epd_eis_srvy_l2_phxtof_deadtime]
      
      
      Instrument Large Pixel in Use [mms3_epd_eis_srvy_l2_phxtof_largepixel]
      
      
      Spin [mms3_epd_eis_srvy_l2_phxtof_spin]
      
      
      Sector [mms3_epd_eis_srvy_l2_phxtof_sector]
      
      
      Quality Word [mms3_epd_eis_srvy_l2_phxtof_quality]
      
      
      MMS3 PhxTOF-Survey proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_counts_t5]
      
      
      MMS3 PhxTOF-Survey proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_cps_t5]
      
      
      MMS3 PhxTOF-Survey proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms3_epd_eis_srvy_l2_phxtof_proton_P6_flux_t5]
      
      
      MMS3 PhxTOF-Survey oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t5]
      
      
      MMS3 PhxTOF-Survey oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t5]
      
      
      MMS3 PhxTOF-Survey oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t5]
      
      
      MMS3 PhxTOF-Survey dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_counts_t5]
      
      
      MMS3 PhxTOF-Survey dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_cps_t5]
      
      
      MMS3 PhxTOF-Survey dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms3_epd_eis_srvy_l2_phxtof_dump_P6_flux_t5]
      
      
      MMS3 PhxTOF-Survey proton_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_counts_t5]
      
      
      MMS3 PhxTOF-Survey proton_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_cps_t5]
      
      
      MMS3 PhxTOF-Survey proton_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms3_epd_eis_srvy_l2_phxtof_proton_P5_flux_t5]
      
      
      MMS3 PhxTOF-Survey oxygen_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t5]
      
      
      MMS3 PhxTOF-Survey oxygen_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t5]
      
      
      MMS3 PhxTOF-Survey oxygen_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t5]
      
      
      MMS3 PhxTOF-Survey proton_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_phxtof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_counts_t5]
      
      
      MMS3 PhxTOF-Survey proton_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_phxtof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_cps_t5]
      
      
      MMS3 PhxTOF-Survey proton_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_phxtof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms3_epd_eis_srvy_l2_phxtof_proton_P4_flux_t5]
      
      
      MMS3 PhxTOF-Survey oxygen_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t5]
      
      
      MMS3 PhxTOF-Survey oxygen_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t5]
      
      
      MMS3 PhxTOF-Survey oxygen_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t5]
      
      
      MMS3 PhxTOF-Survey proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_phxtof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_counts_t5]
      
      
      MMS3 PhxTOF-Survey proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_phxtof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_cps_t5]
      
      
      MMS3 PhxTOF-Survey proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_phxtof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms3_epd_eis_srvy_l2_phxtof_proton_P3_flux_t5]
      
      
      MMS3 PhxTOF-Survey oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t5]
      
      
      MMS3 PhxTOF-Survey oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t5]
      
      
      MMS3 PhxTOF-Survey oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms3_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t5]
      
      
      MMS3 PhxTOF-Survey dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_phxtof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_counts_t5]
      
      
      MMS3 PhxTOF-Survey dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_phxtof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_counts_t5]
      
      
      MMS3 PhxTOF-Survey dump_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_counts_t5]
      
      
      MMS3 PhxTOF-Survey dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_phxtof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_cps_t5]
      
      
      MMS3 PhxTOF-Survey dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_phxtof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_cps_t5]
      
      
      MMS3 PhxTOF-Survey dump_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_cps_t5]
      
      
      MMS3 PhxTOF-Survey dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms3_epd_eis_srvy_l2_phxtof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms3_epd_eis_srvy_l2_phxtof_dump_P3_flux_t5]
      
      
      MMS3 PhxTOF-Survey dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms3_epd_eis_srvy_l2_phxtof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms3_epd_eis_srvy_l2_phxtof_dump_P4_flux_t5]
      
      
      MMS3 PhxTOF-Survey dump_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms3_epd_eis_srvy_l2_phxtof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms3_epd_eis_srvy_l2_phxtof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS3 [mms3_epd_eis_srvy_l2_phxtof_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS3 [mms3_epd_eis_srvy_l2_phxtof_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS3 [mms3_epd_eis_srvy_l2_phxtof_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS3 [mms3_epd_eis_srvy_l2_phxtof_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS3 [mms3_epd_eis_srvy_l2_phxtof_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS3 [mms3_epd_eis_srvy_l2_phxtof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS3 [mms3_epd_eis_srvy_l2_phxtof_look_t0]
      
      
      Look Direction for Telescope 1 MMS3 [mms3_epd_eis_srvy_l2_phxtof_look_t1]
      
      
      Look Direction for Telescope 2 MMS3 [mms3_epd_eis_srvy_l2_phxtof_look_t2]
      
      
      Look Direction for Telescope 3 MMS3 [mms3_epd_eis_srvy_l2_phxtof_look_t3]
      
      
      Look Direction for Telescope 4 MMS3 [mms3_epd_eis_srvy_l2_phxtof_look_t4]
      
      
      Look Direction for Telescope 5 MMS3 [mms3_epd_eis_srvy_l2_phxtof_look_t5]
      
      
      Magnetic Field BCS MMS3 [mms3_epd_eis_srvy_l2_phxtof_b]
      
      
      Spacecraft position GSE MMS3 [mms3_epd_eis_srvy_l2_phxtof_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS3 [mms3_epd_eis_srvy_l2_phxtof_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS3 [mms3_epd_eis_srvy_l2_phxtof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS3 [mms3_epd_eis_srvy_l2_phxtof_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS3 [mms3_epd_eis_srvy_l2_phxtof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS3 [mms3_epd_eis_srvy_l2_phxtof_r]
      
      
      Dipole L-shell MMS3 [mms3_epd_eis_srvy_l2_phxtof_l]
      
      
      Latitude in GSE Frame MMS3 [mms3_epd_eis_srvy_l2_phxtof_gse_lat]
      
      
      Longitude in GSE Frame MMS3 [mms3_epd_eis_srvy_l2_phxtof_gse_lon]
      
      
      Latitude in GSM Frame MMS3 [mms3_epd_eis_srvy_l2_phxtof_gsm_lat]
      
      
      Longitude in GSM Frame MMS3 [mms3_epd_eis_srvy_l2_phxtof_gsm_lon]
      
      
      Latitude in SM Frame MMS3 [mms3_epd_eis_srvy_l2_phxtof_sm_lat]
      
      
      Longitude in SM Frame MMS3 [mms3_epd_eis_srvy_l2_phxtof_sm_lon]
      
      
      Orbit number MMS3 [mms3_epd_eis_srvy_l2_phxtof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS3 [mms3_epd_eis_srvy_l2_phxtof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS3 [mms3_epd_eis_srvy_l2_phxtof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS3 [mms3_epd_eis_srvy_l2_phxtof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS3 [mms3_epd_eis_srvy_l2_phxtof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS3 [mms3_epd_eis_srvy_l2_phxtof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS3 [mms3_epd_eis_srvy_l2_phxtof_ssd5]
      
      
      Valid Events Processed per second MMS3 [mms3_epd_eis_srvy_l2_phxtof_vep]
      
      
      Start 0 Anode Count Rate MMS3 [mms3_epd_eis_srvy_l2_phxtof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS3 [mms3_epd_eis_srvy_l2_phxtof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS3 [mms3_epd_eis_srvy_l2_phxtof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS3 [mms3_epd_eis_srvy_l2_phxtof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS3 [mms3_epd_eis_srvy_l2_phxtof_vtofxphe]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS3_FEEPS_BRST_L2_ELECTRON (spase://NASA/NumericalData/MMS/3/EnergeticParticleDetector/FEEPS/Burst/Level2/Electron/PT0.3025S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms3_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms3_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms3_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms3_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms3_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms3_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms3_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms3_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms3_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_12]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms3_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms3_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms3_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms3_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms3_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms3_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms3_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms3_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms3_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_12]
      
      
      MMS3 FEEPS top side burst mode electron count rate sensor 1 [mms3_epd_feeps_brst_l2_electron_top_count_rate_sensorid_1]
      
      
      MMS3 FEEPS top side burst mode electron count rate sensor 2 [mms3_epd_feeps_brst_l2_electron_top_count_rate_sensorid_2]
      
      
      MMS3 FEEPS top side burst mode electron count rate sensor 3 [mms3_epd_feeps_brst_l2_electron_top_count_rate_sensorid_3]
      
      
      MMS3 FEEPS top side burst mode electron count rate sensor 4 [mms3_epd_feeps_brst_l2_electron_top_count_rate_sensorid_4]
      
      
      MMS3 FEEPS top side burst mode electron count rate sensor 5 [mms3_epd_feeps_brst_l2_electron_top_count_rate_sensorid_5]
      
      
      MMS3 FEEPS top side burst mode electron count rate sensor 9 [mms3_epd_feeps_brst_l2_electron_top_count_rate_sensorid_9]
      
      
      MMS3 FEEPS top side burst mode electron count rate sensor 10 [mms3_epd_feeps_brst_l2_electron_top_count_rate_sensorid_10]
      
      
      MMS3 FEEPS top side burst mode electron count rate sensor 11 [mms3_epd_feeps_brst_l2_electron_top_count_rate_sensorid_11]
      
      
      MMS3 FEEPS top side burst mode electron count rate sensor 12 [mms3_epd_feeps_brst_l2_electron_top_count_rate_sensorid_12]
      
      
      MMS3 FEEPS bottom side burst mode electron count rate sensor 1 [mms3_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_1]
      
      
      MMS3 FEEPS bottom side burst mode electron count rate sensor 2 [mms3_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_2]
      
      
      MMS3 FEEPS bottom side burst mode electron count rate sensor 3 [mms3_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_3]
      
      
      MMS3 FEEPS bottom side burst mode electron count rate sensor 4 [mms3_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_4]
      
      
      MMS3 FEEPS bottom side burst mode electron count rate sensor 5 [mms3_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_5]
      
      
      MMS3 FEEPS bottom side burst mode electron count rate sensor 9 [mms3_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_9]
      
      
      MMS3 FEEPS bottom side burst mode electron count rate sensor 10 [mms3_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_10]
      
      
      MMS3 FEEPS bottom side burst mode electron count rate sensor 11 [mms3_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_11]
      
      
      MMS3 FEEPS bottom side burst mode electron count rate sensor 12 [mms3_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_12]
      
      
      MMS3 FEEPS top side burst mode electron intensity sensor 1 [mms3_epd_feeps_brst_l2_electron_top_intensity_sensorid_1]
      
      
      MMS3 FEEPS top side burst mode electron intensity sensor 2 [mms3_epd_feeps_brst_l2_electron_top_intensity_sensorid_2]
      
      
      MMS3 FEEPS top side burst mode electron intensity sensor 3 [mms3_epd_feeps_brst_l2_electron_top_intensity_sensorid_3]
      
      
      MMS3 FEEPS top side burst mode electron intensity sensor 4 [mms3_epd_feeps_brst_l2_electron_top_intensity_sensorid_4]
      
      
      MMS3 FEEPS top side burst mode electron intensity sensor 5 [mms3_epd_feeps_brst_l2_electron_top_intensity_sensorid_5]
      
      
      MMS3 FEEPS top side burst mode electron intensity sensor 9 [mms3_epd_feeps_brst_l2_electron_top_intensity_sensorid_9]
      
      
      MMS3 FEEPS top side burst mode electron intensity sensor 10 [mms3_epd_feeps_brst_l2_electron_top_intensity_sensorid_10]
      
      
      MMS3 FEEPS top side burst mode electron intensity sensor 11 [mms3_epd_feeps_brst_l2_electron_top_intensity_sensorid_11]
      
      
      MMS3 FEEPS top side burst mode electron intensity sensor 12 [mms3_epd_feeps_brst_l2_electron_top_intensity_sensorid_12]
      
      
      MMS3 FEEPS bottom side burst mode electron intensity sensor 1 [mms3_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_1]
      
      
      MMS3 FEEPS bottom side burst mode electron intensity sensor 2 [mms3_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_2]
      
      
      MMS3 FEEPS bottom side burst mode electron intensity sensor 3 [mms3_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_3]
      
      
      MMS3 FEEPS bottom side burst mode electron intensity sensor 4 [mms3_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_4]
      
      
      MMS3 FEEPS bottom side burst mode electron intensity sensor 5 [mms3_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_5]
      
      
      MMS3 FEEPS bottom side burst mode electron intensity sensor 9 [mms3_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_9]
      
      
      MMS3 FEEPS bottom side burst mode electron intensity sensor 10 [mms3_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_10]
      
      
      MMS3 FEEPS bottom side burst mode electron intensity sensor 11 [mms3_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_11]
      
      
      MMS3 FEEPS bottom side burst mode electron intensity sensor 12 [mms3_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_12]
      
      
      MMS3 FEEPS top side burst mode electron count error statistics sensor 1 [mms3_epd_feeps_brst_l2_electron_top_percent_error_sensorid_1]
      
      
      MMS3 FEEPS top side burst mode electron count error statistics sensor 2 [mms3_epd_feeps_brst_l2_electron_top_percent_error_sensorid_2]
      
      
      MMS3 FEEPS top side burst mode electron count error statistics sensor 3 [mms3_epd_feeps_brst_l2_electron_top_percent_error_sensorid_3]
      
      
      MMS3 FEEPS top side burst mode electron count error statistics sensor 4 [mms3_epd_feeps_brst_l2_electron_top_percent_error_sensorid_4]
      
      
      MMS3 FEEPS top side burst mode electron count error statistics sensor 5 [mms3_epd_feeps_brst_l2_electron_top_percent_error_sensorid_5]
      
      
      MMS3 FEEPS top side burst mode electron count error statistics sensor 9 [mms3_epd_feeps_brst_l2_electron_top_percent_error_sensorid_9]
      
      
      MMS3 FEEPS top side burst mode electron count error statistics sensor 10 [mms3_epd_feeps_brst_l2_electron_top_percent_error_sensorid_10]
      
      
      MMS3 FEEPS top side burst mode electron count error statistics sensor 11 [mms3_epd_feeps_brst_l2_electron_top_percent_error_sensorid_11]
      
      
      MMS3 FEEPS top side burst mode electron count error statistics sensor 12 [mms3_epd_feeps_brst_l2_electron_top_percent_error_sensorid_12]
      
      
      MMS3 FEEPS bottom side burst mode electron count error statistics sensor 1 [mms3_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_1]
      
      
      MMS3 FEEPS bottom side burst mode electron count error statistics sensor 2 [mms3_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_2]
      
      
      MMS3 FEEPS bottom side burst mode electron count error statistics sensor 3 [mms3_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_3]
      
      
      MMS3 FEEPS bottom side burst mode electron count error statistics sensor 4 [mms3_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_4]
      
      
      MMS3 FEEPS bottom side burst mode electron count error statistics sensor 5 [mms3_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_5]
      
      
      MMS3 FEEPS bottom side burst mode electron count error statistics sensor 9 [mms3_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_9]
      
      
      MMS3 FEEPS bottom side burst mode electron count error statistics sensor 10 [mms3_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_10]
      
      
      MMS3 FEEPS bottom side burst mode electron count error statistics sensor 11 [mms3_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_11]
      
      
      MMS3 FEEPS bottom side burst mode electron count error statistics sensor 12 [mms3_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_12]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms3_epd_feeps_brst_l2_electron_pitch_angle]
      
      
      Latitude [mms3_epd_feeps_brst_l2_electron_lat_gse]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS3_FEEPS_BRST_L2_ION (spase://NASA/NumericalData/MMS/3/EnergeticParticleDetector/FEEPS/Burst/Level2/Ion/PT0.3025S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms3_epd_feeps_brst_l2_ion_top_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms3_epd_feeps_brst_l2_ion_top_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms3_epd_feeps_brst_l2_ion_top_quality_indicator_sensorid_8]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms3_epd_feeps_brst_l2_ion_bottom_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms3_epd_feeps_brst_l2_ion_bottom_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms3_epd_feeps_brst_l2_ion_bottom_quality_indicator_sensorid_8]
      
      
      MMS3 FEEPS top side burst mode ion count rate sensor 6 [mms3_epd_feeps_brst_l2_ion_top_count_rate_sensorid_6]
      
      
      MMS3 FEEPS top side burst mode ion count rate sensor 7 [mms3_epd_feeps_brst_l2_ion_top_count_rate_sensorid_7]
      
      
      MMS3 FEEPS top side burst mode ion count rate sensor 8 [mms3_epd_feeps_brst_l2_ion_top_count_rate_sensorid_8]
      
      
      MMS3 FEEPS bottom side burst mode ion count rate sensor 6 [mms3_epd_feeps_brst_l2_ion_bottom_count_rate_sensorid_6]
      
      
      MMS3 FEEPS bottom side burst mode ion count rate sensor 7 [mms3_epd_feeps_brst_l2_ion_bottom_count_rate_sensorid_7]
      
      
      MMS3 FEEPS bottom side burst mode ion count rate sensor 8 [mms3_epd_feeps_brst_l2_ion_bottom_count_rate_sensorid_8]
      
      
      MMS3 FEEPS top side burst mode ion intensity sensor 6 [mms3_epd_feeps_brst_l2_ion_top_intensity_sensorid_6]
      
      
      MMS3 FEEPS top side burst mode ion intensity sensor 7 [mms3_epd_feeps_brst_l2_ion_top_intensity_sensorid_7]
      
      
      MMS3 FEEPS top side burst mode ion intensity sensor 8 [mms3_epd_feeps_brst_l2_ion_top_intensity_sensorid_8]
      
      
      MMS3 FEEPS bottom side burst mode ion intensity sensor 6 [mms3_epd_feeps_brst_l2_ion_bottom_intensity_sensorid_6]
      
      
      MMS3 FEEPS bottom side burst mode ion intensity sensor 7 [mms3_epd_feeps_brst_l2_ion_bottom_intensity_sensorid_7]
      
      
      MMS3 FEEPS bottom side burst mode ion intensity sensor 8 [mms3_epd_feeps_brst_l2_ion_bottom_intensity_sensorid_8]
      
      
      MMS3 FEEPS top side burst mode ion count error statistics sensor 6 [mms3_epd_feeps_brst_l2_ion_top_percent_error_sensorid_6]
      
      
      MMS3 FEEPS top side burst mode ion count error statistics sensor 7 [mms3_epd_feeps_brst_l2_ion_top_percent_error_sensorid_7]
      
      
      MMS3 FEEPS top side burst mode ion count error statistics sensor 8 [mms3_epd_feeps_brst_l2_ion_top_percent_error_sensorid_8]
      
      
      MMS3 FEEPS bottom side burst mode ion count error statistics sensor 6 [mms3_epd_feeps_brst_l2_ion_bottom_percent_error_sensorid_6]
      
      
      MMS3 FEEPS bottom side burst mode ion count error statistics sensor 7 [mms3_epd_feeps_brst_l2_ion_bottom_percent_error_sensorid_7]
      
      
      MMS3 FEEPS bottom side burst mode ion count error statistics sensor 8 [mms3_epd_feeps_brst_l2_ion_bottom_percent_error_sensorid_8]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms3_epd_feeps_brst_l2_ion_pitch_angle]
      
      
      Latitude [mms3_epd_feeps_brst_l2_ion_lat_gse]
      
      
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MMS3_FEEPS_SRVY_L2_ELECTRON (spase://NASA/NumericalData/MMS/3/EnergeticParticleDetector/FEEPS/Survey/Level2/Electron/PT2.42S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms3_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms3_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms3_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms3_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms3_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms3_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms3_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms3_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms3_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_12]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms3_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms3_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms3_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms3_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms3_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms3_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms3_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms3_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms3_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_12]
      
      
      MMS3 FEEPS top side survey mode electron count rate sensor 1 [mms3_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_1]
      
      
      MMS3 FEEPS top side survey mode electron count rate sensor 2 [mms3_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_2]
      
      
      MMS3 FEEPS top side survey mode electron count rate sensor 3 [mms3_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_3]
      
      
      MMS3 FEEPS top side survey mode electron count rate sensor 4 [mms3_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_4]
      
      
      MMS3 FEEPS top side survey mode electron count rate sensor 5 [mms3_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_5]
      
      
      MMS3 FEEPS top side survey mode electron count rate sensor 9 [mms3_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_9]
      
      
      MMS3 FEEPS top side survey mode electron count rate sensor 10 [mms3_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_10]
      
      
      MMS3 FEEPS top side survey mode electron count rate sensor 11 [mms3_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_11]
      
      
      MMS3 FEEPS top side survey mode electron count rate sensor 12 [mms3_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_12]
      
      
      MMS3 FEEPS bottom side survey mode electron count rate sensor 1 [mms3_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_1]
      
      
      MMS3 FEEPS bottom side survey mode electron count rate sensor 2 [mms3_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_2]
      
      
      MMS3 FEEPS bottom side survey mode electron count rate sensor 3 [mms3_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_3]
      
      
      MMS3 FEEPS bottom side survey mode electron count rate sensor 4 [mms3_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_4]
      
      
      MMS3 FEEPS bottom side survey mode electron count rate sensor 5 [mms3_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_5]
      
      
      MMS3 FEEPS bottom side survey mode electron count rate sensor 9 [mms3_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_9]
      
      
      MMS3 FEEPS bottom side survey mode electron count rate sensor 10 [mms3_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_10]
      
      
      MMS3 FEEPS bottom side survey mode electron count rate sensor 11 [mms3_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_11]
      
      
      MMS3 FEEPS bottom side survey mode electron count rate sensor 12 [mms3_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_12]
      
      
      MMS3 FEEPS top side survey mode electron intensity sensor 1 [mms3_epd_feeps_srvy_l2_electron_top_intensity_sensorid_1]
      
      
      MMS3 FEEPS top side survey mode electron intensity sensor 2 [mms3_epd_feeps_srvy_l2_electron_top_intensity_sensorid_2]
      
      
      MMS3 FEEPS top side survey mode electron intensity sensor 3 [mms3_epd_feeps_srvy_l2_electron_top_intensity_sensorid_3]
      
      
      MMS3 FEEPS top side survey mode electron intensity sensor 4 [mms3_epd_feeps_srvy_l2_electron_top_intensity_sensorid_4]
      
      
      MMS3 FEEPS top side survey mode electron intensity sensor 5 [mms3_epd_feeps_srvy_l2_electron_top_intensity_sensorid_5]
      
      
      MMS3 FEEPS top side survey mode electron intensity sensor 9 [mms3_epd_feeps_srvy_l2_electron_top_intensity_sensorid_9]
      
      
      MMS3 FEEPS top side survey mode electron intensity sensor 10 [mms3_epd_feeps_srvy_l2_electron_top_intensity_sensorid_10]
      
      
      MMS3 FEEPS top side survey mode electron intensity sensor 11 [mms3_epd_feeps_srvy_l2_electron_top_intensity_sensorid_11]
      
      
      MMS3 FEEPS top side survey mode electron intensity sensor 12 [mms3_epd_feeps_srvy_l2_electron_top_intensity_sensorid_12]
      
      
      MMS3 FEEPS bottom side survey mode electron intensity sensor 1 [mms3_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_1]
      
      
      MMS3 FEEPS bottom side survey mode electron intensity sensor 2 [mms3_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_2]
      
      
      MMS3 FEEPS bottom side survey mode electron intensity sensor 3 [mms3_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_3]
      
      
      MMS3 FEEPS bottom side survey mode electron intensity sensor 4 [mms3_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_4]
      
      
      MMS3 FEEPS bottom side survey mode electron intensity sensor 5 [mms3_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_5]
      
      
      MMS3 FEEPS bottom side survey mode electron intensity sensor 9 [mms3_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_9]
      
      
      MMS3 FEEPS bottom side survey mode electron intensity sensor 10 [mms3_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_10]
      
      
      MMS3 FEEPS bottom side survey mode electron intensity sensor 11 [mms3_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_11]
      
      
      MMS3 FEEPS bottom side survey mode electron intensity sensor 12 [mms3_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_12]
      
      
      MMS3 FEEPS top side survey mode electron count error statistics sensor 1 [mms3_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_1]
      
      
      MMS3 FEEPS top side survey mode electron count error statistics sensor 2 [mms3_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_2]
      
      
      MMS3 FEEPS top side survey mode electron count error statistics sensor 3 [mms3_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_3]
      
      
      MMS3 FEEPS top side survey mode electron count error statistics sensor 4 [mms3_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_4]
      
      
      MMS3 FEEPS top side survey mode electron count error statistics sensor 5 [mms3_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_5]
      
      
      MMS3 FEEPS top side survey mode electron count error statistics sensor 9 [mms3_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_9]
      
      
      MMS3 FEEPS top side survey mode electron count error statistics sensor 10 [mms3_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_10]
      
      
      MMS3 FEEPS top side survey mode electron count error statistics sensor 11 [mms3_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_11]
      
      
      MMS3 FEEPS top side survey mode electron count error statistics sensor 12 [mms3_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_12]
      
      
      MMS3 FEEPS bottom side survey mode electron count error statistics sensor 1 [mms3_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_1]
      
      
      MMS3 FEEPS bottom side survey mode electron count error statistics sensor 2 [mms3_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_2]
      
      
      MMS3 FEEPS bottom side survey mode electron count error statistics sensor 3 [mms3_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_3]
      
      
      MMS3 FEEPS bottom side survey mode electron count error statistics sensor 4 [mms3_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_4]
      
      
      MMS3 FEEPS bottom side survey mode electron count error statistics sensor 5 [mms3_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_5]
      
      
      MMS3 FEEPS bottom side survey mode electron count error statistics sensor 9 [mms3_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_9]
      
      
      MMS3 FEEPS bottom side survey mode electron count error statistics sensor 10 [mms3_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_10]
      
      
      MMS3 FEEPS bottom side survey mode electron count error statistics sensor 11 [mms3_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_11]
      
      
      MMS3 FEEPS bottom side survey mode electron count error statistics sensor 12 [mms3_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_12]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms3_epd_feeps_srvy_l2_electron_pitch_angle]
      
      
      Latitude [mms3_epd_feeps_srvy_l2_electron_lat_gse]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS3_FEEPS_SRVY_L2_ION (spase://NASA/NumericalData/MMS/3/EnergeticParticleDetector/FEEPS/Survey/Level2/Ion/PT2.42S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms3_epd_feeps_srvy_l2_ion_top_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms3_epd_feeps_srvy_l2_ion_top_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms3_epd_feeps_srvy_l2_ion_top_quality_indicator_sensorid_8]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms3_epd_feeps_srvy_l2_ion_bottom_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms3_epd_feeps_srvy_l2_ion_bottom_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms3_epd_feeps_srvy_l2_ion_bottom_quality_indicator_sensorid_8]
      
      
      MMS3 FEEPS top side survey mode ion count rate sensor 6 [mms3_epd_feeps_srvy_l2_ion_top_count_rate_sensorid_6]
      
      
      MMS3 FEEPS top side survey mode ion count rate sensor 7 [mms3_epd_feeps_srvy_l2_ion_top_count_rate_sensorid_7]
      
      
      MMS3 FEEPS top side survey mode ion count rate sensor 8 [mms3_epd_feeps_srvy_l2_ion_top_count_rate_sensorid_8]
      
      
      MMS3 FEEPS bottom side survey mode ion count rate sensor 6 [mms3_epd_feeps_srvy_l2_ion_bottom_count_rate_sensorid_6]
      
      
      MMS3 FEEPS bottom side survey mode ion count rate sensor 7 [mms3_epd_feeps_srvy_l2_ion_bottom_count_rate_sensorid_7]
      
      
      MMS3 FEEPS bottom side survey mode ion count rate sensor 8 [mms3_epd_feeps_srvy_l2_ion_bottom_count_rate_sensorid_8]
      
      
      MMS3 FEEPS top side survey mode ion intensity sensor 6 [mms3_epd_feeps_srvy_l2_ion_top_intensity_sensorid_6]
      
      
      MMS3 FEEPS top side survey mode ion intensity sensor 7 [mms3_epd_feeps_srvy_l2_ion_top_intensity_sensorid_7]
      
      
      MMS3 FEEPS top side survey mode ion intensity sensor 8 [mms3_epd_feeps_srvy_l2_ion_top_intensity_sensorid_8]
      
      
      MMS3 FEEPS bottom side survey mode ion intensity sensor 6 [mms3_epd_feeps_srvy_l2_ion_bottom_intensity_sensorid_6]
      
      
      MMS3 FEEPS bottom side survey mode ion intensity sensor 7 [mms3_epd_feeps_srvy_l2_ion_bottom_intensity_sensorid_7]
      
      
      MMS3 FEEPS bottom side survey mode ion intensity sensor 8 [mms3_epd_feeps_srvy_l2_ion_bottom_intensity_sensorid_8]
      
      
      MMS3 FEEPS top side survey mode ion count error statistics sensor 6 [mms3_epd_feeps_srvy_l2_ion_top_percent_error_sensorid_6]
      
      
      MMS3 FEEPS top side survey mode ion count error statistics sensor 7 [mms3_epd_feeps_srvy_l2_ion_top_percent_error_sensorid_7]
      
      
      MMS3 FEEPS top side survey mode ion count error statistics sensor 8 [mms3_epd_feeps_srvy_l2_ion_top_percent_error_sensorid_8]
      
      
      MMS3 FEEPS bottom side survey mode ion count error statistics sensor 6 [mms3_epd_feeps_srvy_l2_ion_bottom_percent_error_sensorid_6]
      
      
      MMS3 FEEPS bottom side survey mode ion count error statistics sensor 7 [mms3_epd_feeps_srvy_l2_ion_bottom_percent_error_sensorid_7]
      
      
      MMS3 FEEPS bottom side survey mode ion count error statistics sensor 8 [mms3_epd_feeps_srvy_l2_ion_bottom_percent_error_sensorid_8]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms3_epd_feeps_srvy_l2_ion_pitch_angle]
      
      
      Latitude [mms3_epd_feeps_srvy_l2_ion_lat_gse]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS3_FGM_BRST_L2 (spase://NASA/NumericalData/MMS/3/FIELDS/FGM/Burst/Level2/PT0.0078125S)
Description
The Fluxgate Magnetometers (FGM) on Magnetospheric Multiscale consist of a
traditional Analog Fluxgate Magnetometer (AFG), and a Digital Fluxgate
magnetometer (DFG). The dual magnetometers are operated as a single instrument
providing a single intercalibrated data product. Range changes occur at
different times on the two instruments so the gains checked each periapsis can
be carried out unambiguously to apoapsis. Cross correlation of calibration
parameters can separate causes of the any apparent calibration changes. Use of
Electron Drift Instrument (EDI) to determine the field along the rotation axis
allows accurate monitoring of the zero levels along the rotation axis.  Prior to
launch the magnetometers were calibrated at the Technical University,
Braunschweig, except for the AFG magnetometers on MMS3 and MMS4, which were
calibrated at UCLA.  Both sets of sensors are operated for the entire MMS orbit,
with slow survey (8 samples per second) outside of the Region of Interest (ROI),
and fast survey (16 samples per second) inside the ROI. Within the ROI burst
mode data (128 samples per second) are also acquired.  A detailed description of
the MMS fluxgate magnetometers, including science objectives, instrument
description, calibration, magnetic cleanliness program, and data flow can be
found at http://link.springer.com/article/10.1007%2Fs11214-014-0057-3 (DOI 
10.1007/s11214-014-0057-3).Additional information can also be found at
http://www-spc.igpp.ucla.edu/ssc/mms (UCLA),and http://www.iwf.oeaw.ac.at (IWF,
Graz).
For the purpose of creating a unified FGM Level2 data product, burst mode data
is taken from DFG and survey mode data is taken from AFG.  Because AFG and DFG
are cross-calibrated on an orbit-averaged basis, small differences in offset may
be observed between Level2 burst and survey mode data.  Consequently, any
differences are within the error of the measurement. Based on preliminary
analysis of the data, the absolute error within the Region of Interest (ROI) is
estimated to be no more than 0.1 nT in the spin-plane, 0.15 nT along the
spin-axis and 0.2 nT in total magnitude.
Modification History
version X=5:  * Y-version number comes from cal file entries. 
              *
Ensures there are 2 ephemeris points before/after data to enable proper spline. 

              * Fix to depend_0 of rdeltahalf:  fixes bug when reading position
data.
              * L-vector for DMPA2GSE transformation is smoothed with a
gaussian filter, instead 
                of using a single average value for
the day.  This short-term filter avoids  
                introduding artificial
jumps at 00:00 UTC and removes 7-minute 'wobble' after  
               
maneuvers in the GSE result.   
              * Fixes error with DEFATT file
selection found when choosing the 
                daily DEFATT files to be used
in Phase 2.
              * Fixed bug where reference Etemp was used for high
range gain.  Now uses measured Etemp.
version X=4:  First version for public
release of L2.
              Renamed variables to conform with new MMS variable
name guidelines 
              (obs_instr_paramName[_coordSys]_mode_level):  
  
             Mag field parameters include 'b' for paramName.  
               
Use 'r' instead of 'pos' for S/C position paramName.  
               
Eliminated 'rate', replaced with 'bdeltahalf'.  Added 'rdeltahalf'.
            
   l1a_mode is now just 'mode'.
version X=3:  fixed removal of overlap between
modes.
              fixed a bug that caused stemp and etemp to be
empty.
version X=2:  flag parameter name corrected: was 'status'
               
        added bits 4, 5, 6 to flag saturation on B1, B2, and B3, respectively
  
                     added bit 7 to flag bad data at range changes
             
Added etemp and l1a_mode parameters.  
              rate, hirange, and stemp
parameters now comply with MMS CDF Guidlelines, e.g.
              FILLVAL now
defined for stemp and etemp, and is set to !values.f_nan
              No longer
use Var_Parents attribute in stemp -- see Parents instead
              In this
version, temperature-corrected gains are applied.  Reference temperatures are
used when 
              stemp or etemp are set to FILLVAL. 
             
Non-linearity correction is applied to high rage DFG data.
version X=1:  added
'flag', rate and hirange parameters (but 'flag' is actually called 'status')
 
  • Data Variable Descriptions
      Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (128 S/s) [mms3_fgm_b_gse_brst_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms3_fgm_b_gse_brst_l2]
      
      
      Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (128 S/s) [mms3_fgm_b_gsm_brst_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms3_fgm_b_gsm_brst_l2]
      
      
      Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (128 S/s) [mms3_fgm_b_dmpa_brst_l2_clean]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      ---> Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (128 S/s), including flagged data [mms3_fgm_b_dmpa_brst_l2]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (128 S/s) [mms3_fgm_b_bcs_brst_l2_clean]
      
      
      ---> Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (128 S/s), including flagged data [mms3_fgm_b_bcs_brst_l2]
      
      
      Quality Flag: 0 = No identified problems, non-zero = blank out the data [mms3_fgm_flag_brst_l2]
      bit definitions: .    0: TBD, 1: TBD, 2: user flagged, 3: TBD, .    4: B1
      saturated, 5: B2 saturated, 6: B3 saturated, 7: range-change glitch, .    8-31:
      TBD
      
      Definitive Position in GSE coordinates, 30 second [mms3_fgm_r_gse_brst_l2]
      
      
      Definitive Position in GSM coordinates, 30 second [mms3_fgm_r_gsm_brst_l2]
      
      
Dataset in CDAWeb
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MMS3_FGM_SRVY_L2 (spase://NASA/NumericalData/MMS/3/FIELDS/FGM/Survey/Level2/PT0.125S)
Description
The Fluxgate Magnetometers (FGM) on Magnetospheric Multiscale consist of a
traditional Analog Fluxgate Magnetometer (AFG), and a Digital Fluxgate
magnetometer (DFG). The dual magnetometers are operated as a single instrument
providing a single intercalibrated data product. Range changes occur at
different times on the two instruments so the gains checked each periapsis can
be carried out unambiguously to apoapsis. Cross correlation of calibration
parameters can separate causes of the any apparent calibration changes. Use of
Electron Drift Instrument (EDI) to determine the field along the rotation axis
allows accurate monitoring of the zero levels along the rotation axis.  Prior to
launch the magnetometers were calibrated at the Technical University,
Braunschweig, except for the AFG magnetometers on MMS3 and MMS4, which were
calibrated at UCLA.  Both sets of sensors are operated for the entire MMS orbit,
with slow survey (8 samples per second) outside of the Region of Interest (ROI),
and fast survey (16 samples per second) inside the ROI. Within the ROI burst
mode data (128 samples per second) are also acquired.  A detailed description of
the MMS fluxgate magnetometers, including science objectives, instrument
description, calibration, magnetic cleanliness program, and data flow can be
found at http://link.springer.com/article/10.1007%2Fs11214-014-0057-3 (DOI 
10.1007/s11214-014-0057-3).Additional information can also be found at
http://www-spc.igpp.ucla.edu/ssc/mms (UCLA),and http://www.iwf.oeaw.ac.at (IWF,
Graz).
For the purpose of creating a unified FGM Level2 data product, burst mode data
is taken from DFG and survey mode data is taken from AFG.  Because AFG and DFG
are cross-calibrated on an orbit-averaged basis, small differences in offset may
be observed between Level2 burst and survey mode data.  Consequently, any
differences are within the error of the measurement. Based on preliminary
analysis of the data, the absolute error within the Region of Interest (ROI) is
estimated to be no more than 0.1 nT in the spin-plane, 0.15 nT along the
spin-axis and 0.2 nT in total magnitude.
Modification History
version X=5:  * Y-version number comes from cal file entries. 
              *
Ensures there are 2 ephemeris points before/after data to enable proper spline. 

              * Fix to depend_0 of rdeltahalf:  fixes bug when reading position
data.
              * L-vector for DMPA2GSE transformation is smoothed with a
gaussian filter, instead 
                of using a single average value for
the day.  This short-term filter avoids  
                introduding artificial
jumps at 00:00 UTC and removes 7-minute 'wobble' after  
               
maneuvers in the GSE result.   
              * Fixes error with DEFATT file
selection found when choosing the 
                daily DEFATT files to be used
in Phase 2.
              * Fixed bug where reference Etemp was used for high
range gain.  Now uses measured Etemp.
version X=4:  First version for public
release of L2.
              Renamed variables to conform with new MMS variable
name guidelines 
              (obs_instr_paramName[_coordSys]_mode_level):  
  
             Mag field parameters include 'b' for paramName.  
               
Use 'r' instead of 'pos' for S/C position paramName.  
               
Eliminated 'rate', replaced with 'bdeltahalf'.  Added 'rdeltahalf'.
            
   l1a_mode is now just 'mode'.
version X=3:  fixed removal of overlap between
modes.
              fixed a bug that caused stemp and etemp to be
empty.
version X=2:  flag parameter name corrected: was 'status'
               
        added bits 4, 5, 6 to flag saturation on B1, B2, and B3, respectively
  
                     added bit 7 to flag bad data at range changes
             
Added etemp and l1a_mode parameters.  
              rate, hirange, and stemp
parameters now comply with MMS CDF Guidlelines, e.g.
              FILLVAL now
defined for stemp and etemp, and is set to !values.f_nan
              No longer
use Var_Parents attribute in stemp -- see Parents instead
              In this
version, temperature-corrected gains are applied.  Reference temperatures are
used when 
              stemp or etemp are set to FILLVAL. 
             
Non-linearity correction is applied to high rage DFG data.
version X=1:  added
'flag', rate and hirange parameters (but 'flag' is actually called 'status')
 
  • Data Variable Descriptions
      Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (8 or 16 S/s) [mms3_fgm_b_gse_srvy_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms3_fgm_b_gse_srvy_l2]
      
      
      Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (8 or 16 S/s) [mms3_fgm_b_gsm_srvy_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms3_fgm_b_gsm_srvy_l2]
      
      
      Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (8 or 16 S/s) [mms3_fgm_b_dmpa_srvy_l2_clean]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      ---> Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms3_fgm_b_dmpa_srvy_l2]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (8 or 16 S/s) [mms3_fgm_b_bcs_srvy_l2_clean]
      
      
      ---> Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms3_fgm_b_bcs_srvy_l2]
      
      
      Quality Flag: 0 = No identified problems, non-zero = blank out the data [mms3_fgm_flag_srvy_l2]
      bit definitions: .    0: TBD, 1: TBD, 2: user flagged, 3: TBD, .    4: B1
      saturated, 5: B2 saturated, 6: B3 saturated, 7: range-change glitch, .    8-31:
      TBD
      
      Definitive Position in GSE coordinates, 30 second [mms3_fgm_r_gse_srvy_l2]
      
      
      Definitive Position in GSM coordinates, 30 second [mms3_fgm_r_gsm_srvy_l2]
      
      
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MMS3_FPI_BRST_L2_DES-DIST (spase://NASA/NumericalData/MMS/3/FastPlasmaInvestigation/DES/Burst/Level2/Distribution/PT0.03S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data are taken at burst (30/150 ms for DES/DIS)
resolution in this mode.  Data are also made available at survey (4.5 s, etc)
resolution; these form a separate product from this.  Per mission design, not
all burst-resolution data are downlinked.  This product contains phase-space
distribution maps of those burst-resolution data selected for downlink.  In
particular, the (highest possible quality at the time of release)
corrected/converted "Burst SkyMap" distributions are reported with time-stamps
and other annotation characterizing the state of the instrument system at the
indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      [CDAWeb List/Download/Create ONLY] MMS3 FPI/DES burst sky-map instrument distribution [mms3_des_dist_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 10.9 eV (E1/even) [mms3_des_dist_brst1_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 12.4 eV (E1/odd) [mms3_des_dist_brst1_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~11.6 eV (E1 even-odd) [mms3_des_dist_brst1_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 10.9 eV (E1/even) [mms3_des_dist_brst1_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 12.4 eV (E1/odd) [mms3_des_dist_brst1_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 37.9 eV (E6/even) [mms3_des_dist_brst6_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 42.9 eV (E6/odd) [mms3_des_dist_brst6_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~40.4 eV (E6 even-odd) [mms3_des_dist_brst6_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 37.9 eV (E6/even) [mms3_des_dist_brst6_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 42.9 eV (E6/odd) [mms3_des_dist_brst6_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 80.0 eV (E9/even) [mms3_des_dist_brst9_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 90.6 eV (E9/odd) [mms3_des_dist_brst9_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~85 eV (E9 even-odd) [mms3_des_dist_brst9_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 80.0 eV (E9/even) [mms3_des_dist_brst9_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 90.6 eV (E9/odd) [mms3_des_dist_brst9_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 169 eV (E12/even) [mms3_des_dist_brst12_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 191 eV (E12/odd) [mms3_des_dist_brst12_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~180 eV (E12 even-odd) [mms3_des_dist_brst12_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 169 eV (E12/even) [mms3_des_dist_brst12_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 191 eV (E12/odd) [mms3_des_dist_brst12_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 277 eV (E14/even) [mms3_des_dist_brst14_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 314 eV (E14/odd) [mms3_des_dist_brst14_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~295 eV (E14 even-odd) [mms3_des_dist_brst14_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 277 eV (E14/even) [mms3_des_dist_brst14_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 314 eV (E14/odd) [mms3_des_dist_brst14_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 456 eV (E16/even) [mms3_des_dist_brst16_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 517 eV (E16/odd) [mms3_des_dist_brst16_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~485 eV (E16 even-odd) [mms3_des_dist_brst16_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 456 eV (E16/even) [mms3_des_dist_brst16_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 517 eV (E16/odd) [mms3_des_dist_brst16_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 750 eV (E18/even) [mms3_des_dist_brst18_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 850 eV (E18/odd) [mms3_des_dist_brst18_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~800 eV (E18 even-odd) [mms3_des_dist_brst18_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 750 eV (E18/even) [mms3_des_dist_brst18_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 850 eV (E18/odd) [mms3_des_dist_brst18_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 1230 eV (E20/even) [mms3_des_dist_brst20_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 1400 eV (E20/odd) [mms3_des_dist_brst20_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~1310 eV (E20 even-odd) [mms3_des_dist_brst20_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1230 eV (E20/even) [mms3_des_dist_brst20_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1400 eV (E20/odd) [mms3_des_dist_brst20_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 2600 eV (E23/even) [mms3_des_dist_brst23_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 2950 eV (E23/odd) [mms3_des_dist_brst23_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~2770 eV (E23 even-odd) [mms3_des_dist_brst23_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2600 eV (E23/even) [mms3_des_dist_brst23_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2950 eV (E23/odd) [mms3_des_dist_brst23_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 5490 eV (E26/even) [mms3_des_dist_brst26_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 6210 eV (E26/odd) [mms3_des_dist_brst26_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~5840 eV (E26 even-odd) [mms3_des_dist_brst26_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5490 eV (E26/even) [mms3_des_dist_brst26_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 6210 eV (E26/odd) [mms3_des_dist_brst26_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 24400 eV (E32/even) [mms3_des_dist_brst32_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES burst sky-map instrument distribution - 27600 eV (E32/odd) [mms3_des_dist_brst32_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~26000 eV (E32 even-odd) [mms3_des_dist_brst32_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 24400 eV (E32/even) [mms3_des_dist_brst32_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 27600 eV (E32/odd) [mms3_des_dist_brst32_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [List/Create only in CDAWeb] 1-sigma error: MMS3 FPI/DES burst sky-map instrument distribution [mms3_des_disterr_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES vector of data-quality indicators at burst-start time [mms3_des_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS3 FPI/DES compression lossless/lossy indicator at survey-start time [mms3_des_compressionloss_brst]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS3 FPI/DES step table parity, this burst [mms3_des_steptable_parity_brst]
      FPI/DES alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS3 FPI/DES Del-Phi (obs spin-phase) count at burst-start time [mms3_des_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS3 FPI/DES Del-Phi (obs spin-phase) angle at burst-start time [mms3_des_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS3 FPI/DES burst average f1 count values [mms3_des_avgf1counts_brst]
      Average f1-count level as a function of energy
      
      MMS3 FPI/DES burst sky-map microsecond offsets from Epoch [mms3_des_steptimeoffsets_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order. Offsets reflect 128 steps over the 30 msec sweep
      period. See FPI docs for details.
      
      ---> MMS3 FPI/DES sector de-Spin P value, this burst [mms3_des_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS3 FPI/DES burst sky-map instrument azimuthal angles [mms3_des_phi_brst]
      see FPI docs for details
      
      MMS FPI/DES burst sky-map parity 0/1 energies [mms3_des_energy_brst]
      Energies (parity 0/1) in the 64-step FPI energy table
      
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MMS3_FPI_BRST_L2_DES-MOMS (spase://NASA/NumericalData/MMS/3/FastPlasmaInvestigation/DES/Burst/Level2/Moments/PT0.03S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode.  Data are also made available at survey (4.5
s, etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked.  Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available.  This product contains results from
integrating the standard moments of phase-space distributions formed from the
indicated data type (DES/DIS burst, FS or SS).  For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DES 32-bit vector of data-quality indicators at burst-start time [mms3_des_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>25%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied
      
      ---> MMS3 FPI/DES compression lossless/lossy indicator at survey-start time [mms3_des_compressionloss_brst]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS3 FPI/DES step table parity, this burst [mms3_des_steptable_parity_brst]
      FPI/DES alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS3 FPI/DES Del-Phi (obs spin-phase) count at burst-start time [mms3_des_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS3 FPI/DES Del-Phi (obs spin-phase) angle at burst-start time [mms3_des_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      ---> MMS3 FPI/DES sector de-Spin P value, this burst [mms3_des_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS3 FPI/DES electron pitch-angle distribution for "low" energies during this burst [mms3_des_pitchangdist_lowen_brst]
      low energy bin: 0 eV - 200 eV.  pitch-angle bin size: 6 deg.
      
      ---> MMS3 FPI/DES electron pitch-angle distribution for "mid" energies during this burst [mms3_des_pitchangdist_miden_brst]
      mid energy bin: 200 eV - 2 keV.  pitch-angle bin size: 6 deg.
      
      ---> MMS3 FPI/DES electron pitch-angle distribution for "high" energies during this burst [mms3_des_pitchangdist_highen_brst]
      high energy bin: 2 keV - 30 keV.  pitch-angle bin size: 6 deg.
      
      MMS3 FPI/DES electron energy spectrum "near" +X_DSC during this burst [mms3_des_energyspectr_px_brst]
      Counts, summed over DSC velocity-dirs closest to +X_DSC, by energy bin.
      
      ---> MMS3 FPI/DES electron energy spectrum "near" -X_DSC during this burst [mms3_des_energyspectr_mx_brst]
      Counts, summed over DSC velocity-dirs closest to -X_DSC, by energy bin.
      
      ---> MMS3 FPI/DES electron energy spectrum "near" +Y_DSC during this burst [mms3_des_energyspectr_py_brst]
      Counts, summed over DSC velocity-dirs closest to +Y_DSC, by energy bin.
      
      ---> MMS3 FPI/DES electron energy spectrum "near" -Y_DSC during this burst [mms3_des_energyspectr_my_brst]
      Counts, summed over DSC velocity-dirs closest to -Y_DSC, by energy bin.
      
      ---> MMS3 FPI/DES electron energy spectrum "near" +Z_DSC during this burst [mms3_des_energyspectr_pz_brst]
      Counts, summed over DSC velocity-dirs closest to +Z_DSC, by energy bin.
      
      ---> MMS3 FPI/DES electron energy spectrum "near" -Z_DSC during this burst [mms3_des_energyspectr_mz_brst]
      Counts, summed over DSC velocity-dirs closest to -Z_DSC, by energy bin.
      
      MMS3 FPI/DES electron energy parallel spectrum 30 degrees parallel to B during this burst [mms3_des_energyspectr_par_brst]
      Counts, summed within 30 degrees parallel bentPipe magnetic field.
      
      ---> MMS3 FPI/DES electron energy anti-parallel spectrum 30 degrees anti-parallel to B during this burst [mms3_des_energyspectr_anti_brst]
      Counts, summed within 30 degrees antiparallel to bentPipe magnetic field.
      
      ---> MMS3 FPI/DES electron energy perpendicular spectrum 60 degrees perpendicular to B during this burst [mms3_des_energyspectr_perp_brst]
      Counts, summed within 60 degrees perpendicular to bentPipe magnetic field.
      
      MMS3 FPI/DES omni-directional electron energy spectrum during this burst [mms3_des_energyspectr_omni_brst]
      Differential energy flux, averaged (weighted by solid angle) over all look
      directions, by energy bin.
      
      MMS3 FPI/DES electron number density during this burst [mms3_des_numberdensity_brst]
      
      
      ---> (no error bars displayed) MMS3 FPI/DES electron number density during this burst [mms3_des_numberdensity_brst_noerr]
      
      
      ---> MMS3 FPI/DES electron number density error during this burst [mms3_des_numberdensity_err_brst]
      
      
      MMS3 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms3_des_densityextrapolation_low_brst]
      
      
      MMS3 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms3_des_densityextrapolation_high_brst]
      
      
      MMS3 FPI/DES electron bulk-velocity DBCS vector during this burst [mms3_des_bulkv_dbcs_brst]
      
      
      MMS3 FPI/DES electron bulk-velocity estimated spintone vector in DBCS during this burst [mms3_des_bulkv_spintone_dbcs_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS3 FPI/DES electron bulk-velocity DBCS vector during this burst [mms3_des_bulkv_dbcs_brst_noerr]
      
      
      MMS3 FPI/DES electron bulk-velocity GSE vector during this burst [mms3_des_bulkv_gse_brst]
      
      
      MMS3 FPI/DES electron bulk-velocity estimated spintone vector in GSE during this burst [mms3_des_bulkv_spintone_gse_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS3 FPI/DES electron bulk-velocity GSE vector during this burst [mms3_des_bulkv_gse_brst_noerr]
      
      
      MMS3 FPI/DES electron bulk-velocity spintone vector in DBCS during this burst [mms3_des_bulkv_spin_dbcs_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS3 FPI/DES electron bulk-velocity spintone vector in GSE during this burst [mms3_des_bulkv_spin_gse_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS3 FPI/DES electron pressure tensor DBCS matrix during this burst [mms3_des_prestensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES electron pressure tensor GSE matrix during this burst [mms3_des_prestensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES electron temperature tensor DBCS matrix during this burst [mms3_des_temptensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES electron temperature tensor GSE matrix during this burst [mms3_des_temptensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES electron heat-flux DBCS vector during this burst [mms3_des_heatq_dbcs_brst]
      
      
      MMS3 FPI/DES electron heat-flux GSE vector during this burst [mms3_des_heatq_gse_brst]
      
      
      MMS3 FPI/DES electron parallel temperature during this BP [mms3_des_temppara_brst]
      
      
      MMS3 FPI/DES electron perpendicular temperature during this BP [mms3_des_tempperp_brst]
      
      
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MMS3_FPI_BRST_L2_DES-PARTMOMS (spase://NASA/NumericalData/MMS/3/FastPlasmaInvestigation/DES/Burst/Level2/PartialMoments/PT0.03S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s,
etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked. Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available. This product contains partial moments that
come from performing the standard moment integrals over a limited portion of
velocity space. The resulting quantities are named similarly to their
corresponding standard moments, but are decorated with 'part' to differentiate.
For example, density_part is the density moment integrated from a particular
energy step to infinity. These partial moments are formed from the indicated
data type (DES/DIS burst, FS or SS). For convenience, some additional parameters
are included to augment those most commonly found in a moments product of this
sort, plus time-stamps and other annotation characterizing the state of the
instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DES vector of data-quality indicators at burst-start time [mms3_des_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only)
      
      MMS3 FPI/DES partial electron number density during this burst [mms3_des_numberdensity_part_brst]
      
      
      MMS3 FPI/DES partial electron bulk-velocity vector in DBCS during this burst [mms3_des_bulkv_part_dbcs_brst]
      
      
      MMS3 FPI/DES partial electron bulk-velocity vector in GSE during this burst [mms3_des_bulkv_part_gse_brst]
      
      
      MMS3 FPI/DES partial electron pressure tensor in DBCS during this burst [mms3_des_prestensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES partial electron pressure tensor in GSE during this burst [mms3_des_prestensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES partial electron temperature tensor in DBCS during this burst [mms3_des_temptensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES partial electron temperature tensor in GSE during this burst [mms3_des_temptensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES partial electron parallel temperature during this burst [mms3_des_temppara_part_brst]
      
      
      MMS3 FPI/DES partial electron perpendicular temperature during this burst [mms3_des_tempperp_part_brst]
      
      
      MMS3 FPI/DES recommended energy index during this burst [mms3_des_part_index_brst]
      Recommended energy index during this burst
      
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MMS3_FPI_BRST_L2_DIS-DIST (spase://NASA/NumericalData/MMS/3/FastPlasmaInvestigation/DIS/Burst/Level2/Distribution/PT0.15S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data are taken at burst (30/150 ms for DES/DIS)
resolution in this mode.  Data are also made available at survey (4.5 s, etc)
resolution; these form a separate product from this.  Per mission design, not
all burst-resolution data are downlinked.  This product contains phase-space
distribution maps of those burst-resolution data selected for downlink.  In
particular, the (highest possible quality at the time of release)
corrected/converted "Burst SkyMap" distributions are reported with time-stamps
and other annotation characterizing the state of the instrument system at the
indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      [CDAWeb List/Download/Create ONLY] MMS3 FPI/DIS burst sky-map instrument distribution [mms3_dis_dist_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 10.6 eV (E1/even) [mms3_dis_dist_brst1_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 12.0 eV (E1/odd) [mms3_dis_dist_brst1_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~11.3 eV (E1 even-odd) [mms3_dis_dist_brst1_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 10.6 eV (E1/even) [mms3_dis_dist_brst1_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 12.0 eV (E1/odd) [mms3_dis_dist_brst1_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 37.2 eV (E6/even) [mms3_dis_dist_brst6_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 42.1 eV (E6/odd) [mms3_dis_dist_brst6_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~39.6 eV (E6 even-odd) [mms3_dis_dist_brst6_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 37.2 eV (E6/even) [mms3_dis_dist_brst6_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 42.1 eV (E6/odd) [mms3_dis_dist_brst6_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 78.8 eV (E9/even) [mms3_dis_dist_brst9_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 89.3 eV (E9/odd) [mms3_dis_dist_brst9_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~83.9 eV (E9 even-odd) [mms3_dis_dist_brst9_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 78.8 eV (E9/even) [mms3_dis_dist_brst9_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 89.3 eV (E9/odd) [mms3_dis_dist_brst9_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 167 eV (E12/even) [mms3_dis_dist_brst12_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 189 eV (E12/odd) [mms3_dis_dist_brst12_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~178 eV (E12 even-odd) [mms3_dis_dist_brst12_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 167 eV (E12/even) [mms3_dis_dist_brst12_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 189 eV (E12/odd) [mms3_dis_dist_brst12_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 275 eV (E14/even) [mms3_dis_dist_brst14_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 312 eV (E14/odd) [mms3_dis_dist_brst14_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~293 eV (E14 even-odd) [mms3_dis_dist_brst14_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 275 eV (E14/even) [mms3_dis_dist_brst14_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 312 eV (E14/odd) [mms3_dis_dist_brst14_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 455 eV (E16/even) [mms3_dis_dist_brst16_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 515 eV (E16/odd) [mms3_dis_dist_brst16_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~484 eV (E16 even-odd) [mms3_dis_dist_brst16_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 455 eV (E16/even) [mms3_dis_dist_brst16_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 515 eV (E16/odd) [mms3_dis_dist_brst16_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 750 eV (E18/even) [mms3_dis_dist_brst18_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 850 eV (E18/odd) [mms3_dis_dist_brst18_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~800 eV (E18 even-odd) [mms3_dis_dist_brst18_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 750 eV (E18/even) [mms3_dis_dist_brst18_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 850 eV (E18/odd) [mms3_dis_dist_brst18_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 1240 eV (E20/even) [mms3_dis_dist_brst20_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 1400 eV (E20/odd) [mms3_dis_dist_brst20_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~1320 eV (E20 even-odd) [mms3_dis_dist_brst20_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1240 eV (E20/even) [mms3_dis_dist_brst20_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1400 eV (E20/odd) [mms3_dis_dist_brst20_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 2620 eV (E23/even) [mms3_dis_dist_brst23_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 2970 eV (E23/odd) [mms3_dis_dist_brst23_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~2800 eV (E23 even-odd) [mms3_dis_dist_brst23_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2620 eV (E23/even) [mms3_dis_dist_brst23_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2970 eV (E23/odd) [mms3_dis_dist_brst23_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 5560 eV (E26/even) [mms3_dis_dist_brst26_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 6300 eV (E26/odd) [mms3_dis_dist_brst26_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~5920 eV (E26 even-odd) [mms3_dis_dist_brst26_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5560 eV (E26/even) [mms3_dis_dist_brst26_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 6300 eV (E26/odd) [mms3_dis_dist_brst26_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 25000 eV (E32/even) [mms3_dis_dist_brst32_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS burst sky-map instrument distribution - 28300 eV (E32/odd) [mms3_dis_dist_brst32_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~26600 eV (E32 even-odd) [mms3_dis_dist_brst32_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 25000 eV (E32/even) [mms3_dis_dist_brst32_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 28300 eV (E32/odd) [mms3_dis_dist_brst32_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [List/Create only in CDAWeb] 1-sigma error: MMS3 FPI/DIS burst sky-map instrument distribution [mms3_dis_disterr_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS vector of data-quality indicators at burst-start time [mms3_dis_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS3 FPI/DIS compression lossless/lossy indicator at survey-start time [mms3_dis_compressionloss_brst]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS3 FPI/DIS step table parity, this burst [mms3_dis_steptable_parity_brst]
      FPI/DIS alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS3 FPI/DIS Del-Phi (obs spin-phase) count at burst-start time [mms3_dis_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS3 FPI/DIS Del-Phi (obs spin-phase) angle at burst-start time [mms3_dis_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS3 FPI/DIS burst average f1 count values [mms3_dis_avgf1counts_brst]
      Average f1-count level as a function of energy
      
      MMS3 FPI/DIS burst sky-map microsecond offsets from Epoch [mms3_dis_steptimeoffsets_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order. Offsets reflect 128 steps over the 150 msec sweep
      period. See FPI docs for details.
      
      ---> MMS3 FPI/DIS sector de-Spin P value, this burst [mms3_dis_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS3 FPI/DIS burst sky-map instrument azimuthal angles [mms3_dis_phi_brst]
      see FPI docs for details
      
      MMS FPI/DIS burst sky-map parity 0/1 energies [mms3_dis_energy_brst]
      Energies (parity 0/1) in the 64-step FPI energy table
      
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MMS3_FPI_BRST_L2_DIS-MOMS (spase://NASA/NumericalData/MMS/3/FastPlasmaInvestigation/DIS/Burst/Level2/Moments/PT0.15S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode.  Data are also made available at survey (4.5
s, etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked.  Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available.  This product contains results from
integrating the standard moments of phase-space distributions formed from the
indicated data type (DES/DIS burst, FS or SS).  For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DIS 32-bit vector of data-quality indicators at burst-start time [mms3_dis_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>25%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied
      
      ---> MMS3 FPI/DIS compression lossless/lossy indicator at survey-start time [mms3_dis_compressionloss_brst]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS3 FPI/DIS step table parity, this burst [mms3_dis_steptable_parity_brst]
      FPI/DIS alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS3 FPI/DIS Del-Phi (obs spin-phase) count at burst-start time [mms3_dis_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS3 FPI/DIS Del-Phi (obs spin-phase) angle at burst-start time [mms3_dis_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      ---> MMS3 FPI/DIS sector de-Spin P value, this burst [mms3_dis_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS3 FPI/DIS ion energy spectrum "near" +X_DSC during this burst [mms3_dis_energyspectr_px_brst]
      Counts, summed over DSC velocity-dirs closest to +X_DSC, by energy bin.
      
      ---> MMS3 FPI/DIS ion energy spectrum "near" -X_DSC during this burst [mms3_dis_energyspectr_mx_brst]
      Counts, summed over DSC velocity-dirs closest to -X_DSC, by energy bin.
      
      ---> MMS3 FPI/DIS ion energy spectrum "near" +Y_DSC during this burst [mms3_dis_energyspectr_py_brst]
      Counts, summed over DSC velocity-dirs closest to +Y_DSC, by energy bin.
      
      ---> MMS3 FPI/DIS ion energy spectrum "near" -Y_DSC during this burst [mms3_dis_energyspectr_my_brst]
      Counts, summed over DSC velocity-dirs closest to -Y_DSC, by energy bin.
      
      ---> MMS3 FPI/DIS ion energy spectrum "near" +Z_DSC during this burst [mms3_dis_energyspectr_pz_brst]
      Counts, summed over DSC velocity-dirs closest to +Z_DSC, by energy bin.
      
      ---> MMS3 FPI/DIS ion energy spectrum "near" -Z_DSC during this burst [mms3_dis_energyspectr_mz_brst]
      Counts, summed over DSC velocity-dirs closest to -Z_DSC, by energy bin.
      
      MMS3 FPI/DIS omni-directional ion energy spectrum during this burst [mms3_dis_energyspectr_omni_brst]
      Differential energy flux, averaged (weighted by solid angle) over all look
      directions, by energy bin.
      
      MMS3 FPI/DIS ion background energy during this burst [mms3_dis_spectr_bg_brst]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look) background level.
      
      MMS3 FPI/DIS ion background number density during this burst [mms3_dis_numberdensity_bg_brst]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS3 FPI/DIS ion number density during this burst [mms3_dis_numberdensity_brst]
      
      
      ---> (no error bars displayed) MMS3 FPI/DIS ion number density during this burst [mms3_dis_numberdensity_brst_noerr]
      
      
      ---> MMS3 FPI/DIS ion number density error during this burst [mms3_dis_numberdensity_err_brst]
      
      
      MMS3 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms3_dis_densityextrapolation_low_brst]
      
      
      MMS3 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms3_dis_densityextrapolation_high_brst]
      
      
      MMS3 FPI/DIS ion bulk-velocity DBCS vector during this burst [mms3_dis_bulkv_dbcs_brst]
      
      
      MMS3 FPI/DIS ion bulk-velocity estimated spintone vector in DBCS during this burst [mms3_dis_bulkv_spintone_dbcs_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS3 FPI/DIS ion bulk-velocity DBCS vector during this burst [mms3_dis_bulkv_dbcs_brst_noerr]
      
      
      MMS3 FPI/DIS ion bulk-velocity GSE vector during this burst [mms3_dis_bulkv_gse_brst]
      
      
      MMS3 FPI/DIS ion bulk-velocity estimated spintone vector in GSE during this burst [mms3_dis_bulkv_spintone_gse_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS3 FPI/DIS ion bulk-velocity GSE vector during this burst [mms3_dis_bulkv_gse_brst_noerr]
      
      
      MMS3 FPI/DIS ion bulk-velocity spintone vector in DBCS during this burst [mms3_dis_bulkv_spin_dbcs_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS3 FPI/DIS ion bulk-velocity spintone vector in GSE during this burst [mms3_dis_bulkv_spin_gse_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS3 FPI/DIS ion pressure tensor DBCS matrix during this burst [mms3_dis_prestensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS ion pressure tensor GSE matrix during this burst [mms3_dis_prestensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS ion background pressure during this survey [mms3_dis_pres_bg_brst]
      
      
      MMS3 FPI/DIS ion temperature tensor DBCS matrix during this burst [mms3_dis_temptensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS ion temperature tensor GSE matrix during this burst [mms3_dis_temptensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS ion heat-flux DBCS vector during this burst [mms3_dis_heatq_dbcs_brst]
      
      
      MMS3 FPI/DIS ion heat-flux GSE vector during this burst [mms3_dis_heatq_gse_brst]
      
      
      MMS3 FPI/DIS ion parallel temperature during this BP [mms3_dis_temppara_brst]
      
      
      MMS3 FPI/DIS ion perpendicular temperature during this BP [mms3_dis_tempperp_brst]
      
      
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MMS3_FPI_BRST_L2_DIS-PARTMOMS (spase://NASA/NumericalData/MMS/3/FastPlasmaInvestigation/DIS/Burst/Level2/PartialMoments/PT0.15S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s,
etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked. Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available. This product contains partial moments that
come from performing the standard moment integrals over a limited portion of
velocity space. The resulting quantities are named similarly to their
corresponding standard moments, but are decorated with 'part' to differentiate.
For example, density_part is the density moment integrated from a particular
energy step to infinity. These partial moments are formed from the indicated
data type (DES/DIS burst, FS or SS). For convenience, some additional parameters
are included to augment those most commonly found in a moments product of this
sort, plus time-stamps and other annotation characterizing the state of the
instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DIS vector of data-quality indicators at burst-start time [mms3_dis_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation
      
      MMS3 FPI/DIS partial ion number density during this burst [mms3_dis_numberdensity_part_brst]
      
      
      MMS3 FPI/DIS partial ion bulk-velocity vector in DBCS during this burst [mms3_dis_bulkv_part_dbcs_brst]
      
      
      MMS3 FPI/DIS partial ion bulk-velocity vector in GSE during this burst [mms3_dis_bulkv_part_gse_brst]
      
      
      MMS3 FPI/DIS partial ion pressure tensor in DBCS during this burst [mms3_dis_prestensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS partial ion pressure tensor in GSE during this burst [mms3_dis_prestensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS partial ion temperature tensor in DBCS during this burst [mms3_dis_temptensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS partial ion temperature tensor in GSE during this burst [mms3_dis_temptensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS partial ion parallel temperature during this burst [mms3_dis_temppara_part_brst]
      
      
      MMS3 FPI/DIS partial ion perpendicular temperature during this burst [mms3_dis_tempperp_part_brst]
      
      
      MMS3 FPI/DIS recommended energy index during this burst [mms3_dis_part_index_brst]
      Recommended energy index during this burst
      
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MMS3_FPI_FAST_L2_DES-DIST (spase://NASA/NumericalData/MMS/3/FastPlasmaInvestigation/DES/Fast/Level2/Distribution/PT4.5S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data taken at burst (30/150 ms for DES/DIS)
resolution are aggregated on board and made available at survey (4.5 s)
resolution in this mode.  This product contains phase-space distribution maps of
results from surveying the high-resolution observations during each 4.5 s
period.  In particular, the (highest possible quality at the time of release)
corrected/converted "Fast Survey SkyMap" distributions are reported with
time-stamps and other annotation characterizing the state of the instrument
system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DES fast sky-map instrument distribution - 11.6 eV (E1) using averaged even/odd steps [mms3_des_dist_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 11.6 eV [mms3_des_dist_fast1_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES fast sky-map instrument distribution - 40.4 eV (E6) using averaged even/odd steps [mms3_des_dist_fast6]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 40.4 eV [mms3_des_dist_fast6_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES fast sky-map instrument distribution - 85.1 eV (E9) using averaged even/odd steps [mms3_des_dist_fast9]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 85.1 eV [mms3_des_dist_fast9_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES fast sky-map instrument distribution - 179 eV (E12) using averaged even/odd steps [mms3_des_dist_fast12]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 179 eV [mms3_des_dist_fast12_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES fast sky-map instrument distribution - 295 eV (E14) using averaged even/odd steps [mms3_des_dist_fast14]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 295 eV [mms3_des_dist_fast14_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES fast sky-map instrument distribution - 485 eV (E16) using averaged even/odd steps [mms3_des_dist_fast16]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 485 eV [mms3_des_dist_fast16_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES fast sky-map instrument distribution - 798 eV (E18) using averaged even/odd steps [mms3_des_dist_fast18]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 798 eV [mms3_des_dist_fast18_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES fast sky-map instrument distribution - 1310 eV (E20) using averaged even/odd steps [mms3_des_dist_fast20]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1310 eV [mms3_des_dist_fast20_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES fast sky-map instrument distribution - 2770 eV (E23) using averaged even/odd steps [mms3_des_dist_fast23]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2770 eV [mms3_des_dist_fast23_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES fast sky-map instrument distribution - 5840 eV (E26) using averaged even/odd steps [mms3_des_dist_fast26]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5840 eV [mms3_des_dist_fast26_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES fast sky-map instrument distribution - 26000 eV (E32) using averaged even/odd steps [mms3_des_dist_fast32]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 26000 eV [mms3_des_dist_fast32_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [Only List/Create in CDAWeb] MMS3 FPI/DES fast sky-map instrument distribution 1-sigma error [mms3_des_disterr_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES vector of data-quality indicators at fast survey-start time - 32-bit error flags [mms3_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS3 FPI/DES compression lossless/lossy indicator at survey-start time [mms3_des_compressionloss_fast]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS3 FPI/DES Del-Phi (obs spin-phase) count at fast survey-start time [mms3_des_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS3 FPI/DES Del-Phi (obs spin-phase) angle at fast survey-start time [mms3_des_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS3 FPI/DES fast survey average f1 count values [mms3_des_avgf1counts_fast]
      Average f1-count level as a function of energy
      
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MMS3_FPI_FAST_L2_DES-MOMS (spase://NASA/NumericalData/MMS/3/FastPlasmaInvestigation/DES/Fast/Level2/Moments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution.  Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This moments product
contains results from integrating the standard moments of phase-space
distributions formed from the indicated data type (DES/DIS burst, FS or SS). For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotation characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DES 32-bit vector of data-quality indicators at survey-start time [mms3_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>25%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied
      
      ---> MMS3 FPI/DES compression lossless/lossy indicator at survey-start time [mms3_des_compressionloss_fast]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS3 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms3_des_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS3 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms3_des_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS3 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms3_des_pitchangdist_lowen_fast]
      low energy bin: 0 eV - 200 eV.  pitch-angle bin size: 6 deg.
      
      ---> MMS3 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms3_des_pitchangdist_miden_fast]
      mid energy bin: 200 eV - 2 keV.  pitch-angle bin size: 6 deg.
      
      ---> MMS3 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms3_des_pitchangdist_highen_fast]
      high energy bin: 2 keV - 30 keV.  pitch-angle bin size: 6 deg.
      
      MMS3 FPI/DES electron energy spectrum "near" +X_DSC during this survey [mms3_des_energyspectr_px_fast]
      Counts, summed over DSC velocity-dirs closest to +X_DSC, by energy bin.
      
      ---> MMS3 FPI/DES electron energy spectrum "near" -X_DSC during this survey [mms3_des_energyspectr_mx_fast]
      Counts, summed over DSC velocity-dirs closest to -X_DSC, by energy bin.
      
      ---> MMS3 FPI/DES electron energy spectrum "near" +Y_DSC during this survey [mms3_des_energyspectr_py_fast]
      Counts, summed over DSC velocity-dirs closest to +Y_DSC, by energy bin.
      
      ---> MMS3 FPI/DES electron energy spectrum "near" -Y_DSC during this survey [mms3_des_energyspectr_my_fast]
      Counts, summed over DSC velocity-dirs closest to -Y_DSC, by energy bin.
      
      ---> MMS3 FPI/DES electron energy spectrum "near" +Z_DSC during this survey [mms3_des_energyspectr_pz_fast]
      Counts, summed over DSC velocity-dirs closest to +Z_DSC, by energy bin.
      
      ---> MMS3 FPI/DES electron energy spectrum "near" -Z_DSC during this survey [mms3_des_energyspectr_mz_fast]
      Counts, summed over DSC velocity-dirs closest to -Z_DSC, by energy bin.
      
      MMS3 FPI/DES electron energy parallel spectrum 30 degrees parallel to B during this survey [mms3_des_energyspectr_par_fast]
      Counts, summed within 30 degrees parallel bentPipe magnetic field.
      
      ---> MMS3 FPI/DES electron energy anti-parallel spectrum 30 degrees anti-parallel to B during this survey [mms3_des_energyspectr_anti_fast]
      Counts, summed within 30 degrees antiparallel to bentPipe magnetic field.
      
      ---> MMS3 FPI/DES electron energy perpendicular spectrum 60 degrees perpendicular to B during this survey [mms3_des_energyspectr_perp_fast]
      Counts, summed within 60 degrees perpendicular to bentPipe magnetic field.
      
      MMS3 FPI/DES omni-directional electron energy spectrum during this survey [mms3_des_energyspectr_omni_fast]
      Differential energy flux, averaged (weighted by solid angle) over all look
      directions, by energy bin.
      
      MMS3 FPI/DES electron number density during this survey [mms3_des_numberdensity_fast]
      
      
      ---> (no error bars displayed) MMS3 FPI/DES electron number density during this survey [mms3_des_numberdensity_fast_noerr]
      
      
      ---> MMS3 FPI/DES electron number density error during this survey [mms3_des_numberdensity_err_fast]
      
      
      MMS3 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms3_des_densityextrapolation_low_fast]
      
      
      MMS3 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms3_des_densityextrapolation_high_fast]
      
      
      MMS3 FPI/DES electron bulk-velocity DBCS vector during this survey [mms3_des_bulkv_dbcs_fast]
      
      
      MMS3 FPI/DES electron bulk-velocity estimated spintone vector in DBCS during this survey [mms3_des_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS3 FPI/DES electron bulk-velocity DBCS vector during this survey [mms3_des_bulkv_dbcs_fast_noerr]
      
      
      MMS3 FPI/DES electron bulk-velocity GSE vector during this survey [mms3_des_bulkv_gse_fast]
      
      
      MMS3 FPI/DES electron bulk-velocity estimated spintone vector in GSE during this survey [mms3_des_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS3 FPI/DES electron bulk-velocity GSE vector during this survey [mms3_des_bulkv_gse_fast_noerr]
      
      
      MMS3 FPI/DES electron bulk-velocity spintone vector in DBCS during this survey [mms3_des_bulkv_spin_dbcs_fast]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS3 FPI/DES electron bulk-velocity spintone vector in GSE during this survey [mms3_des_bulkv_spin_gse_fast]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS3 FPI/DES electron pressure tensor DBCS matrix during this survey [mms3_des_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES electron pressure tensor GSE matrix during this survey [mms3_des_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES electron temperature tensor DBCS matrix during this survey [mms3_des_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES electron temperature tensor GSE matrix during this survey [mms3_des_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES electron heat-flux DBCS vector during this survey [mms3_des_heatq_dbcs_fast]
      
      
      MMS3 FPI/DES electron heat-flux GSE vector during this survey [mms3_des_heatq_gse_fast]
      
      
      MMS3 FPI/DES electron parallel temperature during this BP [mms3_des_temppara_fast]
      
      
      MMS3 FPI/DES electron perpendicular temperature during this BP [mms3_des_tempperp_fast]
      
      
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MMS3_FPI_FAST_L2_DES-MOMSAUX
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DES vector of data-quality indicators at survey-start time [mms3_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only)
      
      MMS3 FPI/DES partial electron number density during this survey [mms3_des_numberdensity_part_fast]
      
      
      MMS3 FPI/DES partial electron bulk-velocity vector in DBCS during this survey [mms3_des_bulkv_part_dbcs_fast]
      
      
      MMS3 FPI/DES partial electron bulk-velocity vector in GSE during this survey [mms3_des_bulkv_part_gse_fast]
      
      
      MMS3 FPI/DES partial electron pressure tensor in DBCS during this survey [mms3_des_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES partial electron pressure tensor in GSE during this survey [mms3_des_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES partial electron temperature tensor in DBCS during this survey [mms3_des_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES partial electron temperature tensor in GSE during this survey [mms3_des_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES partial electron parallel temperature during this survey [mms3_des_temppara_part_fast]
      
      
      MMS3 FPI/DES partial electron perpendicular temperature during this survey [mms3_des_tempperp_part_fast]
      
      
      MMS3 FPI/DES recommended energy index for partial moments during this survey [mms3_des_part_index_fast]
      Recommended energy index during this survey
      
      MMS3 FPI/DES compression lossless/lossy indicator at survey-start time [mms3_des_compressionloss_fast]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS3 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms3_des_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS3 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms3_des_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS3 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms3_des_pitchangdist_lowen_fast]
      Low energy bin: energy steps 0-10 (of total steps 0-31). Pitch-angle bin size: 6
      deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS3 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms3_des_pitchangdist_miden_fast]
      Mid energy bin: energy steps 11-20 (of total steps 0-31). Pitch-angle bin size:
      6 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS3 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms3_des_pitchangdist_highen_fast]
      High energy bin: energy steps 21-31 (of total steps 0-31). Pitch-angle bin size:
      6 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS3 FPI/DES electron energy spectrum "near" +X_DBCS during this survey [mms3_des_energyspectr_px_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS3 FPI/DES electron energy spectrum "near" -X_DBCS during this survey [mms3_des_energyspectr_mx_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS3 FPI/DES electron energy spectrum "near" +Y_DBCS during this survey [mms3_des_energyspectr_py_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS3 FPI/DES electron energy spectrum "near" -Y_DBCS during this survey [mms3_des_energyspectr_my_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS3 FPI/DES electron energy spectrum "near" +Z_DBCS during this survey [mms3_des_energyspectr_pz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS3 FPI/DES electron energy spectrum "near" -Z_DBCS during this survey [mms3_des_energyspectr_mz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS3 FPI/DES electron energy parallel to the magnetic field direction during this survey [mms3_des_energyspectr_par_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within 30
      degrees of the magnetic field direction.
      
      MMS3 FPI/DES electron energy anti-parallel to the magnetic field direction during this survey [mms3_des_energyspectr_anti_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      150 degrees of the magnetic field direction.
      
      MMS3 FPI/DES electron energy perpendicular to the magnetic field direction during this survey [mms3_des_energyspectr_perp_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      60-120 degrees of the magnetic field direction.
      
      MMS3 FPI/DES omni-directional electron energy spectrum during this survey [mms3_des_energyspectr_omni_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS3 FPI/DES electron number density during this survey [mms3_des_numberdensity_fast]
      
      
      MMS3 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms3_des_densityextrapolation_low_fast]
      
      
      MMS3 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms3_des_densityextrapolation_high_fast]
      
      
      MMS3 FPI/DES electron bulk-velocity vector in DBCS during this survey [mms3_des_bulkv_dbcs_fast]
      
      
      MMS3 FPI/DES electron bulk-velocity estimated spintone vector in DBCS during this survey [mms3_des_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS3 FPI/DES electron bulk-velocity vector in GSE during this survey [mms3_des_bulkv_gse_fast]
      
      
      MMS3 FPI/DES electron bulk-velocity estimated spintone vector in GSE during this survey [mms3_des_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS3 FPI/DES electron pressure tensor in DBCS during this survey [mms3_des_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES electron pressure tensor in GSE during this survey [mms3_des_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES electron temperature tensor in DBCS during this survey [mms3_des_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES electron temperature tensor in GSE during this survey [mms3_des_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES electron heat-flux vector in DBCS during this survey [mms3_des_heatq_dbcs_fast]
      
      
      MMS3 FPI/DES electron heat-flux vector in GSE during this survey [mms3_des_heatq_gse_fast]
      
      
      MMS3 FPI/DES electron parallel temperature during this BP [mms3_des_temppara_fast]
      
      
      MMS3 FPI/DES electron perpendicular temperature during this BP [mms3_des_tempperp_fast]
      
      
      MMS3 FPI/DES S/C potential mean [mms3_des_scpot_mean_fast]
      Average spacecraft potential during this FP used to shift the measure energies.
      
      MMS3 FPI/DES S/C potential max [mms3_des_scpot_max_fast]
      Maximum spacecraft potential during this FP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      MMS3 FPI/DES Mag data X,Y,Z,Norm DSC components [nT] at survey-start time [mms3_des_fpibentpipe_dsc_fast]
      X, Y, Z are unit vector components.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms3_des_fpib_gse_srvy_fast]
      Averaged survey magnetic field data during this FP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms3_des_fpib_dmpa_srvy_fast]
      Averaged survey magnetic field data during this FP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms3_des_pos_gse_fast]
      
      
      Position in GSM coordinates, 30 second [mms3_des_pos_gsm_fast]
      
      
      MMS3 number density integrands [mms3_des_numberdensity_int_fast]
      Integrand terms used in normalized energy integration for number density
      
      number flux [mms3_des_numberflux_int_dbcs_fast]
      Integrand terms used in normalized energy integration for number flux
      
      MMS3 pressure tensor integrands [mms3_des_prestensor_int_dbcs_fast]
      Integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms3_des_ugrid_int_fast]
      
      
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MMS3_FPI_FAST_L2_DES-PARTMOMS (spase://NASA/NumericalData/MMS/3/FastPlasmaInvestigation/DES/Fast/Level2/PartialMoments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DES vector of data-quality indicators at survey-start time [mms3_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only)
      
      MMS3 FPI/DES partial electron number density during this survey [mms3_des_numberdensity_part_fast]
      
      
      MMS3 FPI/DES partial electron bulk-velocity vector in DBCS during this survey [mms3_des_bulkv_part_dbcs_fast]
      
      
      MMS3 FPI/DES partial electron bulk-velocity vector in GSE during this survey [mms3_des_bulkv_part_gse_fast]
      
      
      MMS3 FPI/DES partial electron pressure tensor in DBCS during this survey [mms3_des_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES partial electron pressure tensor in GSE during this survey [mms3_des_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES partial electron temperature tensor in DBCS during this survey [mms3_des_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES partial electron temperature tensor in GSE during this survey [mms3_des_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES partial electron parallel temperature during this survey [mms3_des_temppara_part_fast]
      
      
      MMS3 FPI/DES partial electron perpendicular temperature during this survey [mms3_des_tempperp_part_fast]
      
      
      MMS3 FPI/DES recommended energy index during this survey [mms3_des_part_index_fast]
      Recommended energy index during this survey
      
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MMS3_FPI_FAST_L2_DIS-DIST (spase://NASA/NumericalData/MMS/3/FastPlasmaInvestigation/DIS/Fast/Level2/Distribution/PT4.5S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data taken at burst (30/150 ms for DES/DIS)
resolution are aggregated on board and made available at survey (4.5 s)
resolution in this mode.  This product contains phase-space distribution maps of
results from surveying the high-resolution observations during each 4.5 s
period.  In particular, the (highest possible quality at the time of release)
corrected/converted "Fast Survey SkyMap" distributions are reported with
time-stamps and other annotation characterizing the state of the instrument
system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DIS fast sky-map instrument distribution - 11.3 eV (E1) using averaged even/odd steps [mms3_dis_dist_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 11.3 eV [mms3_dis_dist_fast1_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS fast sky-map instrument distribution - 39.6 eV (E6) using averaged even/odd steps [mms3_dis_dist_fast6]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 39.6 eV [mms3_dis_dist_fast6_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS fast sky-map instrument distribution - 83.9 eV (E9 using averaged even/odd steps) [mms3_dis_dist_fast9]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 83.9 eV [mms3_dis_dist_fast9_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS fast sky-map instrument distribution - 178 eV (E12) using averaged even/odd steps [mms3_dis_dist_fast12]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 178 eV [mms3_dis_dist_fast12_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS fast sky-map instrument distribution - 293 eV (E14) using averaged even/odd steps [mms3_dis_dist_fast14]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 293 eV [mms3_dis_dist_fast14_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS fast sky-map instrument distribution - 484 eV (E16) using averaged even/odd steps [mms3_dis_dist_fast16]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 484 eV [mms3_dis_dist_fast16_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS fast sky-map instrument distribution - 799 eV (E18) using averaged even/odd steps [mms3_dis_dist_fast18]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 799 eV [mms3_dis_dist_fast18_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS fast sky-map instrument distribution - 1320 eV (E20) using averaged even/odd steps [mms3_dis_dist_fast20]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1320 eV [mms3_dis_dist_fast20_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS fast sky-map instrument distribution - 2800 eV (E23) using averaged even/odd steps [mms3_dis_dist_fast23]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2800 eV [mms3_dis_dist_fast23_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS fast sky-map instrument distribution - 5920 eV (E26) using averaged even/odd steps [mms3_dis_dist_fast26]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5920 eV [mms3_dis_dist_fast26_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS fast sky-map instrument distribution - 26600 eV (E32) using averaged even/odd steps [mms3_dis_dist_fast32]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 26600 eV [mms3_dis_dist_fast32_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [Only List/Create in CDAWeb] MMS3 FPI/DIS fast sky-map instrument distribution 1-sigma error [mms3_dis_disterr_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS vector of data-quality indicators at fast survey-start time - 32-bit error flags [mms3_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS3 FPI/DIS compression lossless/lossy indicator at survey-start time [mms3_dis_compressionloss_fast]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS3 FPI/DIS Del-Phi (obs spin-phase) count at fast survey-start time [mms3_dis_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS3 FPI/DIS Del-Phi (obs spin-phase) angle at fast survey-start time [mms3_dis_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS3 FPI/DIS fast survey average f1 count values [mms3_dis_avgf1counts_fast]
      Average f1-count level as a function of energy
      
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MMS3_FPI_FAST_L2_DIS-MOMS (spase://NASA/NumericalData/MMS/3/FastPlasmaInvestigation/DIS/Fast/Level2/Moments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution.  Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This moments product
contains results from integrating the standard moments of phase-space
distributions formed from the indicated data type (DES/DIS burst, FS or SS). For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotation characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DIS vector of data-quality indicators at survey-start time [mms3_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation, Bit-14 =
      high MMS3 spintone due to DIS008 anomaly
      
      ---> MMS3 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms3_dis_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      ---> MMS3 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms3_dis_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS3 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms3_dis_energyspectr_px_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      ---> MMS3 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms3_dis_energyspectr_mx_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      ---> MMS3 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms3_dis_energyspectr_py_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      ---> MMS3 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms3_dis_energyspectr_my_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      ---> MMS3 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms3_dis_energyspectr_pz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      ---> MMS3 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms3_dis_energyspectr_mz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS3 FPI/DIS omni-directional ion energy spectrum during this survey [mms3_dis_energyspectr_omni_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS3 FPI/DIS ion background energy during this survey [mms3_dis_spectr_bg_fast]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS3 FPI/DIS ion background number density during this survey [mms3_dis_numberdensity_bg_fast]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS3 FPI/DIS ion number density during this survey [mms3_dis_numberdensity_fast]
      
      
      ---> (no error bars displayed) MMS3 FPI/DIS ion number density during this survey [mms3_dis_numberdensity_fast_noerr]
      
      
      MMS3 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms3_dis_densityextrapolation_low_fast]
      
      
      MMS3 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms3_dis_densityextrapolation_high_fast]
      
      
      MMS3 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms3_dis_bulkv_dbcs_fast]
      
      
      ---> (no error bars displayed) MMS3 FPI/DIS ion bulk-velocity DBCS vector during this survey [mms3_dis_bulkv_dbcs_fast_noerr]
      
      
      MMS3 FPI/DIS ion bulk-velocity estimated spintone vector in DBCS during this survey [mms3_dis_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS3 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms3_dis_bulkv_gse_fast]
      
      
      MMS3 FPI/DIS ion bulk-velocity estimated spintone vector in GSE during this survey [mms3_dis_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS3 FPI/DIS ion bulk-velocity GSE vector during this survey [mms3_dis_bulkv_gse_fast_noerr]
      
      
      MMS3 FPI/DIS ion pressure tensor in DBCS during this survey [mms3_dis_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS ion pressure tensor in GSE during this survey [mms3_dis_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS ion background pressure during this survey [mms3_dis_pres_bg_fast]
      
      
      MMS3 FPI/DIS ion temperature tensor in DBCS during this survey [mms3_dis_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS ion temperature tensor in GSE during this survey [mms3_dis_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS ion heat-flux vector in DBCS during this survey [mms3_dis_heatq_dbcs_fast]
      
      
      MMS3 FPI/DIS ion heat-flux vector in GSE during this survey [mms3_dis_heatq_gse_fast]
      
      
      MMS3 FPI/DIS ion parallel temperature during this BP [mms3_dis_temppara_fast]
      
      
      MMS3 FPI/DIS ion perpendicular temperature during this BP [mms3_dis_tempperp_fast]
      
      
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MMS3_FPI_FAST_L2_DIS-MOMSAUX
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DIS vector of data-quality indicators at survey-start time [mms3_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation
      
      MMS3 FPI/DIS partial ion number density during this survey [mms3_dis_numberdensity_part_fast]
      
      
      MMS3 FPI/DIS partial ion bulk-velocity vector in DBCS during this survey [mms3_dis_bulkv_part_dbcs_fast]
      
      
      MMS3 FPI/DIS partial ion bulk-velocity vector in GSE during this survey [mms3_dis_bulkv_part_gse_fast]
      
      
      MMS3 FPI/DIS partial ion pressure tensor in DBCS during this survey [mms3_dis_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS partial ion pressure tensor in GSE during this survey [mms3_dis_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS partial ion temperature tensor in DBCS during this survey [mms3_dis_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS partial ion temperature tensor in GSE during this survey [mms3_dis_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS partial ion parallel temperature during this survey [mms3_dis_temppara_part_fast]
      
      
      MMS3 FPI/DIS partial ion perpendicular temperature during this survey [mms3_dis_tempperp_part_fast]
      
      
      MMS3 FPI/DIS recommended energy index for partial moments during this survey [mms3_dis_part_index_fast]
      Recommended energy index during this survey
      
      MMS3 FPI/DIS compression lossless/lossy indicator at survey-start time [mms3_dis_compressionloss_fast]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS3 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms3_dis_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS3 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms3_dis_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS3 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms3_dis_energyspectr_px_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms3_dis_energyspectr_mx_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms3_dis_energyspectr_py_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms3_dis_energyspectr_my_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms3_dis_energyspectr_pz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms3_dis_energyspectr_mz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS3 FPI/DIS omni-directional ion energy spectrum during this survey [mms3_dis_energyspectr_omni_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS3 FPI/DIS ion background energy during this survey [mms3_dis_spectr_bg_fast]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS3 FPI/DIS ion background number density during this survey [mms3_dis_numberdensity_bg_fast]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS3 FPI/DIS ion number density during this survey [mms3_dis_numberdensity_fast]
      
      
      MMS3 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms3_dis_densityextrapolation_low_fast]
      
      
      MMS3 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms3_dis_densityextrapolation_high_fast]
      
      
      MMS3 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms3_dis_bulkv_dbcs_fast]
      
      
      MMS3 FPI/DIS ion bulk-velocity estimated spintone vector in DBCS during this survey [mms3_dis_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS3 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms3_dis_bulkv_gse_fast]
      
      
      MMS3 FPI/DIS ion bulk-velocity estimated spintone vector in GSE during this survey [mms3_dis_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS3 FPI/DIS ion pressure tensor in DBCS during this survey [mms3_dis_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS ion pressure tensor in GSE during this survey [mms3_dis_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS ion background pressure during this survey [mms3_dis_pres_bg_fast]
      
      
      MMS3 FPI/DIS ion temperature tensor in DBCS during this survey [mms3_dis_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS ion temperature tensor in GSE during this survey [mms3_dis_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS ion heat-flux vector in DBCS during this survey [mms3_dis_heatq_dbcs_fast]
      
      
      MMS3 FPI/DIS ion heat-flux vector in GSE during this survey [mms3_dis_heatq_gse_fast]
      
      
      MMS3 FPI/DIS ion parallel temperature during this BP [mms3_dis_temppara_fast]
      
      
      MMS3 FPI/DIS ion perpendicular temperature during this BP [mms3_dis_tempperp_fast]
      
      
      MMS3 FPI/DIS S/C potential mean [mms3_dis_scpot_mean_fast]
      Average spacecraft potential during this FP used to shift the measure energies.
      
      MMS3 FPI/DIS S/C potential max [mms3_dis_scpot_max_fast]
      Maximum spacecraft potential during this FP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      MMS3 FPI/DIS Mag data X,Y,Z,Norm DSC components [nT] at survey-start time [mms3_dis_fpibentpipe_dsc_fast]
      X, Y, Z are unit vector components.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms3_dis_fpib_gse_srvy_fast]
      Averaged survey magnetic field data during this FP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms3_dis_fpib_dmpa_srvy_fast]
      Averaged survey magnetic field data during this FP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms3_dis_pos_gse_fast]
      
      
      Position in GSM coordinates, 30 second [mms3_dis_pos_gsm_fast]
      
      
      MMS3 number density integrands [mms3_dis_numberdensity_int_fast]
      integrand terms used in normalized energy integration for number density
      
      number flux [mms3_dis_numberflux_int_dbcs_fast]
      integrand terms used in normalized energy integration for number flux
      
      MMS3 pressure tensor integrands [mms3_dis_prestensor_int_dbcs_fast]
      integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms3_dis_ugrid_int_fast]
      
      
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MMS3_FPI_FAST_L2_DIS-PARTMOMS (spase://NASA/NumericalData/MMS/3/FastPlasmaInvestigation/DIS/Fast/Level2/PartialMoments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DIS vector of data-quality indicators at survey-start time [mms3_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation
      
      MMS3 FPI/DIS partial ion number density during this survey [mms3_dis_numberdensity_part_fast]
      
      
      MMS3 FPI/DIS partial ion bulk-velocity vector in DBCS during this survey [mms3_dis_bulkv_part_dbcs_fast]
      
      
      MMS3 FPI/DIS partial ion bulk-velocity vector in GSE during this survey [mms3_dis_bulkv_part_gse_fast]
      
      
      MMS3 FPI/DIS partial ion pressure tensor in DBCS during this survey [mms3_dis_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS partial ion pressure tensor in GSE during this survey [mms3_dis_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS partial ion temperature tensor in DBCS during this survey [mms3_dis_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS partial ion temperature tensor in GSE during this survey [mms3_dis_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS partial ion parallel temperature during this survey [mms3_dis_temppara_part_fast]
      
      
      MMS3 FPI/DIS partial ion perpendicular temperature during this survey [mms3_dis_tempperp_part_fast]
      
      
      MMS3 FPI/DIS recommended energy index during this survey [mms3_dis_part_index_fast]
      Recommended energy index during this survey
      
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MMS3_FPI_SLOW_L2_DES-DIST
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode.  This product contains phase-space distribution maps of those
survey-resolution data from Slow Mode.  In particular, the (highest possible
quality at the time of release) corrected/converted "Slow Survey SkyMap"
distributions are reported with time-stamps and other annotation characterizing
the state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DES vector of data-quality indicators at survey-start time [mms3_des_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = compression pipeline error
      
      MMS3 FPI/DES compression lossless/lossy indicator at survey-start time [mms3_des_compressionloss_slow]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS3 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms3_des_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS3 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms3_des_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS3 FPI/DES Slow Survey sky-map instrument distribution [mms3_des_dist_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES Slow Survey sky-map instrument distribution 1-sigma error [mms3_des_disterr_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DES slow survey average f1 count values [mms3_des_avgf1counts_slow]
      Average f1-count level as a function of energy
      
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MMS3_FPI_SLOW_L2_DES-MOMS
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DES vector of data-quality indicators at survey-start time [mms3_des_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only)
      
      MMS3 FPI/DES compression lossless/lossy indicator at survey-start time [mms3_des_compressionloss_slow]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS3 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms3_des_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS3 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms3_des_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS3 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms3_des_pitchangdist_lowen_slow]
      Low energy bin: energy steps 0-10 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS3 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms3_des_pitchangdist_miden_slow]
      Mid energy bin: energy steps 11-20 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS3 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms3_des_pitchangdist_highen_slow]
      High energy bin: energy steps 21-31 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS3 FPI/DES electron energy spectrum "near" +X_DBCS during this survey [mms3_des_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS3 FPI/DES electron energy spectrum "near" -X_DBCS during this survey [mms3_des_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS3 FPI/DES electron energy spectrum "near" +Y_DBCS during this survey [mms3_des_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS3 FPI/DES electron energy spectrum "near" -Y_DBCS during this survey [mms3_des_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS3 FPI/DES electron energy spectrum "near" +Z_DBCS during this survey [mms3_des_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS3 FPI/DES electron energy spectrum "near" -Z_DBCS during this survey [mms3_des_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS3 FPI/DES electron energy parallel to the magnetic field direction during this survey [mms3_des_energyspectr_par_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within 30
      degrees of the magnetic field direction.
      
      MMS3 FPI/DES electron energy anti-parallel to the magnetic field direction during this survey [mms3_des_energyspectr_anti_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      150 degrees of the magnetic field direction.
      
      MMS3 FPI/DES electron energy perpendicular to the magnetic field direction during this survey [mms3_des_energyspectr_perp_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      60-120 degrees of the magnetic field direction.
      
      MMS3 FPI/DES omni-directional electron energy spectrum during this survey [mms3_des_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS3 FPI/DES electron number density during this survey [mms3_des_numberdensity_slow]
      
      
      MMS3 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms3_des_densityextrapolation_low_slow]
      
      
      MMS3 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms3_des_densityextrapolation_high_slow]
      
      
      MMS3 FPI/DES electron bulk-velocity vector in DBCS during this survey [mms3_des_bulkv_dbcs_slow]
      
      
      MMS3 FPI/DES electron bulk-velocity vector in GSE during this survey [mms3_des_bulkv_gse_slow]
      
      
      MMS3 FPI/DES electron pressure tensor in DBCS during this survey [mms3_des_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES electron pressure tensor in GSE during this survey [mms3_des_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES electron temperature tensor in DBCS during this survey [mms3_des_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES electron temperature tensor in GSE during this survey [mms3_des_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES electron heat-flux vector in DBCS during this survey [mms3_des_heatq_dbcs_slow]
      
      
      MMS3 FPI/DES electron heat-flux vector in GSE during this survey [mms3_des_heatq_gse_slow]
      
      
      MMS3 FPI/DES electron parallel temperature during this BP [mms3_des_temppara_slow]
      
      
      MMS3 FPI/DES electron perpendicular temperature during this BP [mms3_des_tempperp_slow]
      
      
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MMS3_FPI_SLOW_L2_DES-MOMSAUX
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DES vector of data-quality indicators at survey-start time [mms3_des_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only)
      
      MMS3 FPI/DES partial electron number density during this survey [mms3_des_numberdensity_part_slow]
      
      
      MMS3 FPI/DES partial electron bulk-velocity vector in DBCS during this survey [mms3_des_bulkv_part_dbcs_slow]
      
      
      MMS3 FPI/DES partial electron bulk-velocity vector in GSE during this survey [mms3_des_bulkv_part_gse_slow]
      
      
      MMS3 FPI/DES partial electron pressure tensor in DBCS during this survey [mms3_des_prestensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES partial electron pressure tensor in GSE during this survey [mms3_des_prestensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES partial electron temperature tensor in DBCS during this survey [mms3_des_temptensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES partial electron temperature tensor in GSE during this survey [mms3_des_temptensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES partial electron parallel temperature during this survey [mms3_des_temppara_part_slow]
      
      
      MMS3 FPI/DES partial electron perpendicular temperature during this survey [mms3_des_tempperp_part_slow]
      
      
      MMS3 FPI/DES recommended energy index for partial moments during this survey [mms3_des_part_index_slow]
      Recommended energy index during this survey
      
      MMS3 FPI/DES compression lossless/lossy indicator at survey-start time [mms3_des_compressionloss_slow]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS3 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms3_des_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS3 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms3_des_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS3 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms3_des_pitchangdist_lowen_slow]
      Low energy bin: energy steps 0-10 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS3 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms3_des_pitchangdist_miden_slow]
      Mid energy bin: energy steps 11-20 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS3 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms3_des_pitchangdist_highen_slow]
      High energy bin: energy steps 21-31 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS3 FPI/DES electron energy spectrum "near" +X_DBCS during this survey [mms3_des_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS3 FPI/DES electron energy spectrum "near" -X_DBCS during this survey [mms3_des_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS3 FPI/DES electron energy spectrum "near" +Y_DBCS during this survey [mms3_des_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS3 FPI/DES electron energy spectrum "near" -Y_DBCS during this survey [mms3_des_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS3 FPI/DES electron energy spectrum "near" +Z_DBCS during this survey [mms3_des_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS3 FPI/DES electron energy spectrum "near" -Z_DBCS during this survey [mms3_des_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS3 FPI/DES electron energy parallel to the magnetic field direction during this survey [mms3_des_energyspectr_par_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within 30
      degrees of the magnetic field direction.
      
      MMS3 FPI/DES electron energy anti-parallel to the magnetic field direction during this survey [mms3_des_energyspectr_anti_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      150 degrees of the magnetic field direction.
      
      MMS3 FPI/DES electron energy perpendicular to the magnetic field direction during this survey [mms3_des_energyspectr_perp_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      60-120 degrees of the magnetic field direction.
      
      MMS3 FPI/DES omni-directional electron energy spectrum during this survey [mms3_des_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS3 FPI/DES electron number density during this survey [mms3_des_numberdensity_slow]
      
      
      MMS3 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms3_des_densityextrapolation_low_slow]
      
      
      MMS3 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms3_des_densityextrapolation_high_slow]
      
      
      MMS3 FPI/DES electron bulk-velocity vector in DBCS during this survey [mms3_des_bulkv_dbcs_slow]
      
      
      MMS3 FPI/DES electron bulk-velocity vector in GSE during this survey [mms3_des_bulkv_gse_slow]
      
      
      MMS3 FPI/DES electron pressure tensor in DBCS during this survey [mms3_des_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES electron pressure tensor in GSE during this survey [mms3_des_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DES electron temperature tensor in DBCS during this survey [mms3_des_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES electron temperature tensor in GSE during this survey [mms3_des_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DES electron heat-flux vector in DBCS during this survey [mms3_des_heatq_dbcs_slow]
      
      
      MMS3 FPI/DES electron heat-flux vector in GSE during this survey [mms3_des_heatq_gse_slow]
      
      
      MMS3 FPI/DES electron parallel temperature during this BP [mms3_des_temppara_slow]
      
      
      MMS3 FPI/DES electron perpendicular temperature during this BP [mms3_des_tempperp_slow]
      
      
      MMS3 FPI/DES S/C potential mean [mms3_des_scpot_mean_slow]
      Average spacecraft potential during this SP used to shift the measure energies.
      
      MMS3 FPI/DES S/C potential max [mms3_des_scpot_max_slow]
      Maximum spacecraft potential during this SP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms3_des_fpib_gse_srvy_slow]
      Averaged survey magnetic field data during this SP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms3_des_fpib_dmpa_srvy_slow]
      Averaged survey magnetic field data during this SP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms3_des_pos_gse_slow]
      
      
      Position in GSM coordinates, 30 second [mms3_des_pos_gsm_slow]
      
      
      MMS3 number density integrands [mms3_des_numberdensity_int_slow]
      integrand terms used in normalized energy integration for number density
      
      number flux [mms3_des_numberflux_int_dbcs_slow]
      integrand terms used in normalized energy integration for number flux
      
      MMS3 pressure tensor integrands [mms3_des_prestensor_int_dbcs_slow]
      integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms3_des_ugrid_int_slow]
      
      
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MMS3_FPI_SLOW_L2_DIS-DIST
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode.  This product contains phase-space distribution maps of those
survey-resolution data from Slow Mode.  In particular, the (highest possible
quality at the time of release) corrected/converted "Slow Survey SkyMap"
distributions are reported with time-stamps and other annotation characterizing
the state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DIS vector of data-quality indicators at survey-start time [mms3_dis_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = compression pipeline error
      
      MMS3 FPI/DIS compression lossless/lossy indicator at survey-start time [mms3_dis_compressionloss_slow]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS3 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms3_dis_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS3 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms3_dis_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS3 FPI/DIS Slow Survey sky-map instrument distribution [mms3_dis_dist_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS Slow Survey sky-map instrument distribution 1-sigma error [mms3_dis_disterr_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS3 FPI/DIS slow survey average f1 count values [mms3_dis_avgf1counts_slow]
      Average f1-count level as a function of energy
      
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MMS3_FPI_SLOW_L2_DIS-MOMS
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DIS vector of data-quality indicators at survey-start time [mms3_dis_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only), Bit-13 =
      significant (>=20%) penetrating radiation, Bit-14 = high MMS3 spintone due to
      DIS008 anomaly
      
      MMS3 FPI/DIS compression lossless/lossy indicator at survey-start time [mms3_dis_compressionloss_slow]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS3 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms3_dis_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS3 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms3_dis_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS3 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms3_dis_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms3_dis_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms3_dis_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms3_dis_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms3_dis_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms3_dis_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS3 FPI/DIS omni-directional ion energy spectrum during this survey [mms3_dis_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS3 FPI/DIS ion background energy during this survey [mms3_dis_spectr_bg_slow]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS3 FPI/DIS ion background number density during this survey [mms3_dis_numberdensity_bg_slow]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS3 FPI/DIS ion number density during this survey [mms3_dis_numberdensity_slow]
      
      
      MMS3 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms3_dis_densityextrapolation_low_slow]
      
      
      MMS3 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms3_dis_densityextrapolation_high_slow]
      
      
      MMS3 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms3_dis_bulkv_dbcs_slow]
      
      
      MMS3 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms3_dis_bulkv_gse_slow]
      
      
      MMS3 FPI/DIS ion pressure tensor in DBCS during this survey [mms3_dis_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS ion pressure tensor in GSE during this survey [mms3_dis_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS ion background pressure during this survey [mms3_dis_pres_bg_slow]
      
      
      MMS3 FPI/DIS ion temperature tensor in DBCS during this survey [mms3_dis_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS ion temperature tensor in GSE during this survey [mms3_dis_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS ion heat-flux vector in DBCS during this survey [mms3_dis_heatq_dbcs_slow]
      
      
      MMS3 FPI/DIS ion heat-flux vector in GSE during this survey [mms3_dis_heatq_gse_slow]
      
      
      MMS3 FPI/DIS ion parallel temperature during this BP [mms3_dis_temppara_slow]
      
      
      MMS3 FPI/DIS ion perpendicular temperature during this BP [mms3_dis_tempperp_slow]
      
      
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MMS3_FPI_SLOW_L2_DIS-MOMSAUX
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS3 FPI/DIS vector of data-quality indicators at survey-start time [mms3_dis_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only), Bit-13 =
      significant (>=20%) penetrating radiation, Bit-14 = high MMS3 spintone due to
      DIS008 anomaly
      
      MMS3 FPI/DIS partial ion number density during this survey [mms3_dis_numberdensity_part_slow]
      
      
      MMS3 FPI/DIS partial ion bulk-velocity vector in DBCS during this survey [mms3_dis_bulkv_part_dbcs_slow]
      
      
      MMS3 FPI/DIS partial ion bulk-velocity vector in GSE during this survey [mms3_dis_bulkv_part_gse_slow]
      
      
      MMS3 FPI/DIS partial ion pressure tensor in DBCS during this survey [mms3_dis_prestensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS partial ion pressure tensor in GSE during this survey [mms3_dis_prestensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS partial ion temperature tensor in DBCS during this survey [mms3_dis_temptensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS partial ion temperature tensor in GSE during this survey [mms3_dis_temptensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS partial ion parallel temperature during this survey [mms3_dis_temppara_part_slow]
      
      
      MMS3 FPI/DIS partial ion perpendicular temperature during this survey [mms3_dis_tempperp_part_slow]
      
      
      MMS3 FPI/DIS recommended energy index for partial moments during this survey [mms3_dis_part_index_slow]
      Recommended energy index during this survey
      
      MMS3 FPI/DIS compression lossless/lossy indicator at survey-start time [mms3_dis_compressionloss_slow]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS3 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms3_dis_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS3 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms3_dis_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS3 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms3_dis_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms3_dis_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms3_dis_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms3_dis_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms3_dis_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS3 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms3_dis_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS3 FPI/DIS omni-directional ion energy spectrum during this survey [mms3_dis_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS3 FPI/DIS ion background energy during this survey [mms3_dis_spectr_bg_slow]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS3 FPI/DIS ion background number density during this survey [mms3_dis_numberdensity_bg_slow]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS3 FPI/DIS ion number density during this survey [mms3_dis_numberdensity_slow]
      
      
      MMS3 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms3_dis_densityextrapolation_low_slow]
      
      
      MMS3 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms3_dis_densityextrapolation_high_slow]
      
      
      MMS3 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms3_dis_bulkv_dbcs_slow]
      
      
      MMS3 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms3_dis_bulkv_gse_slow]
      
      
      MMS3 FPI/DIS ion pressure tensor in DBCS during this survey [mms3_dis_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS ion pressure tensor in GSE during this survey [mms3_dis_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS3 FPI/DIS ion background pressure during this survey [mms3_dis_pres_bg_slow]
      
      
      MMS3 FPI/DIS ion temperature tensor in DBCS during this survey [mms3_dis_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS ion temperature tensor in GSE during this survey [mms3_dis_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS3 FPI/DIS ion heat-flux vector in DBCS during this survey [mms3_dis_heatq_dbcs_slow]
      
      
      MMS3 FPI/DIS ion heat-flux vector in GSE during this survey [mms3_dis_heatq_gse_slow]
      
      
      MMS3 FPI/DIS ion parallel temperature during this BP [mms3_dis_temppara_slow]
      
      
      MMS3 FPI/DIS ion perpendicular temperature during this BP [mms3_dis_tempperp_slow]
      
      
      MMS3 FPI/DIS S/C potential mean [mms3_dis_scpot_mean_slow]
      Average spacecraft potential during this SP used to shift the measure energies.
      
      MMS3 FPI/DIS S/C potential max [mms3_dis_scpot_max_slow]
      Maximum spacecraft potential during this SP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms3_dis_fpib_gse_srvy_slow]
      Averaged survey magnetic field data during this SP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms3_dis_fpib_dmpa_srvy_slow]
      Averaged survey magnetic field data during this SP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms3_dis_pos_gse_slow]
      
      
      Position in GSM coordinates, 30 second [mms3_dis_pos_gsm_slow]
      
      
      MMS3 number density integrands [mms3_dis_numberdensity_int_slow]
      integrand terms used in normalized energy integration for number density
      
      number flux [mms3_dis_numberflux_int_dbcs_slow]
      integrand terms used in normalized energy integration for number flux
      
      MMS3 pressure tensor integrands [mms3_dis_prestensor_int_dbcs_slow]
      integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms3_dis_ugrid_int_slow]
      
      
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MMS3_HPCA_BRST_L2_ION (spase://NASA/NumericalData/MMS/3/HotPlasmaCompositionAnalyzer/Burst/Level2/Ion/PT0.625S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Start Azimuth [mms3_hpca_start_azimuth]
      
      
      Science Mode Value as defined in the HPCA Science Algorithm Document [mms3_hpca_science_mode]
      
      
      H+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms3_hpca_hplus_data_quality]
      
      
      Hydrogen+ Flux for all Elevation Anodes across all energies [mms3_hpca_hplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_hplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_hplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_hplus_flux_byAnode_atE]
      
      
      Hydrogen+ Phase Space Density for all Elevation Anodes across all energies [mms3_hpca_hplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_hplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anodes [mms3_hpca_hplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_hplus_phase_space_density_byAnode_atE]
      
      
      He+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms3_hpca_heplus_data_quality]
      
      
      Helium+ Flux for all Elevation Anodes across all energies [mms3_hpca_heplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_heplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_heplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_heplus_flux_byAnode_atE]
      
      
      Helium+ Phase Space Density for all Elevation Anodes across all energies [mms3_hpca_heplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_heplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_heplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_heplus_phase_space_density_byAnode_atE]
      
      
      He++ per sweep status (0=bad): see Data_Quality_Key global attribute [mms3_hpca_heplusplus_data_quality]
      
      
      Helium++ Flux for all Elevation Anodes across all energies [mms3_hpca_heplusplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_heplusplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_heplusplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_heplusplus_flux_byAnode_atE]
      
      
      Helium++ Phase Space Density for all Elevation Anodes across all energies [mms3_hpca_heplusplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_heplusplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_heplusplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_heplusplus_phase_space_density_byAnode_atE]
      
      
      O+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms3_hpca_oplus_data_quality]
      
      
      Oxygen+ Flux for all Elevation Anodes across all energies [mms3_hpca_oplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_oplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_oplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_oplus_flux_byAnode_atE]
      
      
      Oxygen+ Phase Space Density for all Elevation Anodes across all energies [mms3_hpca_oplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_oplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_oplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_oplus_phase_space_density_byAnode_atE]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s), Despun MPA-aligned cartesian coordinates [mms3_hpca_B_GSE_sweep_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s), Geocentric Solar Magnetospheric (GSM) cartesian coordinates [mms3_hpca_B_GSM_sweep_avg]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms3_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms3_hpca_TOF_VMON_MIN_converted]
      
      
      Decimation Factor Index from mode config file [mms3_hpca_decimation_factor_index]
      
      
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MMS3_HPCA_BRST_L2_MOMENTS (spase://NASA/NumericalData/MMS/3/HotPlasmaCompositionAnalyzer/Burst/Level2/Moments/PT10S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Number Density Hydrogen+ for each HPCA half-spin [mms3_hpca_hplus_number_density]
      
      
      ---> Ion Bulk Velocity Hydrogen+ for each HPCA half-spin (x, y, z) [mms3_hpca_hplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Hydrogen+ for each HPCA half-spin [mms3_hpca_hplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_hplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_hplus_temperature_tensor]
      
      
      Number Density Helium+ for each HPCA half-spin [mms3_hpca_heplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium+ for each HPCA half-spin (x, y, z) [mms3_hpca_heplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium+ for each HPCA half-spin [mms3_hpca_heplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_heplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_heplus_temperature_tensor]
      
      
      Number Density Helium++ for each HPCA half-spin [mms3_hpca_heplusplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium++ for each HPCA half-spin (x, y, z) [mms3_hpca_heplusplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium++ for each HPCA half-spin [mms3_hpca_heplusplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_heplusplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_heplusplus_temperature_tensor]
      
      
      Number Density Oxygen+ for each HPCA half-spin [mms3_hpca_oplus_number_density]
      
      
      ---> Ion Bulk Velocity Oxygen+ for each HPCA half-spin (x, y, z) [mms3_hpca_oplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Oxygen+ for each HPCA half-spin [mms3_hpca_oplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_oplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_oplus_temperature_tensor]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms3_hpca_B_GSE_spin_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms3_hpca_B_GSM_spin_avg]
      
      
      Bulk Velocity in GSM for H+ for each HPCA half-spin (x, y, z) [mms3_hpca_hplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp H+ for each HPCA half-spin [mms3_hpca_hplus_tperp]
      
      
      ---> Tparallel H+ for each HPCA half-spin [mms3_hpca_hplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_hplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_hplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_hplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_hplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He+ for each HPCA half-spin (x, y, z) [mms3_hpca_heplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He+ for each HPCA half-spin [mms3_hpca_heplus_tperp]
      
      
      ---> Tparallel He+ for each HPCA half-spin [mms3_hpca_heplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He++ for each HPCA half-spin (x, y, z) [mms3_hpca_heplusplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He++ for each HPCA half-spin [mms3_hpca_heplusplus_tperp]
      
      
      ---> Tparallel He++ for each HPCA half-spin [mms3_hpca_heplusplus_tparallel]
      
      
      Vperp vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplusplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplusplus_vparallel]
      
      
      Vperp vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplusplus_vperp_GSM]
      
      
      Vparallel vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplusplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for O+ for each HPCA half-spin (x, y, z) [mms3_hpca_oplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp O+ for each HPCA half-spin [mms3_hpca_oplus_tperp]
      
      
      ---> Tparallel O+ for each HPCA half-spin [mms3_hpca_oplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_oplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_oplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_oplus_vperp_GSM]
      
      
      --->Vparallel vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_oplus_vparallel_GSM]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms3_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms3_hpca_TOF_VMON_MIN_converted]
      
      
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MMS3_HPCA_SRVY_L2_ION (spase://NASA/NumericalData/MMS/3/HotPlasmaCompositionAnalyzer/Survey/Level2/Ion/PT0.625S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Start Azimuth [mms3_hpca_start_azimuth]
      
      
      Science Mode Value as defined in the HPCA Science Algorithm Document [mms3_hpca_science_mode]
      
      
      H+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms3_hpca_hplus_data_quality]
      
      
      Hydrogen+ Flux for all Elevation Anodes across all energies [mms3_hpca_hplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_hplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_hplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_hplus_flux_byAnode_atE]
      
      
      Hydrogen+ Phase Space Density for all Elevation Anodes across all energies [mms3_hpca_hplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_hplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anodes [mms3_hpca_hplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_hplus_phase_space_density_byAnode_atE]
      
      
      He+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms3_hpca_heplus_data_quality]
      
      
      Helium+ Flux for all Elevation Anodes across all energies [mms3_hpca_heplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_heplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_heplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_heplus_flux_byAnode_atE]
      
      
      Helium+ Phase Space Density for all Elevation Anodes across all energies [mms3_hpca_heplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_heplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_heplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_heplus_phase_space_density_byAnode_atE]
      
      
      He++ per sweep status (0=bad): see Data_Quality_Key global attribute [mms3_hpca_heplusplus_data_quality]
      
      
      Helium++ Flux for all Elevation Anodes across all energies [mms3_hpca_heplusplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_heplusplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_heplusplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_heplusplus_flux_byAnode_atE]
      
      
      Helium++ Phase Space Density for all Elevation Anodes across all energies [mms3_hpca_heplusplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_heplusplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_heplusplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_heplusplus_phase_space_density_byAnode_atE]
      
      
      O+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms3_hpca_oplus_data_quality]
      
      
      Oxygen+ Flux for all Elevation Anodes across all energies [mms3_hpca_oplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_oplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_oplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_oplus_flux_byAnode_atE]
      
      
      Oxygen+ Phase Space Density for all Elevation Anodes across all energies [mms3_hpca_oplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms3_hpca_oplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms3_hpca_oplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms3_hpca_oplus_phase_space_density_byAnode_atE]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s), Despun MPA-aligned cartesian coordinates [mms3_hpca_B_GSE_sweep_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s), Geocentric Solar Magnetospheric (GSM) cartesian coordinates [mms3_hpca_B_GSM_sweep_avg]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms3_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms3_hpca_TOF_VMON_MIN_converted]
      
      
      Decimation Factor Index from mode config file [mms3_hpca_decimation_factor_index]
      
      
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MMS3_HPCA_SRVY_L2_MOMENTS (spase://NASA/NumericalData/MMS/3/HotPlasmaCompositionAnalyzer/Survey/Level2/Moments/PT10S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Number Density Hydrogen+ for each HPCA half-spin [mms3_hpca_hplus_number_density]
      
      
      ---> Ion Bulk Velocity Hydrogen+ for each HPCA half-spin (x, y, z) [mms3_hpca_hplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Hydrogen+ for each HPCA half-spin [mms3_hpca_hplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_hplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_hplus_temperature_tensor]
      
      
      Number Density Helium+ for each HPCA half-spin [mms3_hpca_heplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium+ for each HPCA half-spin (x, y, z) [mms3_hpca_heplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium+ for each HPCA half-spin [mms3_hpca_heplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_heplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_heplus_temperature_tensor]
      
      
      Number Density Helium++ for each HPCA half-spin [mms3_hpca_heplusplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium++ for each HPCA half-spin (x, y, z) [mms3_hpca_heplusplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium++ for each HPCA half-spin [mms3_hpca_heplusplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_heplusplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_heplusplus_temperature_tensor]
      
      
      Number Density Oxygen+ for each HPCA half-spin [mms3_hpca_oplus_number_density]
      
      
      ---> Ion Bulk Velocity Oxygen+ for each HPCA half-spin (x, y, z) [mms3_hpca_oplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Oxygen+ for each HPCA half-spin [mms3_hpca_oplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_oplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms3_hpca_oplus_temperature_tensor]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms3_hpca_B_GSE_spin_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms3_hpca_B_GSM_spin_avg]
      
      
      Bulk Velocity in GSM for H+ for each HPCA half-spin (x, y, z) [mms3_hpca_hplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp H+ for each HPCA half-spin [mms3_hpca_hplus_tperp]
      
      
      ---> Tparallel H+ for each HPCA half-spin [mms3_hpca_hplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_hplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_hplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_hplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_hplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He+ for each HPCA half-spin (x, y, z) [mms3_hpca_heplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He+ for each HPCA half-spin [mms3_hpca_heplus_tperp]
      
      
      ---> Tparallel He+ for each HPCA half-spin [mms3_hpca_heplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He++ for each HPCA half-spin (x, y, z) [mms3_hpca_heplusplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He++ for each HPCA half-spin [mms3_hpca_heplusplus_tperp]
      
      
      ---> Tparallel He++ for each HPCA half-spin [mms3_hpca_heplusplus_tparallel]
      
      
      Vperp vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplusplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplusplus_vparallel]
      
      
      Vperp vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplusplus_vperp_GSM]
      
      
      Vparallel vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms3_hpca_heplusplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for O+ for each HPCA half-spin (x, y, z) [mms3_hpca_oplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp O+ for each HPCA half-spin [mms3_hpca_oplus_tperp]
      
      
      ---> Tparallel O+ for each HPCA half-spin [mms3_hpca_oplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_oplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_oplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_oplus_vperp_GSM]
      
      
      --->Vparallel vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms3_hpca_oplus_vparallel_GSM]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms3_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms3_hpca_TOF_VMON_MIN_converted]
      
      
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MMS3_HPCA_SRVY_L2_TOF-COUNTS (spase://NASA/NumericalData/MMS/3/HotPlasmaCompositionAnalyzer/Survey/Level2/TimeOfFlight/Counts/PT0.625S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      TOF Counts for all angles, across all energies [mms3_hpca_tof_counts]
      
      
      ---> Spectrograms all angles, at selected energies [mms3_hpca_tof_counts_allA_atE]
      
      
      ---> Spectrograms at select angles, for all energies [mms3_hpca_tof_counts_allE_atA]
      
      
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MMS3_MEC_BRST_L2_EPHT89D (spase://NASA/NumericalData/MMS/3/Ephemeris/Burst/Level2/Tsyganenko_89_Dynamic/PT0.030S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms3_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms3_mec_gmst]
      
      
      Magnetic Latitude. [mms3_mec_mlat]
      
      
      Magnetic Local Time. [mms3_mec_mlt]
      
      
      Dipole L-shell value. [mms3_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms3_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms3_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms3_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms3_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms3_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms3_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms3_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms3_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms3_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms3_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms3 (km) [mms3_mec_r_eci]
      
      
      Velocity of mms3 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms3_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms3 (km) [mms3_mec_r_gsm]
      
      
      Velocity of mms3 spacecraft in GSM coordinates (km/s) [mms3_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms3 (km) [mms3_mec_r_geo]
      
      
      Velocity of mms3 spacecraft in GEO coordinates (km/s) [mms3_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms3 (km) [mms3_mec_r_sm]
      
      
      Velocity of mms3 spacecraft in SM coordinates (km/s) [mms3_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms3 (km) [mms3_mec_r_gse]
      
      
      Velocity of mms3 spacecraft in GSE coordinates (km/s) [mms3_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms3 (km) [mms3_mec_r_gse2000]
      
      
      Velocity of mms3 spacecraft in GSE2000 coordinates (km/s) [mms3_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms3 spacecraft [mms3_mec_geod_lat]
      
      
      Geodetic longitude of mms3 spacecraft [mms3_mec_geod_lon]
      
      
      Geodetic height of mms3 spacecraft. (Height above WGS84 Spheroid.) [mms3_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms3_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms3_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms3_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms3 spacecraft [mms3_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms3_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms3_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms3 spacecraft [mms3_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms3 spacecraft [mms3_mec_bmin_gsm]
      
      
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MMS3_MEC_BRST_L2_EPHT89Q (spase://NASA/NumericalData/MMS/3/Ephemeris/Burst/Level2/Tsyganenko_89_Quiet/PT0.030S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms3_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms3_mec_gmst]
      
      
      Magnetic Latitude. [mms3_mec_mlat]
      
      
      Magnetic Local Time. [mms3_mec_mlt]
      
      
      Dipole L-shell value. [mms3_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms3_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms3_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms3_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms3_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms3_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms3_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms3_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms3_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms3_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms3_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms3 (km) [mms3_mec_r_eci]
      
      
      Velocity of mms3 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms3_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms3 (km) [mms3_mec_r_gsm]
      
      
      Velocity of mms3 spacecraft in GSM coordinates (km/s) [mms3_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms3 (km) [mms3_mec_r_geo]
      
      
      Velocity of mms3 spacecraft in GEO coordinates (km/s) [mms3_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms3 (km) [mms3_mec_r_sm]
      
      
      Velocity of mms3 spacecraft in SM coordinates (km/s) [mms3_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms3 (km) [mms3_mec_r_gse]
      
      
      Velocity of mms3 spacecraft in GSE coordinates (km/s) [mms3_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms3 (km) [mms3_mec_r_gse2000]
      
      
      Velocity of mms3 spacecraft in GSE2000 coordinates (km/s) [mms3_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms3 spacecraft [mms3_mec_geod_lat]
      
      
      Geodetic longitude of mms3 spacecraft [mms3_mec_geod_lon]
      
      
      Geodetic height of mms3 spacecraft. (Height above WGS84 Spheroid.) [mms3_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms3_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms3_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms3_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms3 spacecraft [mms3_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms3_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms3_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms3 spacecraft [mms3_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms3 spacecraft [mms3_mec_bmin_gsm]
      
      
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MMS3_MEC_BRST_L2_EPHTS04D (spase://NASA/NumericalData/MMS/3/Ephemeris/Burst/Level2/Tsyganenko_04_Dynamic/PT0.030S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms3_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms3_mec_gmst]
      
      
      Magnetic Latitude. [mms3_mec_mlat]
      
      
      Magnetic Local Time. [mms3_mec_mlt]
      
      
      Dipole L-shell value. [mms3_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms3_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms3_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms3_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms3_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms3_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms3_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms3_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms3_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms3_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms3_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms3 (km) [mms3_mec_r_eci]
      
      
      Velocity of mms3 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms3_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms3 (km) [mms3_mec_r_gsm]
      
      
      Velocity of mms3 spacecraft in GSM coordinates (km/s) [mms3_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms3 (km) [mms3_mec_r_geo]
      
      
      Velocity of mms3 spacecraft in GEO coordinates (km/s) [mms3_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms3 (km) [mms3_mec_r_sm]
      
      
      Velocity of mms3 spacecraft in SM coordinates (km/s) [mms3_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms3 (km) [mms3_mec_r_gse]
      
      
      Velocity of mms3 spacecraft in GSE coordinates (km/s) [mms3_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms3 (km) [mms3_mec_r_gse2000]
      
      
      Velocity of mms3 spacecraft in GSE2000 coordinates (km/s) [mms3_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms3 spacecraft [mms3_mec_geod_lat]
      
      
      Geodetic longitude of mms3 spacecraft [mms3_mec_geod_lon]
      
      
      Geodetic height of mms3 spacecraft. (Height above WGS84 Spheroid.) [mms3_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms3_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms3_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms3_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms3 spacecraft [mms3_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms3_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms3_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms3 spacecraft [mms3_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms3 spacecraft [mms3_mec_bmin_gsm]
      
      
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MMS3_MEC_SRVY_L2_EPHT89D (spase://NASA/NumericalData/MMS/3/Ephemeris/Survey/Level2/Tsyganenko_89_Dynamic/PT30S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms3_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms3_mec_gmst]
      
      
      Magnetic Latitude. [mms3_mec_mlat]
      
      
      Magnetic Local Time. [mms3_mec_mlt]
      
      
      Dipole L-shell value. [mms3_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms3_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms3_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms3_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms3_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms3_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms3_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms3_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms3_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms3_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms3_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms3 (km) [mms3_mec_r_eci]
      
      
      Velocity of mms3 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms3_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms3 (km) [mms3_mec_r_gsm]
      
      
      Velocity of mms3 spacecraft in GSM coordinates (km/s) [mms3_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms3 (km) [mms3_mec_r_geo]
      
      
      Velocity of mms3 spacecraft in GEO coordinates (km/s) [mms3_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms3 (km) [mms3_mec_r_sm]
      
      
      Velocity of mms3 spacecraft in SM coordinates (km/s) [mms3_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms3 (km) [mms3_mec_r_gse]
      
      
      Velocity of mms3 spacecraft in GSE coordinates (km/s) [mms3_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms3 (km) [mms3_mec_r_gse2000]
      
      
      Velocity of mms3 spacecraft in GSE2000 coordinates (km/s) [mms3_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms3 spacecraft [mms3_mec_geod_lat]
      
      
      Geodetic longitude of mms3 spacecraft [mms3_mec_geod_lon]
      
      
      Geodetic height of mms3 spacecraft. (Height above WGS84 Spheroid.) [mms3_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms3_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms3_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms3_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms3 spacecraft [mms3_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms3_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms3_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms3 spacecraft [mms3_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms3 spacecraft [mms3_mec_bmin_gsm]
      
      
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MMS3_MEC_SRVY_L2_EPHT89Q (spase://NASA/NumericalData/MMS/3/Ephemeris/Survey/Level2/Tsyganenko_89_Quiet/PT30S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms3_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms3_mec_gmst]
      
      
      Magnetic Latitude. [mms3_mec_mlat]
      
      
      Magnetic Local Time. [mms3_mec_mlt]
      
      
      Dipole L-shell value. [mms3_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms3_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms3_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms3_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms3_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms3_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms3_mec_P_phase]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms3_mec_ang_mom_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms3_mec_ang_mom_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms3_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms3_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms3_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms3_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms3 (km) [mms3_mec_r_eci]
      
      
      Velocity of mms3 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms3_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms3 (km) [mms3_mec_r_gsm]
      
      
      Velocity of mms3 spacecraft in GSM coordinates (km/s) [mms3_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms3 (km) [mms3_mec_r_geo]
      
      
      Velocity of mms3 spacecraft in GEO coordinates (km/s) [mms3_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms3 (km) [mms3_mec_r_sm]
      
      
      Velocity of mms3 spacecraft in SM coordinates (km/s) [mms3_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms3 (km) [mms3_mec_r_gse]
      
      
      Velocity of mms3 spacecraft in GSE coordinates (km/s) [mms3_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms3 (km) [mms3_mec_r_gse2000]
      
      
      Velocity of mms3 spacecraft in GSE2000 coordinates (km/s) [mms3_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms3 spacecraft [mms3_mec_geod_lat]
      
      
      Geodetic longitude of mms3 spacecraft [mms3_mec_geod_lon]
      
      
      Geodetic height of mms3 spacecraft. (Height above WGS84 Spheroid.) [mms3_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms3_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms3_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms3_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms3 spacecraft [mms3_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms3_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms3_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms3 spacecraft [mms3_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms3 spacecraft [mms3_mec_bmin_gsm]
      
      
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MMS3_MEC_SRVY_L2_EPHTS04D (spase://NASA/NumericalData/MMS/3/Ephemeris/Survey/Level2/Tsyganenko_04_Dynamic/PT30S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms3_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms3_mec_gmst]
      
      
      Magnetic Latitude. [mms3_mec_mlat]
      
      
      Magnetic Local Time. [mms3_mec_mlt]
      
      
      Dipole L-shell value. [mms3_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms3_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms3_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms3_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms3_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms3_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms3_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms3_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms3_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms3_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms3_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms3 (km) [mms3_mec_r_eci]
      
      
      Velocity of mms3 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms3_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms3 (km) [mms3_mec_r_gsm]
      
      
      Velocity of mms3 spacecraft in GSM coordinates (km/s) [mms3_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms3 (km) [mms3_mec_r_geo]
      
      
      Velocity of mms3 spacecraft in GEO coordinates (km/s) [mms3_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms3 (km) [mms3_mec_r_sm]
      
      
      Velocity of mms3 spacecraft in SM coordinates (km/s) [mms3_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms3 (km) [mms3_mec_r_gse]
      
      
      Velocity of mms3 spacecraft in GSE coordinates (km/s) [mms3_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms3 (km) [mms3_mec_r_gse2000]
      
      
      Velocity of mms3 spacecraft in GSE2000 coordinates (km/s) [mms3_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms3_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms3 spacecraft [mms3_mec_geod_lat]
      
      
      Geodetic longitude of mms3 spacecraft [mms3_mec_geod_lon]
      
      
      Geodetic height of mms3 spacecraft. (Height above WGS84 Spheroid.) [mms3_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms3_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms3_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms3_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms3 spacecraft [mms3_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms3_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms3_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms3 spacecraft [mms3_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms3 spacecraft [mms3_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms3 spacecraft [mms3_mec_bmin_gsm]
      
      
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MMS3_R0_SUMMARY
Description
Pre-generated MMS Quicklook Summary Plots
File location: https://cdaweb.gsfc.nasa.gov/pub/data/mms/ql_plots/all_mms3_summ 
 
  • Data Variable Descriptions
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MMS3_SCM_BRST_L2_SCB (spase://NASA/NumericalData/MMS/3/FIELDS/SCM/Burst/Level2/PT0.0001220703125S)
Description
The tri-axial search-coil magnetometer (SCM) with its associated preamplifier
provides the three-dimensional measurement of the magnetic field fluctuations.
The analog magnetic waveforms measured by the SCM are digitized and processed
inside the digital signal processor (DSP), collected and stored by the central
instrument data processor (CIDP) via the Fields central electronics box (CEB).
Prior to launch, all SCM Flight models were calibrated by LPP at the National
Magnetic Observatory at Chambon-la-Foret (Orleans). Once per orbit, each SCM
transfer function is checked thanks to the onboard calibration signal provided
by DSP. SCM is operated for the entire MMS orbit in survey mode. Within the ROI,
burst mode data are also acquired as well as high burst mode data. 
SCM data set corresponds to the AC magnetic field waveforms in nanoTesla and in
the GSE frame.
The instrument paper for SCM can be found at
https://urldefense.proofpoint.com/v2/url?u=http-3A__link.springer.com_article_10
.1007_s11214-2D014-2D0096-2D9&d=DwIFAg&c=c6MrceVCY5m5A_KAUkrdoA&r=bjziExGTRYoZgE
2xb_dDSm9NxNIo0lG6Q-rB0Y6rHS4&m=CMzo0Vv9zPtWSdbdY1Wq9-jIkYS2cOMV9JYZsMV10y0&s=Xb
P9PiEAswHGl5lqgsDVI6zs8ivJx7yek9i2undKl10&e= 
Modification History
unpack telemetry, assign sample times
2026-07-10T20:11:42.00002789497058Z - [L1A->L1B (step 1/1)] Calibration
(TMcounts->nT). See CALIBRATION_PARAMETERS for details.
2026-07-16T12:36:48.00005346536624Z - [L1B->L2 (step 1/2)] Coordinate transform
(SCM123->GSE). See COORD_TRANS_PARAMETERS for details.
2026-07-16T12:36:54.00006115436542Z - [L1B->L2 (step 2/2)] Frequency filtering.
See FREQUENCY_FILTER for details.
 
  • Data Variable Descriptions
      L2 AC magnetic field in GSE frame [mms3_scm_acb_gse_scb_brst_l2]
      These calibrated (nT) AC magnetic field waveform data are sampled at 8192S/s.
      They are high-pass filtered above 1.00Hz but not low-pass filtered. See global
      attributes for details. For more information, please have a look at the SCM Data
      Products Guide.
      
      (List/Create Only) Quality Factor (one letter per antenna, G=good) [mms3_scm_qf_scm123_scb_brst_l2]
      Each letter refers to one SCM physical antenna in the SCM123 order. 'G' stands
      for good data, 'Z' for data that are affected or set to zero by convolution
      boundary effect, 'S' for saturated data, 'X' for out of range data, 'B' for
      fillvalue/bad data.
      
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MMS3_SCM_BRST_L2_SCHB (spase://NASA/NumericalData/MMS/3/FIELDS/SCM/Burst/Level2/PT0.00006101515625S)
Description
The tri-axial search-coil magnetometer (SCM) with its associated preamplifier
provides the three-dimensional measurement of the magnetic field fluctuations.
The analog magnetic waveforms measured by the SCM are digitized and processed
inside the digital signal processor (DSP), collected and stored by the central
instrument data processor (CIDP) via the Fields central electronics box (CEB).
Prior to launch, all SCM Flight models were calibrated by LPP at the National
Magnetic Observatory at Chambon-la-Foret (Orleans). Once per orbit, each SCM
transfer function is checked thanks to the onboard calibration signal provided
by DSP. SCM is operated for the entire MMS orbit in survey mode. Within the ROI,
burst mode data are also acquired as well as high burst mode data. 
SCM data set corresponds to the AC magnetic field waveforms in nanoTesla and in
the GSE frame.
The instrument paper for SCM can be found at
http://link.springer.com/article/10.1007/s11214-014-0096-9
Modification History
unpack telemetry, assign sample times
2026-07-10T20:12:07.0000532269446Z - [L1A->L1B (step 1/1)] Calibration
(TMcounts->nT). See CALIBRATION_PARAMETERS for details.
2026-07-16T12:41:22.00005590915685Z - [L1B->L2 (step 1/2)] Coordinate transform
(SCM123->GSE). See COORD_TRANS_PARAMETERS for details.
2026-07-16T12:41:26.00003421306615Z - [L1B->L2 (step 2/2)] Frequency filtering.
See FREQUENCY_FILTER for details.
 
  • Data Variable Descriptions
      L2 AC magnetic field in GSE frame [mms3_scm_acb_gse_schb_brst_l2]
      These calibrated (nT) AC magnetic field waveform data are sampled at 16384S/s.
      They are high-pass filtered above 32.00Hz but not low-pass filtered. See global
      attributes for details. For more information, please have a look at the SCM Data
      Products Guide
      (https://lasp.colorado.edu/mms/sdc/public/datasets/fields/Science_Data_Products_ 
      Guide_vol2_SCM_v11_20160301.pdf).
      
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MMS3_SCM_SRVY_L2_SCSRVY (spase://NASA/NumericalData/MMS/3/FIELDS/SCM/Survey/Level2/PT0.03125S)
Description
The tri-axial search-coil magnetometer (SCM) with its associated preamplifier
provides the three-dimensional measurement of the magnetic field fluctuations.
The analog magnetic waveforms measured by the SCM are digitized and processed
inside the digital signal processor (DSP), collected and stored by the central
instrument data processor (CIDP) via the Fields central electronics box (CEB).
Prior to launch, all SCM Flight models were calibrated by LPP at the National
Magnetic Observatory at Chambon-la-Foret (Orleans). Once per orbit, each SCM
transfer function is checked thanks to the onboard calibration signal provided
by DSP. SCM is operated for the entire MMS orbit in survey mode. Within the ROI,
burst mode data are also acquired as well as high burst mode data. 
SCM data set corresponds to the AC magnetic field waveforms in nanoTesla and in
the GSE frame.
The instrument paper for SCM can be found at
http://link.springer.com/article/10.1007/s11214-014-0096-9
Modification History
unpack telemetry, assign sample times
2026-07-02T23:58:23.00004333257333Z - [L1A->L1B (step 1/1)] Calibration
(TMcounts->nT). See CALIBRATION_PARAMETERS for details.
2026-07-15T23:56:24.0000450611082Z - [L1B->L2 (step 1/2)] Coordinate transform
(SCM123->GSE). See COORD_TRANS_PARAMETERS for details.
2026-07-15T23:57:09.0000423788994Z - [L1B->L2 (step 2/2)] Frequency filtering.
See FREQUENCY_FILTER for details.
 
  • Data Variable Descriptions
      L2 AC magnetic field in GSE frame [mms3_scm_acb_gse_scsrvy_srvy_l2]
      These calibrated (nT) AC magnetic field waveform data are sampled at 32S/s. They
      are high-pass filtered above 0.50Hz but not low-pass filtered. See global
      attributes for details. For more information, please have a look at the SCM Data
      Products Guide
      (https://lasp.colorado.edu/mms/sdc/public/datasets/fields/Science_Data_Products_ 
      Guide_vol2_SCM_v11_20160301.pdf).
      
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MMS4_ASPOC_SRVY_L2 (spase://NASA/NumericalData/MMS/4/ASPOC/Survey/Level2/PT1S)
Description
K. Torkar et al, Active Spacecraft Potential Control Investigation
Space Science Reviews, 2014, DOI: 10.1007/s11214-014-0049-3
Further information:
- http://www.iwf.oeaw.ac.at/en/research/near-earth-space/mms/ 
- http://mms.space.swri.edu/ 
Modification History
150224 Initial version
150831 Minor updates and fixes
160205 CDF file format guide compliant
 
  • Data Variable Descriptions
      ASPOC Ion Emission Current Sum, 1s resolution [mms4_aspoc_ionc]
      
      
      ASPOC Unit 1 Ion Emission Current, 1s resolution [mms4_asp1_ionc]
      
      
      ASPOC Unit 2 Ion Emission Current, 1s resolution [mms4_asp2_ionc]
      
      
      ASPOC Unit 1 Emitted Beam Energy, 1s resolution [mms4_asp1_energy]
      
      
      ASPOC Unit 2 Emitted Beam Energy, 1s resolution [mms4_asp2_energy]
      
      
      ASPOC Data Quality and Instrument Status, 1s resolution [mms4_aspoc_status]
      
      
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MMS4_DSP_FAST_L2_BPSD (spase://NASA/NumericalData/MMS/4/FIELDS/DSP/Fast/Level2/MagneticFieldPowerSpectralDensity/PT2S)
Description
BPSD is the low frequency B spectral density covering the frequency range of .2
to 6000 Hz.
 
  • Data Variable Descriptions
      SCM Axis 1 (X) component magnetic power spectral density [mms4_dsp_bpsd_scm1_fast_l2]
      
      
      SCM Axis 2 (Y, ~direction of S/C Z) component magnetic power spectral density [mms4_dsp_bpsd_scm2_fast_l2]
      
      
      SCM Axis 3 (Z) component magnetic power spectral density [mms4_dsp_bpsd_scm3_fast_l2]
      
      
      Omni-directional magnetic power spectral density: square root of the sum of the squares of 3 components [mms4_dsp_bpsd_omni_fast_l2]
      
      
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MMS4_DSP_FAST_L2_EPSD (spase://NASA/NumericalData/MMS/4/FIELDS/DSP/Fast/Level2/ElectricFieldPowerSpectralDensity/PT2S)
Description
EPSD combines the low frequency E spectral density covering the frequency range
of 1 to 8000 Hz and the  medium frequency E spectral density covering the
frequency range of .25 to 100 kHz.
 
  • Data Variable Descriptions
      null [mms4_dsp_epsd_x]
      
      
      null [mms4_dsp_epsd_y]
      
      
      null [mms4_dsp_epsd_z]
      
      
      null [mms4_dsp_epsd_omni]
      
      
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MMS4_DSP_SLOW_L2_BPSD (spase://NASA/NumericalData/MMS/4/FIELDS/DSP/Slow/Level2/MagneticFieldPowerSpectralDensity/PT16S)
Description
search coil magnetometer spectral density
 
  • Data Variable Descriptions
      SCM1 component magnetic power spectral density [mms4_dsp_bpsd_scm1_slow_l2]
      
      
      SCM2 component magnetic power spectral density - NO DATA in Slow Survey [mms4_dsp_bpsd_scm2_slow_l2]
      
      
      SCM3 component magnetic power spectral density [mms4_dsp_bpsd_scm3_slow_l2]
      
      
      Omni-directional magnetic power spectral density: square root of the sum of the squares of 2 components [mms4_dsp_bpsd_omni_slow_l2]
      
      
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MMS4_DSP_SLOW_L2_EPSD (spase://NASA/NumericalData/MMS/4/FIELDS/DSP/Slow/Level2/ElectricFieldPowerSpectralDensity/PT16S)
Description
electric spectral density
 
  • Data Variable Descriptions
      null [mms4_dsp_epsd_x]
      
      
      null [mms4_dsp_epsd_y]
      
      
      null [mms4_dsp_epsd_z]
      
      
      null [mms4_dsp_epsd_omni]
      
      
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MMS4_EDI_BRST_L2_AMB (spase://NASA/NumericalData/MMS/4/FIELDS/EDI/Burst/Level2/ElectronFluxAmbient/ProjectionMethod1/PT0.0009765625S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - Original version.
v1.0.0 - Include trajectory vectors and optics state.
v1.1.0 - Update metadata: counts -> flux.
v1.2.0 - Added flux error.
v1.3.0 - Trajectory vector errors are now deltas.
v1.4.0 - Fixed dead-time correction and error values.
v1.5.0 - Factor of 2 for accumulation time & 2 for abscal factor in srvy mode.
v1.6.0 - No factor of 2 for accumulation time in srvy mode.
v2.0.0 - Reduced file size with scalar errors. Update metadata.
v2.1.0 - Correct fill value for fluxes.
v3.0.0 - Omni-directional error for trajectories. Y-Version linked to cal file.
Single epoch for counts.
v4.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
 
  • Data Variable Descriptions
      Optics state [mms4_edi_optics_state_brst_l2]
      
      
      ---> GDU1 energy [mms4_edi_energy_gdu1_brst_l2]
      
      
      ---> GDU2 energy [mms4_edi_energy_gdu2_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-1 0PA [mms4_edi_flux1_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-1 0PA [mms4_edi_flux1_0_brst_l2_noerr]
      
      
      ---> Error for flux1 0-degree pitch angle electron flux. [mms4_edi_flux1_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-2 0PA [mms4_edi_flux2_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-2 0PA [mms4_edi_flux2_0_brst_l2_noerr]
      
      
      ---> Error for flux2 0-degree pitch angle electron flux. [mms4_edi_flux2_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-3 0PA [mms4_edi_flux3_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-3 0PA [mms4_edi_flux3_0_brst_l2_noerr]
      
      
      ---> Error for flux3 0-degree pitch angle electron flux. [mms4_edi_flux3_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-4 0PA [mms4_edi_flux4_0_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-4 0PA [mms4_edi_flux4_0_brst_l2_noerr]
      
      
      ---> Error for flux4 0-degree pitch angle electron flux. [mms4_edi_flux4_0_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by Traj-1 180PA [mms4_edi_flux1_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-1 180PA [mms4_edi_flux1_180_brst_l2_noerr]
      
      
      ---> Error for flux1 180-degree pitch angle electron flux. [mms4_edi_flux1_180_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by traj2 180PA [mms4_edi_flux2_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-2 180PA [mms4_edi_flux2_180_brst_l2_noerr]
      
      
      ---> Error for flux2 180-degree pitch angle electron flux. [mms4_edi_flux2_180_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by traj3 180PA [mms4_edi_flux3_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-3 180PA [mms4_edi_flux3_180_brst_l2_noerr]
      
      
      ---> Error for flux3 180-degree pitch angle electron flux. [mms4_edi_flux3_180_delta_brst_l2]
      
      
      Flux for electrons with trajectories given by traj4 180PA [mms4_edi_flux4_180_brst_l2]
      
      
      ---> (no error bars displayed) Flux for electrons with trajectories given by Traj-4 180PA [mms4_edi_flux4_180_brst_l2_noerr]
      
      
      ---> Error for flux4 180-degree pitch angle electron flux. [mms4_edi_flux4_180_delta_brst_l2]
      
      
      Trajectory of flux1 0-degree pitch angle electrons in GSE coordinates. [mms4_edi_traj1_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 0-degree pitch angle electrons in GSE coordinates. [mms4_edi_traj2_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 0-degree pitch angle electrons in GSE coordinates. [mms4_edi_traj3_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 0-degree pitch angle electrons in GSE coordinates. [mms4_edi_traj4_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of flux1 180-degree pitch angle electrons in GSE coordinates. [mms4_edi_traj1_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 180-degree pitch angle electrons in GSE coordinates. [mms4_edi_traj2_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 180-degree pitch angle electrons in GSE coordinates. [mms4_edi_traj3_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 180-degree pitch angle electrons in GSE coordinates. [mms4_edi_traj4_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj1_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 0-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj2_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 0-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj3_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 0-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj4_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj1_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux2 180-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj2_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux3 180-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj3_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      ---> Trajectory of flux4 180-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj4_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms4_edi_traj1_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms4_edi_traj2_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms4_edi_traj3_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms4_edi_traj4_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms4_edi_traj1_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms4_edi_traj2_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms4_edi_traj3_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms4_edi_traj4_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS4_EDI_BRST_L2_AMB-PM2 (spase://NASA/NumericalData/MMS/4/FIELDS/EDI/Burst/Level2/AmbientElectronFlux/ProjectionMethod2/PT0.0009765625S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v1.0.0 - Original version.
v1.1.0 - Correct fill value for fluxes.
v2.0.0 - Omni-directional error for trajectories. Y-Version linked to cal file.
Single epoch for counts.
v3.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
v4.0.0 - Each trajectory has its own LABL_PTR_1 variable.
 
  • Data Variable Descriptions
      Optics state [mms4_edi_optics_state_brst_l2]
      
      
      ---> GDU1 energy [mms4_edi_energy_gdu1_brst_l2]
      
      
      ---> GDU2 energy [mms4_edi_energy_gdu2_brst_l2]
      
      
      Field-aligned electron flux from channel 1 of both GDUs [mms4_edi_flux1_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 1 of both GDUs [mms4_edi_flux1_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 1 of both GDUs. [mms4_edi_flux1_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 1 of both GDUs [mms4_edi_flux1_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 1 of both GDUs [mms4_edi_flux1_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 1 of both GDUs. [mms4_edi_flux1_180_delta_brst_l2]
      
      
      Field-aligned electron flux from channel 2 of both GDUs [mms4_edi_flux2_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 2 of both GDUs [mms4_edi_flux2_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 2 of both GDUs. [mms4_edi_flux2_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 2 of both GDUs [mms4_edi_flux2_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 2 of both GDUs [mms4_edi_flux2_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 2 of both GDUs. [mms4_edi_flux2_180_delta_brst_l2]
      
      
      Field-aligned electron flux from channel 3 of both GDUs [mms4_edi_flux3_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 3 of both GDUs [mms4_edi_flux3_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 3 of both GDUs. [mms4_edi_flux3_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 3 of both GDUs [mms4_edi_flux3_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 3 of both GDUs [mms4_edi_flux3_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 3 of both GDUs. [mms4_edi_flux3_180_delta_brst_l2]
      
      
      Field-aligned electron flux from channel 4 of both GDUs [mms4_edi_flux4_0_brst_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from channel 4 of both GDUs [mms4_edi_flux4_0_brst_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from channel 4 of both GDUs. [mms4_edi_flux4_0_delta_brst_l2]
      
      
      Anti-field-aligned electron flux from channel 4 of both GDUs [mms4_edi_flux4_180_brst_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from channel 4 of both GDUs [mms4_edi_flux4_180_brst_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from channel 4 of both GDUs. [mms4_edi_flux4_180_delta_brst_l2]
      
      
      Trajectory of field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms4_edi_traj1_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 1 of both GDUs in DBCS coordinates. [mms4_edi_traj1_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 1 of both GDUs in GSE coordinates. [mms4_edi_traj1_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 1 of both GDUs, in GSE coordinates. [mms4_edi_traj1_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms4_edi_traj2_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 2 of both GDUs in DBCS coordinates. [mms4_edi_traj2_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 2 of both GDUs in GSE coordinates. [mms4_edi_traj2_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 2 of both GDUs, in GSE coordinates. [mms4_edi_traj2_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms4_edi_traj3_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 3 of both GDUs in DBCS coordinates. [mms4_edi_traj3_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 3 of both GDUs in GSE coordinates. [mms4_edi_traj3_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 3 of both GDUs, in GSE coordinates. [mms4_edi_traj3_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms4_edi_traj4_dbcs_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 4 of both GDUs in DBCS coordinates. [mms4_edi_traj4_dbcs_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from channel 4 of both GDUs in GSE coordinates. [mms4_edi_traj4_gse_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from channel 4 of both GDUs, in GSE coordinates. [mms4_edi_traj4_gse_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj1_gsm_0_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj1_gsm_180_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS4_EDI_BRST_L2_EFIELD (spase://NASA/NumericalData/MMS/4/FIELDS/EDI/Burst/Level2/ElectricField/PT0.0009765625S)
Description
EDI electric field data. Instrument papers for EDI can be found at:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7
Modification History
v1.0.0 - First version. TRI-TOF selection based on smallest error.
v1.1.0 - TRI-TOF merged by weighted average.
v1.2.0 - Fixed t_delta_plus/minus CDF_type.
v1.3.0 - Fixed Fixed vdrift SI conversion.
v1.4.0 - Fixed data duplication caused by multiple l2pre file locations.
v1.5.0 - Inplemented baseline*beams*Bmag filter for triangulation.
v1.6.0 - Inplemented null files for no or low quality data.
 
  • Data Variable Descriptions
      ExB drift velocity in DSL coordinates. [mms4_edi_vdrift_dsl_brst_l2]
      
      
      ---> ExB drift velocity in DSL coordinates (no error bars) [mms4_edi_vdrift_dsl_brst_l2_noerr]
      
      
      ExB drift velocity in GSE coordinates. [mms4_edi_vdrift_gse_brst_l2]
      
      
      ---> ExB drift velocity in GSE coordinates (no error bars) [mms4_edi_vdrift_gse_brst_l2_noerr]
      
      
      ExB drift velocity in GSM coordinates. [mms4_edi_vdrift_gsm_brst_l2]
      
      
      ---> ExB drift velocity in GSM coordinates (no error bars) [mms4_edi_vdrift_gsm_brst_l2_noerr]
      
      
      Electric field in DSL coordinates. [mms4_edi_e_dsl_brst_l2]
      
      
      ---> Electric field in DSL coordinates (no error bars) [mms4_edi_e_dsl_brst_l2_noerr]
      
      
      Electric field in GSE coordinates. [mms4_edi_e_gse_brst_l2]
      
      
      ---> Electric field in GSE coordinates (no error bars) [mms4_edi_e_gse_brst_l2_noerr]
      
      
      Electric field in GSM coordinates. [mms4_edi_e_gsm_brst_l2]
      
      
      ---> Electric field in GSM coordinates (no error bars) [mms4_edi_e_gsm_brst_l2_noerr]
      
      
      Weighted use of TRI method in L2 results. [mms4_edi_tri_weight_brst_l2]
      
      
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MMS4_EDI_BRST_L2_Q0 (spase://NASA/NumericalData/MMS/4/FIELDS/EDI/Burst/Level2/QualityZero/PT0.0078125S)
Description
EDI Q0 data. The EDI instrument paper and data products guidescan be found at
the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - First version.
v0.0.1 - Filled energy variables.
v0.0.2 - Energy written properly.
v1.0.0 - Update variable names.
v1.1.0 - Added optics state.
v2.0.0 - Added electron trajectories.
v2.1.0 - Deltas on trajectory vectors are now deltas.
v3.0.0 - Reduced file size with scalar errors. Add VAR_NOTES.
v3.1.0 - Fixed optics datatype.
v4.0.0 - Removed unused Epoch variable.
v5.0.0 - Trajectories are provided in DBCS coordinates.
 
  • Data Variable Descriptions
      Optics state [mms4_edi_optics_state_brst_l2]
      
      
      ---> GDU1 energy [mms4_edi_energy_gdu1_brst_l2]
      
      
      ---> GDU2 energy [mms4_edi_energy_gdu2_brst_l2]
      
      
      GDU1 quality 0 counts. [mms4_edi_counts_gdu1_brst_l2]
      Q0 data consists of raw electron counts. The error at any one time is the
      square-root of the counts. Note that there may be contamination from the EDI
      electron beams. See the data products guide or contact an EDI team member to
      learn about beam contamination.
      
      GDU2 quality 0 counts. [mms4_edi_counts_gdu2_brst_l2]
      
      
      GDU1 electron incident trajectory vectors in spherical BCS coordinates. [mms4_edi_traj_bcs_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical BCS coordinates. [mms4_edi_traj_bcs_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical DBCS coordinates. [mms4_edi_traj_dbcs_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical DBCS coordinates. [mms4_edi_traj_dbcs_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSE coordinates. [mms4_edi_traj_gse_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSE coordinates. [mms4_edi_traj_gse_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSM coordinates. [mms4_edi_traj_gsm_gdu1_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSM coordinates. [mms4_edi_traj_gsm_gdu2_brst_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS4_EDI_SRVY_L2_AMB (spase://NASA/NumericalData/MMS/4/FIELDS/EDI/Survey/Level2/ElectronFluxAmbient/ProjectionMethod1/PT0.03125S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - Original version.
v1.0.0 - Include trajectory vectors and optics state.
v1.1.0 - Update metadata: counts -> flux.
v1.2.0 - Added flux error.
v1.3.0 - Trajectory vector errors are now deltas.
v1.4.0 - Fixed dead-time correction and error values.
v1.5.0 - Factor of 2 for accumulation time & 2 for abscal factor in srvy mode.
v1.6.0 - No factor of 2 for accumulation time in srvy mode.
v2.0.0 - Reduced file size with scalar errors. Update metadata.
v2.1.0 - Correct fill value for fluxes.
v3.0.0 - Omni-directional error for trajectories. Correct time deltas. Y-Version
linked to cal file. Single epoch for counts.
v4.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
 
  • Data Variable Descriptions
      Optics state [mms4_edi_optics_state_srvy_l2]
      
      
      ---> GDU1 energy [mms4_edi_energy_gdu1_srvy_l2]
      
      
      ---> GDU2 energy [mms4_edi_energy_gdu2_srvy_l2]
      
      
      Field-aligned electron flux from both GDUs [mms4_edi_flux1_0_srvy_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from both GDUs [mms4_edi_flux1_0_srvy_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from both GDUs. [mms4_edi_flux1_0_delta_srvy_l2]
      
      
      Anti-field-aligned electron flux from both GDUs [mms4_edi_flux1_180_srvy_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from both GDUs [mms4_edi_flux1_180_srvy_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from both GDUs. [mms4_edi_flux1_180_delta_srvy_l2]
      
      
      Trajectory of field-aligned electrons from both GDUs in DBCS coordinates. [mms4_edi_traj1_dbcs_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs in DBCS coordinates. [mms4_edi_traj1_dbcs_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from both GDUs in GSE coordinates. [mms4_edi_traj1_gse_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs, in GSE coordinates. [mms4_edi_traj1_gse_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj1_gsm_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj1_gsm_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS4_EDI_SRVY_L2_AMB-PM2 (spase://NASA/NumericalData/MMS/4/FIELDS/EDI/Survey/Level2/ElectronFluxAmbient/ProjectionMethod2/PT0.03125S)
Description
EDI ambient data. The EDI instrument paper and data products guide can be found
at the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v1.0.0 - Original version.
v1.1.0 - Correct fill value for fluxes.
v2.0.0 - Omni-directional error for trajectories. Y-Version linked to cal file.
Single epoch for counts.
v3.0.0 - Replace data in GSM coordinates with data in DBCS to be consistent with
other particle instruments.
v4.0.0 - Each trajectory has its own LABL_PTR_1 variable.
 
  • Data Variable Descriptions
      Optics state [mms4_edi_optics_state_srvy_l2]
      
      
      ---> GDU1 energy [mms4_edi_energy_gdu1_srvy_l2]
      
      
      ---> GDU2 energy [mms4_edi_energy_gdu2_srvy_l2]
      
      
      Field-aligned electron flux from both GDUs [mms4_edi_flux1_0_srvy_l2]
      
      
      ---> (no error bars displayed) Field-aligned electron flux from both GDUs [mms4_edi_flux1_0_srvy_l2_noerr]
      
      
      ---> Error in field-aligned electron flux from both GDUs. [mms4_edi_flux1_0_delta_srvy_l2]
      
      
      Anti-field-aligned electron flux from both GDUs [mms4_edi_flux1_180_srvy_l2]
      
      
      ---> (no error bars displayed) Anti-field-aligned electron flux from both GDUs [mms4_edi_flux1_180_srvy_l2_noerr]
      
      
      ---> Error in anti-field-aligned electron flux from both GDUs. [mms4_edi_flux1_180_delta_srvy_l2]
      
      
      Trajectory of field-aligned electrons from both GDUs in DBCS coordinates. [mms4_edi_traj1_dbcs_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs in DBCS coordinates. [mms4_edi_traj1_dbcs_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of field-aligned electrons from both GDUs in GSE coordinates. [mms4_edi_traj1_gse_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      Trajectory of anti-field-aligned electrons from both GDUs, in GSE coordinates. [mms4_edi_traj1_gse_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 0-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj1_gsm_0_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      [OUTDATED] Trajectory of flux1 180-degree pitch angle electrons in GSM coordinates. [mms4_edi_traj1_gsm_180_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS4_EDI_SRVY_L2_EFIELD (spase://NASA/NumericalData/MMS/4/FIELDS/EDI/Survey/Level2/ElectricField/PT5S)
Description
EDI electric field data. Instrument papers for EDI can be found at:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7
Modification History
v1.0.0 - First version. TRI-TOF selection based on smallest error.
v1.1.0 - TRI-TOF merged by weighted average.
v1.2.0 - Fixed t_delta_plus/minus CDF_type.
v1.3.0 - Fixed Fixed vdrift SI conversion.
v1.4.0 - Fixed data duplication caused by multiple l2pre file locations.
v1.5.0 - Inplemented baseline*beams*Bmag filter for triangulation.
v1.6.0 - Inplemented null files for no or low quality data.
 
  • Data Variable Descriptions
      ExB drift velocity in DSL coordinates. [mms4_edi_vdrift_dsl_srvy_l2]
      
      
      ---> ExB drift velocity in DSL coordinates (no error bars) [mms4_edi_vdrift_dsl_srvy_l2_noerr]
      
      
      ExB drift velocity in GSE coordinates. [mms4_edi_vdrift_gse_srvy_l2]
      
      
      ---> ExB drift velocity in GSE coordinates (no error bars) [mms4_edi_vdrift_gse_srvy_l2_noerr]
      
      
      ExB drift velocity in GSM coordinates. [mms4_edi_vdrift_gsm_srvy_l2]
      
      
      ---> ExB drift velocity in GSM coordinates (no error bars) [mms4_edi_vdrift_gsm_srvy_l2_noerr]
      
      
      Electric field in DSL coordinates. [mms4_edi_e_dsl_srvy_l2]
      
      
      ---> Electric field in DSL coordinates (no error bars) [mms4_edi_e_dsl_srvy_l2_noerr]
      
      
      Electric field in GSE coordinates. [mms4_edi_e_gse_srvy_l2]
      
      
      ---> Electric field in GSE coordinates (no error bars) [mms4_edi_e_gse_srvy_l2_noerr]
      
      
      Electric field in GSM coordinates. [mms4_edi_e_gsm_srvy_l2]
      
      
      ---> Electric field in GSM coordinates (no error bars) [mms4_edi_e_gsm_srvy_l2_noerr]
      
      
      Weighted use of TRI method in L2 results. [mms4_edi_tri_weight_srvy_l2]
      
      
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MMS4_EDI_SRVY_L2_Q0 (spase://NASA/NumericalData/MMS/4/FIELDS/EDI/Survey/Level2/QualityZero/PT0.125S)
Description
EDI Q0 data. The EDI instrument paper and data products guidescan be found at
the following two links:
http://link.springer.com/article/10.1007%2Fs11214-015-0182-7,
https://lasp.colorado.edu/mms/sdc/public/datasets/fields/
Modification History
v0.0.0 - First version.
v0.0.1 - Filled energy variables.
v0.0.2 - Energy written properly.
v1.0.0 - Update variable names.
v1.1.0 - Added optics state.
v2.0.0 - Added electron trajectories.
v2.1.0 - Deltas on trajectory vectors are now deltas.
v3.0.0 - Reduced file size with scalar errors. Add VAR_NOTES.
v4.0.0 - Removed unused Epoch variable.
v5.0.0 - Trajectories are provided in DBCS coordinates.
 
  • Data Variable Descriptions
      Optics state [mms4_edi_optics_state_srvy_l2]
      
      
      ---> GDU1 energy [mms4_edi_energy_gdu1_srvy_l2]
      
      
      ---> GDU2 energy [mms4_edi_energy_gdu2_srvy_l2]
      
      
      GDU1 quality 0 counts. [mms4_edi_counts_gdu1_srvy_l2]
      Q0 data consists of raw electron counts. The error at any one time is the
      square-root of the counts. Note that there may be contamination from the EDI
      electron beams. See the data products guide or contact an EDI team member to
      learn about beam contamination.
      
      GDU2 quality 0 counts. [mms4_edi_counts_gdu2_srvy_l2]
      
      
      GDU1 electron incident trajectory vectors in spherical BCS coordinates. [mms4_edi_traj_bcs_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical BCS coordinates. [mms4_edi_traj_bcs_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical DBCS coordinates. [mms4_edi_traj_dbcs_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical DBCS coordinates. [mms4_edi_traj_dbcs_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSE coordinates. [mms4_edi_traj_gse_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSE coordinates. [mms4_edi_traj_gse_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU1 electron incident trajectory vectors in spherical GSM coordinates. [mms4_edi_traj_gsm_gdu1_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
      GDU2 Electron incident trajectory vectors in spherical GSM coordinates. [mms4_edi_traj_gsm_gdu2_srvy_l2]
      Trajectories are given as unit vectors in spherical coordinates, with phi
      (theta) representing the azimuthal (polar) directions, in the indicated
      coordinate system. They are opposite to the nominal look-direction of the
      instrument. Errors represent an omni-directional error. For more details about
      errors, contact the EDI instrument team.
      
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MMS4_EDP_BRST_L2_DCE (spase://NASA/NumericalData/MMS/4/FIELDS/EDP/Burst/Level2/DCElectricField/PT0.0001220703125S)
Description
http://mms.gsfc.nasa.gov/
Modification History
V.0. Initial release.
 
  • Data Variable Descriptions
      L2 DC E Field calibrated for SDP and ADP (data begins 2023/07/04) [mms4_edp_dce_dsl2d_brst_l2]
      
      
      L2 DC E Field (GSE coords) calibrated for SDP and ADP, all flag values included (No data after 7/3/2023) [mms4_edp_dce_gse_brst_l2]
      
      
      L2 DC E Field (DSL coords) calibrated for SDP and ADP, all flag values included (No data after 7/3/2023) [mms4_edp_dce_dsl_brst_l2]
      
      
      L2 DC E Parallel Field calibrated for SDP and ADP (No data after 7/3/2023) [mms4_edp_dce_par_epar_brst_l2]
      
      
      Quality indicator (3 good), (2 ok data, use with some caution), (1 bad data, use with caution), (0 Really bad data or no data at all) [mms4_edp_quality_brst_l2]
      
      
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MMS4_EDP_BRST_L2_HMFE (spase://NASA/NumericalData/MMS/4/FIELDS/EDP/Burst/Level2Pre/HMFE/PT0.00001525878906S)
Description
 d
 
  • Data Variable Descriptions
      DC E Field calibrated for SDP and ADP [mms4_edp_hmfe_dsl_brst_l2]
      
      
      DC E parallel Field from calibrated SDP and ADP [mms4_edp_hmfe_par_epar_brst_l2]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS4_EDP_BRST_L2_SCPOT doi:10.48322/j5ge-t096
Proper citations should include the "Accessed on date" in the form .
Description
http://mms.gsfc.nasa.gov/
The full name of PI affiliations: SWRI - Southwest Research Institute. LASP -
Laboratory for Atmospheric and Space Physics. KTH - Kungliga Tekniska Hogskolan
(Swedish Royal Institute of Technology). 
Modification History
V.0. Initial release.
V.1. QL (v1.0.z), SCPOT (v1.0.z), L2A (v0.1.z) now uses ASPOC srvy l2 and
DEFATT, if these are available. Brst QL uses intermediate L2A file from Fast
mode for delta offsets. Bitmask changed to uint16 and Quality to uint8.
V.2. SCPOT (v2.0.z), L2A (v1.0.z) now uses variable names in accordance with new
recommended standard for FIELDS, All products change shortening factor to 1.25
on SDP, offsets applied indicated by GlobalAttribute Calibration_file.
V.2. L2a (v2.0.z), QL (v1.6.z) now try to remove solar wind wake which
previously left a clear sinusodial signal in the data.
V.3. L2a (v3.0.z) Slow Mode probe Gain set to 1.0 when orbital radius less than
5 RE (1.25 otherwise), L2pre (v2.0.z) DSL offsets removed from field is now
included in the file as the Slow mode is dependent on scpot product (Fast/Brst
is simply based on offset in Calibration_file).
 
  • Data Variable Descriptions
      Spacecraft potential [mms4_edp_scpot_brst_l2]
      
      
      Probe to spacecraft potential, averaged [mms4_edp_psp_brst_l2]
      
      
      Probe to spacecraft potential, individual probes [mms4_edp_dcv_brst_l2]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS4_EDP_FAST_L2_DCE (spase://NASA/NumericalData/MMS/4/FIELDS/EDP/Fast/Level2/DCElectricField/PT0.03125S)
Description
http://mms.gsfc.nasa.gov/
Modification History
V.0. Initial release.
 
  • Data Variable Descriptions
      L2 DC E Field (GSE coords) calibrated for SDP and ADP, all flag values included (No data after 7/3/2023) [mms4_edp_dce_gse_fast_l2]
      
      
      L2 DC E Field (DSL coords) calibrated for SDP and ADP, all flag values included (No data after 7/3/2023) [mms4_edp_dce_dsl_fast_l2]
      
      
      L2 DC E Parallel Field with error calibrated for SDP and ADP (No data after 7/3/2023) [mms4_edp_dce_par_epar_fast_l2]
      
      
      Approximate DC E field error derived from SDP (quality and bitmask) and ADP (residue) [mms4_edp_dce_err_fast_l2]
      
      
      Quality indicator (3 good), (2 ok data, use with some caution), (1 bad data, use with caution), (0 Really bad data or no data at all) [mms4_edp_quality_fast_l2]
      
      
      L2 DC E Field calibrated for SDP and ADP (data begins 2023/07/04) [mms4_edp_dce_dsl2d_fast_l2]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS4_EDP_FAST_L2_SCPOT doi:10.48322/194m-pq72
Proper citations should include the "Accessed on date" in the form .
Description
http://mms.gsfc.nasa.gov/
The full name of PI affiliations: SWRI - Southwest Research Institute. LASP -
Laboratory for Atmospheric and Space Physics. KTH - Kungliga Tekniska Hogskolan
(Swedish Royal Institute of Technology). 
Modification History
V.0. Initial release.
V.1. QL (v1.0.z), SCPOT (v1.0.z), L2A (v0.1.z) now uses ASPOC srvy l2 and
DEFATT, if these are available. Brst QL uses intermediate L2A file from Fast
mode for delta offsets. Bitmask changed to uint16 and Quality to uint8.
V.2. SCPOT (v2.0.z), L2A (v1.0.z) now uses variable names in accordance with new
recommended standard for FIELDS, All products change shortening factor to 1.25
on SDP, offsets applied indicated by GlobalAttribute Calibration_file.
V.2. L2a (v2.0.z), QL (v1.6.z) now try to remove solar wind wake which
previously left a clear sinusodial signal in the data.
V.3. L2a (v3.0.z) Slow Mode probe Gain set to 1.0 when orbital radius less than
5 RE (1.25 otherwise), L2pre (v2.0.z) DSL offsets removed from field is now
included in the file as the Slow mode is dependent on scpot product (Fast/Brst
is simply based on offset in Calibration_file).
 
  • Data Variable Descriptions
      Spacecraft potential [mms4_edp_scpot_fast_l2]
      
      
      Probe to spacecraft potential, averaged [mms4_edp_psp_fast_l2]
      
      
      Probe to spacecraft potential, individual probes [mms4_edp_dcv_fast_l2]
      
      
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MMS4_EDP_SLOW_L2_DCE (spase://NASA/NumericalData/MMS/4/FIELDS/EDP/Slow/Level2/DCElectricField/PT0.125S)
Description
http://mms.gsfc.nasa.gov/
Modification History
V.0. Initial release.
 
  • Data Variable Descriptions
      L2 DC E Field (GSE coords) calibrated for SDP and ADP, all flag values included (No data after 7/3/2023) [mms4_edp_dce_gse_slow_l2]
      
      
      L2 DC E Field (DSL coords) calibrated for SDP and ADP, all flag values included (No data after 7/3/2023) [mms4_edp_dce_dsl_slow_l2]
      
      
      L2 DC E Parallel Field with error calibrated for SDP and ADP (No data after 7/3/2023) [mms4_edp_dce_par_epar_slow_l2]
      
      
      Approximate DC E field error derived from SDP (quality and bitmask) and ADP (residue) [mms4_edp_dce_err_slow_l2]
      
      
      Quality indicator (3 good), (2 ok data, use with some caution), (1 bad data, use with caution), (0 Really bad data or no data at all) [mms4_edp_quality_slow_l2]
      
      
      L2 DC E Field calibrated for SDP and ADP (data begins 2023/07/04) [mms4_edp_dce_dsl2d_slow_l2]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS4_EDP_SLOW_L2_SCPOT doi:10.48322/t44j-x227
Proper citations should include the "Accessed on date" in the form .
Description
http://mms.gsfc.nasa.gov/
The full name of PI affiliations: SWRI - Southwest Research Institute. LASP -
Laboratory for Atmospheric and Space Physics. KTH - Kungliga Tekniska Hogskolan
(Swedish Royal Institute of Technology). 
Modification History
V.0. Initial release.
V.1. QL (v1.0.z), SCPOT (v1.0.z), L2A (v0.1.z) now uses ASPOC srvy l2 and
DEFATT, if these are available. Brst QL uses intermediate L2A file from Fast
mode for delta offsets. Bitmask changed to uint16 and Quality to uint8.
V.2. SCPOT (v2.0.z), L2A (v1.0.z) now uses variable names in accordance with new
recommended standard for FIELDS, All products change shortening factor to 1.25
on SDP, offsets applied indicated by GlobalAttribute Calibration_file.
V.2. L2a (v2.0.z), QL (v1.6.z) now try to remove solar wind wake which
previously left a clear sinusodial signal in the data.
V.3. L2a (v3.0.z) Slow Mode probe Gain set to 1.0 when orbital radius less than
5 RE (1.25 otherwise), L2pre (v2.0.z) DSL offsets removed from field is now
included in the file as the Slow mode is dependent on scpot product (Fast/Brst
is simply based on offset in Calibration_file).
 
  • Data Variable Descriptions
      Spacecraft potential [mms4_edp_scpot_slow_l2]
      
      
      Probe to spacecraft potential, averaged [mms4_edp_psp_slow_l2]
      
      
      Probe to spacecraft potential, individual probes [mms4_edp_dcv_slow_l2]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS4_EDP_SRVY_L2_HFESP (spase://NASA/NumericalData/MMS/4/FIELDS/EDP/Survey/Level2/HighFrequencyElectricFieldSpectra/PT16S)
Description
 AC Electric Field
 
  • Data Variable Descriptions
      HF ACE E Field Spectral Density [mms4_edp_hfesp_srvy_l2]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS4_EPD-EIS_BRST_L2_EXTOF (spase://NASA/NumericalData/MMS/4/EnergeticParticleDetector/EIS/Burst/Level2/EnergyByTimeOfFlight/PT0.605S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms4_epd_eis_brst_l2_extof_duration]
      
      
      ---> Instrument Deadtime [mms4_epd_eis_brst_l2_extof_deadtime]
      
      
      ---> Instrument Large Pixel in Use [mms4_epd_eis_brst_l2_extof_largepixel]
      
      
      ---> Spin [mms4_epd_eis_brst_l2_extof_spin]
      
      
      ---> Sector [mms4_epd_eis_brst_l2_extof_sector]
      
      
      ---> Quality Word [mms4_epd_eis_brst_l2_extof_quality]
      
      
      MMS4 ExTOF-Burst proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_extof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms4_epd_eis_brst_l2_extof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms4_epd_eis_brst_l2_extof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms4_epd_eis_brst_l2_extof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms4_epd_eis_brst_l2_extof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms4_epd_eis_brst_l2_extof_proton_P6_counts_t5]
      
      
      MMS4 ExTOF-Burst proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_extof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms4_epd_eis_brst_l2_extof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms4_epd_eis_brst_l2_extof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms4_epd_eis_brst_l2_extof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms4_epd_eis_brst_l2_extof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms4_epd_eis_brst_l2_extof_proton_P6_cps_t5]
      
      
      MMS4 ExTOF-Burst proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_extof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms4_epd_eis_brst_l2_extof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms4_epd_eis_brst_l2_extof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms4_epd_eis_brst_l2_extof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms4_epd_eis_brst_l2_extof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms4_epd_eis_brst_l2_extof_proton_P6_flux_t5]
      
      
      MMS4 ExTOF-Burst helium_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_extof_helium_P6_counts_t0]
      
      
      ---> helium_P6_counts_t1 [mms4_epd_eis_brst_l2_extof_helium_P6_counts_t1]
      
      
      ---> helium_P6_counts_t2 [mms4_epd_eis_brst_l2_extof_helium_P6_counts_t2]
      
      
      ---> helium_P6_counts_t3 [mms4_epd_eis_brst_l2_extof_helium_P6_counts_t3]
      
      
      ---> helium_P6_counts_t4 [mms4_epd_eis_brst_l2_extof_helium_P6_counts_t4]
      
      
      ---> helium_P6_counts_t5 [mms4_epd_eis_brst_l2_extof_helium_P6_counts_t5]
      
      
      MMS4 ExTOF-Burst helium_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_extof_helium_P6_cps_t0]
      
      
      ---> helium_P6_cps_t1 [mms4_epd_eis_brst_l2_extof_helium_P6_cps_t1]
      
      
      ---> helium_P6_cps_t2 [mms4_epd_eis_brst_l2_extof_helium_P6_cps_t2]
      
      
      ---> helium_P6_cps_t3 [mms4_epd_eis_brst_l2_extof_helium_P6_cps_t3]
      
      
      ---> helium_P6_cps_t4 [mms4_epd_eis_brst_l2_extof_helium_P6_cps_t4]
      
      
      ---> helium_P6_cps_t5 [mms4_epd_eis_brst_l2_extof_helium_P6_cps_t5]
      
      
      MMS4 ExTOF-Burst helium_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_extof_helium_P6_flux_t0]
      
      
      ---> helium_P6_flux_t1 [mms4_epd_eis_brst_l2_extof_helium_P6_flux_t1]
      
      
      ---> helium_P6_flux_t2 [mms4_epd_eis_brst_l2_extof_helium_P6_flux_t2]
      
      
      ---> helium_P6_flux_t3 [mms4_epd_eis_brst_l2_extof_helium_P6_flux_t3]
      
      
      ---> helium_P6_flux_t4 [mms4_epd_eis_brst_l2_extof_helium_P6_flux_t4]
      
      
      ---> helium_P6_flux_t5 [mms4_epd_eis_brst_l2_extof_helium_P6_flux_t5]
      
      
      MMS4 ExTOF-Burst oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_extof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms4_epd_eis_brst_l2_extof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms4_epd_eis_brst_l2_extof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms4_epd_eis_brst_l2_extof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms4_epd_eis_brst_l2_extof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms4_epd_eis_brst_l2_extof_oxygen_P6_counts_t5]
      
      
      MMS4 ExTOF-Burst oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_extof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms4_epd_eis_brst_l2_extof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms4_epd_eis_brst_l2_extof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms4_epd_eis_brst_l2_extof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms4_epd_eis_brst_l2_extof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms4_epd_eis_brst_l2_extof_oxygen_P6_cps_t5]
      
      
      MMS4 ExTOF-Burst oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_extof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms4_epd_eis_brst_l2_extof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms4_epd_eis_brst_l2_extof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms4_epd_eis_brst_l2_extof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms4_epd_eis_brst_l2_extof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms4_epd_eis_brst_l2_extof_oxygen_P6_flux_t5]
      
      
      MMS4 ExTOF-Burst dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_extof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms4_epd_eis_brst_l2_extof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms4_epd_eis_brst_l2_extof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms4_epd_eis_brst_l2_extof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms4_epd_eis_brst_l2_extof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms4_epd_eis_brst_l2_extof_dump_P6_counts_t5]
      
      
      MMS4 ExTOF-Burst dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_extof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms4_epd_eis_brst_l2_extof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms4_epd_eis_brst_l2_extof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms4_epd_eis_brst_l2_extof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms4_epd_eis_brst_l2_extof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms4_epd_eis_brst_l2_extof_dump_P6_cps_t5]
      
      
      MMS4 ExTOF-Burst dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_extof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms4_epd_eis_brst_l2_extof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms4_epd_eis_brst_l2_extof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms4_epd_eis_brst_l2_extof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms4_epd_eis_brst_l2_extof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms4_epd_eis_brst_l2_extof_dump_P6_flux_t5]
      
      
      MMS4 ExTOF-Burst proton_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_extof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms4_epd_eis_brst_l2_extof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms4_epd_eis_brst_l2_extof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms4_epd_eis_brst_l2_extof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms4_epd_eis_brst_l2_extof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms4_epd_eis_brst_l2_extof_proton_P5_counts_t5]
      
      
      MMS4 ExTOF-Burst proton_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_extof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms4_epd_eis_brst_l2_extof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms4_epd_eis_brst_l2_extof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms4_epd_eis_brst_l2_extof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms4_epd_eis_brst_l2_extof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms4_epd_eis_brst_l2_extof_proton_P5_cps_t5]
      
      
      MMS4 ExTOF-Burst proton_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_extof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms4_epd_eis_brst_l2_extof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms4_epd_eis_brst_l2_extof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms4_epd_eis_brst_l2_extof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms4_epd_eis_brst_l2_extof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms4_epd_eis_brst_l2_extof_proton_P5_flux_t5]
      
      
      MMS4 ExTOF-Burst oxygen_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_extof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms4_epd_eis_brst_l2_extof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms4_epd_eis_brst_l2_extof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms4_epd_eis_brst_l2_extof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms4_epd_eis_brst_l2_extof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms4_epd_eis_brst_l2_extof_oxygen_P5_counts_t5]
      
      
      MMS4 ExTOF-Burst oxygen_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_extof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms4_epd_eis_brst_l2_extof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms4_epd_eis_brst_l2_extof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms4_epd_eis_brst_l2_extof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms4_epd_eis_brst_l2_extof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms4_epd_eis_brst_l2_extof_oxygen_P5_cps_t5]
      
      
      MMS4 ExTOF-Burst oxygen_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_extof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms4_epd_eis_brst_l2_extof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms4_epd_eis_brst_l2_extof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms4_epd_eis_brst_l2_extof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms4_epd_eis_brst_l2_extof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms4_epd_eis_brst_l2_extof_oxygen_P5_flux_t5]
      
      
      MMS4 ExTOF-Burst helium_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_extof_helium_P5_counts_t0]
      
      
      ---> helium_P5_counts_t1 [mms4_epd_eis_brst_l2_extof_helium_P5_counts_t1]
      
      
      ---> helium_P5_counts_t2 [mms4_epd_eis_brst_l2_extof_helium_P5_counts_t2]
      
      
      ---> helium_P5_counts_t3 [mms4_epd_eis_brst_l2_extof_helium_P5_counts_t3]
      
      
      ---> helium_P5_counts_t4 [mms4_epd_eis_brst_l2_extof_helium_P5_counts_t4]
      
      
      ---> helium_P5_counts_t5 [mms4_epd_eis_brst_l2_extof_helium_P5_counts_t5]
      
      
      MMS4 ExTOF-Burst helium_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_extof_helium_P5_cps_t0]
      
      
      ---> helium_P5_cps_t1 [mms4_epd_eis_brst_l2_extof_helium_P5_cps_t1]
      
      
      ---> helium_P5_cps_t2 [mms4_epd_eis_brst_l2_extof_helium_P5_cps_t2]
      
      
      ---> helium_P5_cps_t3 [mms4_epd_eis_brst_l2_extof_helium_P5_cps_t3]
      
      
      ---> helium_P5_cps_t4 [mms4_epd_eis_brst_l2_extof_helium_P5_cps_t4]
      
      
      ---> helium_P5_cps_t5 [mms4_epd_eis_brst_l2_extof_helium_P5_cps_t5]
      
      
      MMS4 ExTOF-Burst helium_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_extof_helium_P5_flux_t0]
      
      
      ---> helium_P5_flux_t1 [mms4_epd_eis_brst_l2_extof_helium_P5_flux_t1]
      
      
      ---> helium_P5_flux_t2 [mms4_epd_eis_brst_l2_extof_helium_P5_flux_t2]
      
      
      ---> helium_P5_flux_t3 [mms4_epd_eis_brst_l2_extof_helium_P5_flux_t3]
      
      
      ---> helium_P5_flux_t4 [mms4_epd_eis_brst_l2_extof_helium_P5_flux_t4]
      
      
      ---> helium_P5_flux_t5 [mms4_epd_eis_brst_l2_extof_helium_P5_flux_t5]
      
      
      MMS4 ExTOF-Burst proton_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_extof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms4_epd_eis_brst_l2_extof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms4_epd_eis_brst_l2_extof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms4_epd_eis_brst_l2_extof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms4_epd_eis_brst_l2_extof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms4_epd_eis_brst_l2_extof_proton_P4_counts_t5]
      
      
      MMS4 ExTOF-Burst proton_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_extof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms4_epd_eis_brst_l2_extof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms4_epd_eis_brst_l2_extof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms4_epd_eis_brst_l2_extof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms4_epd_eis_brst_l2_extof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms4_epd_eis_brst_l2_extof_proton_P4_cps_t5]
      
      
      MMS4 ExTOF-Burst proton_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_extof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms4_epd_eis_brst_l2_extof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms4_epd_eis_brst_l2_extof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms4_epd_eis_brst_l2_extof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms4_epd_eis_brst_l2_extof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms4_epd_eis_brst_l2_extof_proton_P4_flux_t5]
      
      
      MMS4 ExTOF-Burst alpha_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_extof_helium_P4_counts_t0]
      
      
      ---> alpha_P4_counts_t1 [mms4_epd_eis_brst_l2_extof_helium_P4_counts_t1]
      
      
      ---> alpha_P4_counts_t2 [mms4_epd_eis_brst_l2_extof_helium_P4_counts_t2]
      
      
      ---> alpha_P4_counts_t3 [mms4_epd_eis_brst_l2_extof_helium_P4_counts_t3]
      
      
      ---> alpha_P4_counts_t4 [mms4_epd_eis_brst_l2_extof_helium_P4_counts_t4]
      
      
      ---> alpha_P4_counts_t5 [mms4_epd_eis_brst_l2_extof_helium_P4_counts_t5]
      
      
      MMS4 ExTOF-Burst alpha_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_extof_helium_P4_cps_t0]
      
      
      ---> alpha_P4_cps_t1 [mms4_epd_eis_brst_l2_extof_helium_P4_cps_t1]
      
      
      ---> alpha_P4_cps_t2 [mms4_epd_eis_brst_l2_extof_helium_P4_cps_t2]
      
      
      ---> alpha_P4_cps_t3 [mms4_epd_eis_brst_l2_extof_helium_P4_cps_t3]
      
      
      ---> alpha_P4_cps_t4 [mms4_epd_eis_brst_l2_extof_helium_P4_cps_t4]
      
      
      ---> alpha_P4_cps_t5 [mms4_epd_eis_brst_l2_extof_helium_P4_cps_t5]
      
      
      MMS4 ExTOF-Burst alpha_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_extof_helium_P4_flux_t0]
      
      
      ---> alpha_P4_flux_t1 [mms4_epd_eis_brst_l2_extof_helium_P4_flux_t1]
      
      
      ---> alpha_P4_flux_t2 [mms4_epd_eis_brst_l2_extof_helium_P4_flux_t2]
      
      
      ---> alpha_P4_flux_t3 [mms4_epd_eis_brst_l2_extof_helium_P4_flux_t3]
      
      
      ---> alpha_P4_flux_t4 [mms4_epd_eis_brst_l2_extof_helium_P4_flux_t4]
      
      
      ---> alpha_P4_flux_t5 [mms4_epd_eis_brst_l2_extof_helium_P4_flux_t5]
      
      
      MMS4 ExTOF-Burst oxygen_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_extof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms4_epd_eis_brst_l2_extof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms4_epd_eis_brst_l2_extof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms4_epd_eis_brst_l2_extof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms4_epd_eis_brst_l2_extof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms4_epd_eis_brst_l2_extof_oxygen_P4_counts_t5]
      
      
      MMS4 ExTOF-Burst oxygen_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_extof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms4_epd_eis_brst_l2_extof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms4_epd_eis_brst_l2_extof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms4_epd_eis_brst_l2_extof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms4_epd_eis_brst_l2_extof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms4_epd_eis_brst_l2_extof_oxygen_P4_cps_t5]
      
      
      MMS4 ExTOF-Burst oxygen_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_extof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms4_epd_eis_brst_l2_extof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms4_epd_eis_brst_l2_extof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms4_epd_eis_brst_l2_extof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms4_epd_eis_brst_l2_extof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms4_epd_eis_brst_l2_extof_oxygen_P4_flux_t5]
      
      
      MMS4 ExTOF-Burst proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_extof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms4_epd_eis_brst_l2_extof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms4_epd_eis_brst_l2_extof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms4_epd_eis_brst_l2_extof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms4_epd_eis_brst_l2_extof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms4_epd_eis_brst_l2_extof_proton_P3_counts_t5]
      
      
      MMS4 ExTOF-Burst proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_extof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms4_epd_eis_brst_l2_extof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms4_epd_eis_brst_l2_extof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms4_epd_eis_brst_l2_extof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms4_epd_eis_brst_l2_extof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms4_epd_eis_brst_l2_extof_proton_P3_cps_t5]
      
      
      MMS4 ExTOF-Burst proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_extof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms4_epd_eis_brst_l2_extof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms4_epd_eis_brst_l2_extof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms4_epd_eis_brst_l2_extof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms4_epd_eis_brst_l2_extof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms4_epd_eis_brst_l2_extof_proton_P3_flux_t5]
      
      
      MMS4 ExTOF-Burst alpha_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_extof_helium_P3_counts_t0]
      
      
      ---> alpha_P3_counts_t1 [mms4_epd_eis_brst_l2_extof_helium_P3_counts_t1]
      
      
      ---> alpha_P3_counts_t2 [mms4_epd_eis_brst_l2_extof_helium_P3_counts_t2]
      
      
      ---> alpha_P3_counts_t3 [mms4_epd_eis_brst_l2_extof_helium_P3_counts_t3]
      
      
      ---> alpha_P3_counts_t4 [mms4_epd_eis_brst_l2_extof_helium_P3_counts_t4]
      
      
      ---> alpha_P3_counts_t5 [mms4_epd_eis_brst_l2_extof_helium_P3_counts_t5]
      
      
      MMS4 ExTOF-Burst alpha_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_extof_helium_P3_cps_t0]
      
      
      ---> alpha_P3_cps_t1 [mms4_epd_eis_brst_l2_extof_helium_P3_cps_t1]
      
      
      ---> alpha_P3_cps_t2 [mms4_epd_eis_brst_l2_extof_helium_P3_cps_t2]
      
      
      ---> alpha_P3_cps_t3 [mms4_epd_eis_brst_l2_extof_helium_P3_cps_t3]
      
      
      ---> alpha_P3_cps_t4 [mms4_epd_eis_brst_l2_extof_helium_P3_cps_t4]
      
      
      ---> alpha_P3_cps_t5 [mms4_epd_eis_brst_l2_extof_helium_P3_cps_t5]
      
      
      MMS4 ExTOF-Burst alpha_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_extof_helium_P3_flux_t0]
      
      
      ---> alpha_P3_flux_t1 [mms4_epd_eis_brst_l2_extof_helium_P3_flux_t1]
      
      
      ---> alpha_P3_flux_t2 [mms4_epd_eis_brst_l2_extof_helium_P3_flux_t2]
      
      
      ---> alpha_P3_flux_t3 [mms4_epd_eis_brst_l2_extof_helium_P3_flux_t3]
      
      
      ---> alpha_P3_flux_t4 [mms4_epd_eis_brst_l2_extof_helium_P3_flux_t4]
      
      
      ---> alpha_P3_flux_t5 [mms4_epd_eis_brst_l2_extof_helium_P3_flux_t5]
      
      
      MMS4 ExTOF-Burst oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_extof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms4_epd_eis_brst_l2_extof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms4_epd_eis_brst_l2_extof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms4_epd_eis_brst_l2_extof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms4_epd_eis_brst_l2_extof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms4_epd_eis_brst_l2_extof_oxygen_P3_counts_t5]
      
      
      MMS4 ExTOF-Burst oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_extof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms4_epd_eis_brst_l2_extof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms4_epd_eis_brst_l2_extof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms4_epd_eis_brst_l2_extof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms4_epd_eis_brst_l2_extof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms4_epd_eis_brst_l2_extof_oxygen_P3_cps_t5]
      
      
      MMS4 ExTOF-Burst oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_extof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms4_epd_eis_brst_l2_extof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms4_epd_eis_brst_l2_extof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms4_epd_eis_brst_l2_extof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms4_epd_eis_brst_l2_extof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms4_epd_eis_brst_l2_extof_oxygen_P3_flux_t5]
      
      
      MMS4 ExTOF-Burst dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_extof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms4_epd_eis_brst_l2_extof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms4_epd_eis_brst_l2_extof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms4_epd_eis_brst_l2_extof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms4_epd_eis_brst_l2_extof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms4_epd_eis_brst_l2_extof_dump_P3_counts_t5]
      
      
      MMS4 ExTOF-Burst dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_extof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms4_epd_eis_brst_l2_extof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms4_epd_eis_brst_l2_extof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms4_epd_eis_brst_l2_extof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms4_epd_eis_brst_l2_extof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms4_epd_eis_brst_l2_extof_dump_P4_counts_t5]
      
      
      MMS4 ExTOF-Burst dump_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_extof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms4_epd_eis_brst_l2_extof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms4_epd_eis_brst_l2_extof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms4_epd_eis_brst_l2_extof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms4_epd_eis_brst_l2_extof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms4_epd_eis_brst_l2_extof_dump_P5_counts_t5]
      
      
      MMS4 ExTOF-Burst dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_extof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms4_epd_eis_brst_l2_extof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms4_epd_eis_brst_l2_extof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms4_epd_eis_brst_l2_extof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms4_epd_eis_brst_l2_extof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms4_epd_eis_brst_l2_extof_dump_P3_cps_t5]
      
      
      MMS4 ExTOF-Burst dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_extof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms4_epd_eis_brst_l2_extof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms4_epd_eis_brst_l2_extof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms4_epd_eis_brst_l2_extof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms4_epd_eis_brst_l2_extof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms4_epd_eis_brst_l2_extof_dump_P4_cps_t5]
      
      
      MMS4 ExTOF-Burst dump_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_extof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms4_epd_eis_brst_l2_extof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms4_epd_eis_brst_l2_extof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms4_epd_eis_brst_l2_extof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms4_epd_eis_brst_l2_extof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms4_epd_eis_brst_l2_extof_dump_P5_cps_t5]
      
      
      MMS4 ExTOF-Burst dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_extof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms4_epd_eis_brst_l2_extof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms4_epd_eis_brst_l2_extof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms4_epd_eis_brst_l2_extof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms4_epd_eis_brst_l2_extof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms4_epd_eis_brst_l2_extof_dump_P3_flux_t5]
      
      
      MMS4 ExTOF-Burst dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_extof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms4_epd_eis_brst_l2_extof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms4_epd_eis_brst_l2_extof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms4_epd_eis_brst_l2_extof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms4_epd_eis_brst_l2_extof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms4_epd_eis_brst_l2_extof_dump_P4_flux_t5]
      
      
      MMS4 ExTOF-Burst dump_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_extof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms4_epd_eis_brst_l2_extof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms4_epd_eis_brst_l2_extof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms4_epd_eis_brst_l2_extof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms4_epd_eis_brst_l2_extof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms4_epd_eis_brst_l2_extof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS4 [mms4_epd_eis_brst_l2_extof_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS4 [mms4_epd_eis_brst_l2_extof_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS4 [mms4_epd_eis_brst_l2_extof_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS4 [mms4_epd_eis_brst_l2_extof_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS4 [mms4_epd_eis_brst_l2_extof_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS4 [mms4_epd_eis_brst_l2_extof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS4 [mms4_epd_eis_brst_l2_extof_look_t0]
      
      
      Look Direction for Telescope 1 MMS4 [mms4_epd_eis_brst_l2_extof_look_t1]
      
      
      Look Direction for Telescope 2 MMS4 [mms4_epd_eis_brst_l2_extof_look_t2]
      
      
      Look Direction for Telescope 3 MMS4 [mms4_epd_eis_brst_l2_extof_look_t3]
      
      
      Look Direction for Telescope 4 MMS4 [mms4_epd_eis_brst_l2_extof_look_t4]
      
      
      Look Direction for Telescope 5 MMS4 [mms4_epd_eis_brst_l2_extof_look_t5]
      
      
      Magnetic Field BCS MMS4 [mms4_epd_eis_brst_l2_extof_b]
      
      
      Spacecraft position GSE MMS4 [mms4_epd_eis_brst_l2_extof_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS4 [mms4_epd_eis_brst_l2_extof_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS4 [mms4_epd_eis_brst_l2_extof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS4 [mms4_epd_eis_brst_l2_extof_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS4 [mms4_epd_eis_brst_l2_extof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS4 [mms4_epd_eis_brst_l2_extof_r]
      
      
      Dipole L-shell MMS4 [mms4_epd_eis_brst_l2_extof_l]
      
      
      Latitude in GSE Frame MMS4 [mms4_epd_eis_brst_l2_extof_gse_lat]
      
      
      Longitude in GSE Frame MMS4 [mms4_epd_eis_brst_l2_extof_gse_lon]
      
      
      Latitude in GSM Frame MMS4 [mms4_epd_eis_brst_l2_extof_gsm_lat]
      
      
      Longitude in GSM Frame MMS4 [mms4_epd_eis_brst_l2_extof_gsm_lon]
      
      
      Latitude in SM Frame MMS4 [mms4_epd_eis_brst_l2_extof_sm_lat]
      
      
      Longitude in SM Frame MMS4 [mms4_epd_eis_brst_l2_extof_sm_lon]
      
      
      Orbit number MMS4 [mms4_epd_eis_brst_l2_extof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS4 [mms4_epd_eis_brst_l2_extof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS4 [mms4_epd_eis_brst_l2_extof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS4 [mms4_epd_eis_brst_l2_extof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS4 [mms4_epd_eis_brst_l2_extof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS4 [mms4_epd_eis_brst_l2_extof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS4 [mms4_epd_eis_brst_l2_extof_ssd5]
      
      
      Valid Events Processed per second MMS4 [mms4_epd_eis_brst_l2_extof_vep]
      
      
      Start 0 Anode Count Rate MMS4 [mms4_epd_eis_brst_l2_extof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS4 [mms4_epd_eis_brst_l2_extof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS4 [mms4_epd_eis_brst_l2_extof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS4 [mms4_epd_eis_brst_l2_extof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS4 [mms4_epd_eis_brst_l2_extof_vtofxphe]
      
      
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MMS4_EPD-EIS_BRST_L2_PHXTOF (spase://NASA/NumericalData/MMS/4/EnergeticParticleDetector/EIS/Burst/Level2/PulseHeightByTimeOfFlight/PT0.605S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms4_epd_eis_brst_l2_phxtof_duration]
      
      
      ---> Instrument Deadtime [mms4_epd_eis_brst_l2_phxtof_deadtime]
      
      
      ---> Instrument Large Pixel in Use [mms4_epd_eis_brst_l2_phxtof_largepixel]
      
      
      ---> Spin [mms4_epd_eis_brst_l2_phxtof_spin]
      
      
      ---> Sector [mms4_epd_eis_brst_l2_phxtof_sector]
      
      
      ---> Quality Word [mms4_epd_eis_brst_l2_phxtof_quality]
      
      
      MMS4 PhxTOF-Burst proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms4_epd_eis_brst_l2_phxtof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms4_epd_eis_brst_l2_phxtof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms4_epd_eis_brst_l2_phxtof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms4_epd_eis_brst_l2_phxtof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms4_epd_eis_brst_l2_phxtof_proton_P6_counts_t5]
      
      
      MMS4 PhxTOF-Burst proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms4_epd_eis_brst_l2_phxtof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms4_epd_eis_brst_l2_phxtof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms4_epd_eis_brst_l2_phxtof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms4_epd_eis_brst_l2_phxtof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms4_epd_eis_brst_l2_phxtof_proton_P6_cps_t5]
      
      
      MMS4 PhxTOF-Burst proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms4_epd_eis_brst_l2_phxtof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms4_epd_eis_brst_l2_phxtof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms4_epd_eis_brst_l2_phxtof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms4_epd_eis_brst_l2_phxtof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms4_epd_eis_brst_l2_phxtof_proton_P6_flux_t5]
      
      
      MMS4 PhxTOF-Burst oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_counts_t5]
      
      
      MMS4 PhxTOF-Burst oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_cps_t5]
      
      
      MMS4 PhxTOF-Burst oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms4_epd_eis_brst_l2_phxtof_oxygen_P6_flux_t5]
      
      
      MMS4 PhxTOF-Burst dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms4_epd_eis_brst_l2_phxtof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms4_epd_eis_brst_l2_phxtof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms4_epd_eis_brst_l2_phxtof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms4_epd_eis_brst_l2_phxtof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms4_epd_eis_brst_l2_phxtof_dump_P6_counts_t5]
      
      
      MMS4 PhxTOF-Burst dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms4_epd_eis_brst_l2_phxtof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms4_epd_eis_brst_l2_phxtof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms4_epd_eis_brst_l2_phxtof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms4_epd_eis_brst_l2_phxtof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms4_epd_eis_brst_l2_phxtof_dump_P6_cps_t5]
      
      
      MMS4 PhxTOF-Burst dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms4_epd_eis_brst_l2_phxtof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms4_epd_eis_brst_l2_phxtof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms4_epd_eis_brst_l2_phxtof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms4_epd_eis_brst_l2_phxtof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms4_epd_eis_brst_l2_phxtof_dump_P6_flux_t5]
      
      
      MMS4 PhxTOF-Burst proton_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms4_epd_eis_brst_l2_phxtof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms4_epd_eis_brst_l2_phxtof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms4_epd_eis_brst_l2_phxtof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms4_epd_eis_brst_l2_phxtof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms4_epd_eis_brst_l2_phxtof_proton_P5_counts_t5]
      
      
      MMS4 PhxTOF-Burst proton_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms4_epd_eis_brst_l2_phxtof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms4_epd_eis_brst_l2_phxtof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms4_epd_eis_brst_l2_phxtof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms4_epd_eis_brst_l2_phxtof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms4_epd_eis_brst_l2_phxtof_proton_P5_cps_t5]
      
      
      MMS4 PhxTOF-Burst proton_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms4_epd_eis_brst_l2_phxtof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms4_epd_eis_brst_l2_phxtof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms4_epd_eis_brst_l2_phxtof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms4_epd_eis_brst_l2_phxtof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms4_epd_eis_brst_l2_phxtof_proton_P5_flux_t5]
      
      
      MMS4 PhxTOF-Burst oxygen_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_counts_t5]
      
      
      MMS4 PhxTOF-Burst oxygen_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_cps_t5]
      
      
      MMS4 PhxTOF-Burst oxygen_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms4_epd_eis_brst_l2_phxtof_oxygen_P5_flux_t5]
      
      
      MMS4 PhxTOF-Burst proton_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_phxtof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms4_epd_eis_brst_l2_phxtof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms4_epd_eis_brst_l2_phxtof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms4_epd_eis_brst_l2_phxtof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms4_epd_eis_brst_l2_phxtof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms4_epd_eis_brst_l2_phxtof_proton_P4_counts_t5]
      
      
      MMS4 PhxTOF-Burst proton_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_phxtof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms4_epd_eis_brst_l2_phxtof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms4_epd_eis_brst_l2_phxtof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms4_epd_eis_brst_l2_phxtof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms4_epd_eis_brst_l2_phxtof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms4_epd_eis_brst_l2_phxtof_proton_P4_cps_t5]
      
      
      MMS4 PhxTOF-Burst proton_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_phxtof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms4_epd_eis_brst_l2_phxtof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms4_epd_eis_brst_l2_phxtof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms4_epd_eis_brst_l2_phxtof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms4_epd_eis_brst_l2_phxtof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms4_epd_eis_brst_l2_phxtof_proton_P4_flux_t5]
      
      
      MMS4 PhxTOF-Burst oxygen_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_counts_t5]
      
      
      MMS4 PhxTOF-Burst oxygen_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_cps_t5]
      
      
      MMS4 PhxTOF-Burst oxygen_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms4_epd_eis_brst_l2_phxtof_oxygen_P4_flux_t5]
      
      
      MMS4 PhxTOF-Burst proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_phxtof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms4_epd_eis_brst_l2_phxtof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms4_epd_eis_brst_l2_phxtof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms4_epd_eis_brst_l2_phxtof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms4_epd_eis_brst_l2_phxtof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms4_epd_eis_brst_l2_phxtof_proton_P3_counts_t5]
      
      
      MMS4 PhxTOF-Burst proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_phxtof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms4_epd_eis_brst_l2_phxtof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms4_epd_eis_brst_l2_phxtof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms4_epd_eis_brst_l2_phxtof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms4_epd_eis_brst_l2_phxtof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms4_epd_eis_brst_l2_phxtof_proton_P3_cps_t5]
      
      
      MMS4 PhxTOF-Burst proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_phxtof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms4_epd_eis_brst_l2_phxtof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms4_epd_eis_brst_l2_phxtof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms4_epd_eis_brst_l2_phxtof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms4_epd_eis_brst_l2_phxtof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms4_epd_eis_brst_l2_phxtof_proton_P3_flux_t5]
      
      
      MMS4 PhxTOF-Burst oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_counts_t5]
      
      
      MMS4 PhxTOF-Burst oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_cps_t5]
      
      
      MMS4 PhxTOF-Burst oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms4_epd_eis_brst_l2_phxtof_oxygen_P3_flux_t5]
      
      
      MMS4 PhxTOF-Burst dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_phxtof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms4_epd_eis_brst_l2_phxtof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms4_epd_eis_brst_l2_phxtof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms4_epd_eis_brst_l2_phxtof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms4_epd_eis_brst_l2_phxtof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms4_epd_eis_brst_l2_phxtof_dump_P3_counts_t5]
      
      
      MMS4 PhxTOF-Burst dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_phxtof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms4_epd_eis_brst_l2_phxtof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms4_epd_eis_brst_l2_phxtof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms4_epd_eis_brst_l2_phxtof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms4_epd_eis_brst_l2_phxtof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms4_epd_eis_brst_l2_phxtof_dump_P4_counts_t5]
      
      
      MMS4 PhxTOF-Burst dump_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms4_epd_eis_brst_l2_phxtof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms4_epd_eis_brst_l2_phxtof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms4_epd_eis_brst_l2_phxtof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms4_epd_eis_brst_l2_phxtof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms4_epd_eis_brst_l2_phxtof_dump_P5_counts_t5]
      
      
      MMS4 PhxTOF-Burst dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_phxtof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms4_epd_eis_brst_l2_phxtof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms4_epd_eis_brst_l2_phxtof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms4_epd_eis_brst_l2_phxtof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms4_epd_eis_brst_l2_phxtof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms4_epd_eis_brst_l2_phxtof_dump_P3_cps_t5]
      
      
      MMS4 PhxTOF-Burst dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_phxtof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms4_epd_eis_brst_l2_phxtof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms4_epd_eis_brst_l2_phxtof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms4_epd_eis_brst_l2_phxtof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms4_epd_eis_brst_l2_phxtof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms4_epd_eis_brst_l2_phxtof_dump_P4_cps_t5]
      
      
      MMS4 PhxTOF-Burst dump_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms4_epd_eis_brst_l2_phxtof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms4_epd_eis_brst_l2_phxtof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms4_epd_eis_brst_l2_phxtof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms4_epd_eis_brst_l2_phxtof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms4_epd_eis_brst_l2_phxtof_dump_P5_cps_t5]
      
      
      MMS4 PhxTOF-Burst dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_brst_l2_phxtof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms4_epd_eis_brst_l2_phxtof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms4_epd_eis_brst_l2_phxtof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms4_epd_eis_brst_l2_phxtof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms4_epd_eis_brst_l2_phxtof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms4_epd_eis_brst_l2_phxtof_dump_P3_flux_t5]
      
      
      MMS4 PhxTOF-Burst dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_brst_l2_phxtof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms4_epd_eis_brst_l2_phxtof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms4_epd_eis_brst_l2_phxtof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms4_epd_eis_brst_l2_phxtof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms4_epd_eis_brst_l2_phxtof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms4_epd_eis_brst_l2_phxtof_dump_P4_flux_t5]
      
      
      MMS4 PhxTOF-Burst dump_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_brst_l2_phxtof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms4_epd_eis_brst_l2_phxtof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms4_epd_eis_brst_l2_phxtof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms4_epd_eis_brst_l2_phxtof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms4_epd_eis_brst_l2_phxtof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms4_epd_eis_brst_l2_phxtof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS4 [mms4_epd_eis_brst_l2_phxtof_pitch_angle_t0]
      
      
      ---> Pitch Angle for Telescope 1 MMS4 [mms4_epd_eis_brst_l2_phxtof_pitch_angle_t1]
      
      
      ---> Pitch Angle for Telescope 2 MMS4 [mms4_epd_eis_brst_l2_phxtof_pitch_angle_t2]
      
      
      ---> Pitch Angle for Telescope 3 MMS4 [mms4_epd_eis_brst_l2_phxtof_pitch_angle_t3]
      
      
      ---> Pitch Angle for Telescope 4 MMS4 [mms4_epd_eis_brst_l2_phxtof_pitch_angle_t4]
      
      
      ---> Pitch Angle for Telescope 5 MMS4 [mms4_epd_eis_brst_l2_phxtof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS4 [mms4_epd_eis_brst_l2_phxtof_look_t0]
      
      
      ---> Look Direction for Telescope 1 MMS4 [mms4_epd_eis_brst_l2_phxtof_look_t1]
      
      
      ---> Look Direction for Telescope 2 MMS4 [mms4_epd_eis_brst_l2_phxtof_look_t2]
      
      
      ---> Look Direction for Telescope 3 MMS4 [mms4_epd_eis_brst_l2_phxtof_look_t3]
      
      
      ---> Look Direction for Telescope 4 MMS4 [mms4_epd_eis_brst_l2_phxtof_look_t4]
      
      
      ---> Look Direction for Telescope 5 MMS4 [mms4_epd_eis_brst_l2_phxtof_look_t5]
      
      
      Magnetic Field BCS MMS4 [mms4_epd_eis_brst_l2_phxtof_b]
      
      
      Spacecraft position GSE MMS4 [mms4_epd_eis_brst_l2_phxtof_position_gse]
      
      
      ---> Spacecraft position in GSM coordinates MMS4 [mms4_epd_eis_brst_l2_phxtof_position_gsm]
      
      
      ---> Spacecraft-Moon vector in GSE coordinates MMS4 [mms4_epd_eis_brst_l2_phxtof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS4 [mms4_epd_eis_brst_l2_phxtof_sc_to_gse]
      
      
      ---> Transformation Matrix GSE to GSM Frame MMS4 [mms4_epd_eis_brst_l2_phxtof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS4 [mms4_epd_eis_brst_l2_phxtof_r]
      
      
      Dipole L-shell MMS4 [mms4_epd_eis_brst_l2_phxtof_l]
      
      
      Latitude in GSE Frame MMS4 [mms4_epd_eis_brst_l2_phxtof_gse_lat]
      
      
      Longitude in GSE Frame MMS4 [mms4_epd_eis_brst_l2_phxtof_gse_lon]
      
      
      Latitude in GSM Frame MMS4 [mms4_epd_eis_brst_l2_phxtof_gsm_lat]
      
      
      Longitude in GSM Frame MMS4 [mms4_epd_eis_brst_l2_phxtof_gsm_lon]
      
      
      Latitude in SM Frame MMS4 [mms4_epd_eis_brst_l2_phxtof_sm_lat]
      
      
      Longitude in SM Frame MMS4 [mms4_epd_eis_brst_l2_phxtof_sm_lon]
      
      
      Orbit number MMS4 [mms4_epd_eis_brst_l2_phxtof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS4 [mms4_epd_eis_brst_l2_phxtof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS4 [mms4_epd_eis_brst_l2_phxtof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS4 [mms4_epd_eis_brst_l2_phxtof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS4 [mms4_epd_eis_brst_l2_phxtof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS4 [mms4_epd_eis_brst_l2_phxtof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS4 [mms4_epd_eis_brst_l2_phxtof_ssd5]
      
      
      Valid Events Processed per second MMS4 [mms4_epd_eis_brst_l2_phxtof_vep]
      
      
      Start 0 Anode Count Rate MMS4 [mms4_epd_eis_brst_l2_phxtof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS4 [mms4_epd_eis_brst_l2_phxtof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS4 [mms4_epd_eis_brst_l2_phxtof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS4 [mms4_epd_eis_brst_l2_phxtof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS4 [mms4_epd_eis_brst_l2_phxtof_vtofxphe]
      
      
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MMS4_EPD-EIS_SRVY_L2_ELECTRONENERGY (spase://NASA/NumericalData/MMS/4/EnergeticParticleDetector/EIS/Survey/Level2/ElectronEnergySpectra/PT2.42S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms4_epd_eis_srvy_l2_electronenergy_duration]
      
      
      Instrument Deadtime [mms4_epd_eis_srvy_l2_electronenergy_deadtime]
      
      
      Instrument Large Pixel in Use [mms4_epd_eis_srvy_l2_electronenergy_largepixel]
      
      
      Spin [mms4_epd_eis_srvy_l2_electronenergy_spin]
      
      
      Sector [mms4_epd_eis_srvy_l2_electronenergy_sector]
      
      
      Quality Word [mms4_epd_eis_srvy_l2_electronenergy_quality]
      
      
      MMS4 ElectronEnergy-Survey electron_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t0]
      
      
      ---> electron_P6_counts_t1 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t1]
      
      
      ---> electron_P6_counts_t2 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t2]
      
      
      ---> electron_P6_counts_t3 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t3]
      
      
      ---> electron_P6_counts_t4 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t4]
      
      
      ---> electron_P6_counts_t5 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_counts_t5]
      
      
      MMS4 ElectronEnergy-Survey electron_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t0]
      
      
      ---> electron_P6_cps_t1 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t1]
      
      
      ---> electron_P6_cps_t2 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t2]
      
      
      ---> electron_P6_cps_t3 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t3]
      
      
      ---> electron_P6_cps_t4 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t4]
      
      
      ---> electron_P6_cps_t5 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_cps_t5]
      
      
      MMS4 ElectronEnergy-Survey electron_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t0]
      
      
      ---> electron_P6_flux_t1 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t1]
      
      
      ---> electron_P6_flux_t2 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t2]
      
      
      ---> electron_P6_flux_t3 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t3]
      
      
      ---> electron_P6_flux_t4 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t4]
      
      
      ---> electron_P6_flux_t5 [mms4_epd_eis_srvy_l2_electronenergy_electron_P6_flux_t5]
      
      
      MMS4 ElectronEnergy-Survey dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_counts_t5]
      
      
      MMS4 ElectronEnergy-Survey dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_cps_t5]
      
      
      MMS4 ElectronEnergy-Survey dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms4_epd_eis_srvy_l2_electronenergy_dump_P6_flux_t5]
      
      
      MMS4 ElectronEnergy-Survey electron_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t0]
      
      
      ---> electron_P5_counts_t1 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t1]
      
      
      ---> electron_P5_counts_t2 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t2]
      
      
      ---> electron_P5_counts_t3 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t3]
      
      
      ---> electron_P5_counts_t4 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t4]
      
      
      ---> electron_P5_counts_t5 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_counts_t5]
      
      
      MMS4 ElectronEnergy-Survey electron_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t0]
      
      
      ---> electron_P5_cps_t1 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t1]
      
      
      ---> electron_P5_cps_t2 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t2]
      
      
      ---> electron_P5_cps_t3 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t3]
      
      
      ---> electron_P5_cps_t4 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t4]
      
      
      ---> electron_P5_cps_t5 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_cps_t5]
      
      
      MMS4 ElectronEnergy-Survey electron_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t0]
      
      
      ---> electron_P5_flux_t1 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t1]
      
      
      ---> electron_P5_flux_t2 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t2]
      
      
      ---> electron_P5_flux_t3 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t3]
      
      
      ---> electron_P5_flux_t4 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t4]
      
      
      ---> electron_P5_flux_t5 [mms4_epd_eis_srvy_l2_electronenergy_electron_P5_flux_t5]
      
      
      MMS4 ElectronEnergy-Survey electron_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t0]
      
      
      ---> electron_P4_counts_t1 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t1]
      
      
      ---> electron_P4_counts_t2 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t2]
      
      
      ---> electron_P4_counts_t3 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t3]
      
      
      ---> electron_P4_counts_t4 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t4]
      
      
      ---> electron_P4_counts_t5 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_counts_t5]
      
      
      MMS4 ElectronEnergy-Survey electron_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t0]
      
      
      ---> electron_P4_cps_t1 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t1]
      
      
      ---> electron_P4_cps_t2 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t2]
      
      
      ---> electron_P4_cps_t3 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t3]
      
      
      ---> electron_P4_cps_t4 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t4]
      
      
      ---> electron_P4_cps_t5 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_cps_t5]
      
      
      MMS4 ElectronEnergy-Survey electron_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t0]
      
      
      ---> electron_P4_flux_t1 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t1]
      
      
      ---> electron_P4_flux_t2 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t2]
      
      
      ---> electron_P4_flux_t3 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t3]
      
      
      ---> electron_P4_flux_t4 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t4]
      
      
      ---> electron_P4_flux_t5 [mms4_epd_eis_srvy_l2_electronenergy_electron_P4_flux_t5]
      
      
      MMS4 ElectronEnergy-Survey electron_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t0]
      
      
      ---> electron_P3_counts_t1 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t1]
      
      
      ---> electron_P3_counts_t2 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t2]
      
      
      ---> electron_P3_counts_t3 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t3]
      
      
      ---> electron_P3_counts_t4 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t4]
      
      
      ---> electron_P3_counts_t5 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_counts_t5]
      
      
      MMS4 ElectronEnergy-Survey electron_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t0]
      
      
      ---> electron_P3_cps_t1 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t1]
      
      
      ---> electron_P3_cps_t2 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t2]
      
      
      ---> electron_P3_cps_t3 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t3]
      
      
      ---> electron_P3_cps_t4 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t4]
      
      
      ---> electron_P3_cps_t5 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_cps_t5]
      
      
      MMS4 ElectronEnergy-Survey electron_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t0]
      
      
      ---> electron_P3_flux_t1 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t1]
      
      
      ---> electron_P3_flux_t2 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t2]
      
      
      ---> electron_P3_flux_t3 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t3]
      
      
      ---> electron_P3_flux_t4 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t4]
      
      
      ---> electron_P3_flux_t5 [mms4_epd_eis_srvy_l2_electronenergy_electron_P3_flux_t5]
      
      
      MMS4 ElectronEnergy-Survey dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_counts_t5]
      
      
      MMS4 ElectronEnergy-Survey dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_counts_t5]
      
      
      MMS4 ElectronEnergy-Survey dump_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_counts_t5]
      
      
      MMS4 ElectronEnergy-Survey dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_cps_t5]
      
      
      MMS4 ElectronEnergy-Survey dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_cps_t5]
      
      
      MMS4 ElectronEnergy-Survey dump_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_cps_t5]
      
      
      MMS4 ElectronEnergy-Survey dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms4_epd_eis_srvy_l2_electronenergy_dump_P3_flux_t5]
      
      
      MMS4 ElectronEnergy-Survey dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms4_epd_eis_srvy_l2_electronenergy_dump_P4_flux_t5]
      
      
      MMS4 ElectronEnergy-Survey dump_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms4_epd_eis_srvy_l2_electronenergy_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS4 [mms4_epd_eis_srvy_l2_electronenergy_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS4 [mms4_epd_eis_srvy_l2_electronenergy_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS4 [mms4_epd_eis_srvy_l2_electronenergy_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS4 [mms4_epd_eis_srvy_l2_electronenergy_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS4 [mms4_epd_eis_srvy_l2_electronenergy_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS4 [mms4_epd_eis_srvy_l2_electronenergy_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS4 [mms4_epd_eis_srvy_l2_electronenergy_look_t0]
      
      
      Look Direction for Telescope 1 MMS4 [mms4_epd_eis_srvy_l2_electronenergy_look_t1]
      
      
      Look Direction for Telescope 2 MMS4 [mms4_epd_eis_srvy_l2_electronenergy_look_t2]
      
      
      Look Direction for Telescope 3 MMS4 [mms4_epd_eis_srvy_l2_electronenergy_look_t3]
      
      
      Look Direction for Telescope 4 MMS4 [mms4_epd_eis_srvy_l2_electronenergy_look_t4]
      
      
      Look Direction for Telescope 5 MMS4 [mms4_epd_eis_srvy_l2_electronenergy_look_t5]
      
      
      Magnetic Field BCS MMS4 [mms4_epd_eis_srvy_l2_electronenergy_b]
      
      
      Spacecraft position GSE MMS4 [mms4_epd_eis_srvy_l2_electronenergy_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS4 [mms4_epd_eis_srvy_l2_electronenergy_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS4 [mms4_epd_eis_srvy_l2_electronenergy_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS4 [mms4_epd_eis_srvy_l2_electronenergy_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS4 [mms4_epd_eis_srvy_l2_electronenergy_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS4 [mms4_epd_eis_srvy_l2_electronenergy_r]
      
      
      Dipole L-shell MMS4 [mms4_epd_eis_srvy_l2_electronenergy_l]
      
      
      Latitude in GSE Frame MMS4 [mms4_epd_eis_srvy_l2_electronenergy_gse_lat]
      
      
      Longitude in GSE Frame MMS4 [mms4_epd_eis_srvy_l2_electronenergy_gse_lon]
      
      
      Latitude in GSM Frame MMS4 [mms4_epd_eis_srvy_l2_electronenergy_gsm_lat]
      
      
      Longitude in GSM Frame MMS4 [mms4_epd_eis_srvy_l2_electronenergy_gsm_lon]
      
      
      Latitude in SM Frame MMS4 [mms4_epd_eis_srvy_l2_electronenergy_sm_lat]
      
      
      Longitude in SM Frame MMS4 [mms4_epd_eis_srvy_l2_electronenergy_sm_lon]
      
      
      Orbit number MMS4 [mms4_epd_eis_srvy_l2_electronenergy_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS4 [mms4_epd_eis_srvy_l2_electronenergy_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS4 [mms4_epd_eis_srvy_l2_electronenergy_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS4 [mms4_epd_eis_srvy_l2_electronenergy_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS4 [mms4_epd_eis_srvy_l2_electronenergy_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS4 [mms4_epd_eis_srvy_l2_electronenergy_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS4 [mms4_epd_eis_srvy_l2_electronenergy_ssd5]
      
      
      Valid Events Processed per second MMS4 [mms4_epd_eis_srvy_l2_electronenergy_vep]
      
      
      Valid Electron Events per second MMS4 [mms4_epd_eis_srvy_l2_electronenergy_vee]
      
      
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MMS4_EPD-EIS_SRVY_L2_EXTOF (spase://NASA/NumericalData/MMS/4/EnergeticParticleDetector/EIS/Survey/Level2/EnergyByTimeOfFlight/PT2.42S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms4_epd_eis_srvy_l2_extof_duration]
      
      
      ---> Instrument Deadtime [mms4_epd_eis_srvy_l2_extof_deadtime]
      
      
      ---> Instrument Large Pixel in Use [mms4_epd_eis_srvy_l2_extof_largepixel]
      
      
      ---> Spin [mms4_epd_eis_srvy_l2_extof_spin]
      
      
      ---> Sector [mms4_epd_eis_srvy_l2_extof_sector]
      
      
      ---> Quality Word [mms4_epd_eis_srvy_l2_extof_quality]
      
      
      MMS4 ExTOF-Survey proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_extof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms4_epd_eis_srvy_l2_extof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms4_epd_eis_srvy_l2_extof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms4_epd_eis_srvy_l2_extof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms4_epd_eis_srvy_l2_extof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms4_epd_eis_srvy_l2_extof_proton_P6_counts_t5]
      
      
      MMS4 ExTOF-Survey proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_extof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms4_epd_eis_srvy_l2_extof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms4_epd_eis_srvy_l2_extof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms4_epd_eis_srvy_l2_extof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms4_epd_eis_srvy_l2_extof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms4_epd_eis_srvy_l2_extof_proton_P6_cps_t5]
      
      
      MMS4 ExTOF-Survey proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_extof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms4_epd_eis_srvy_l2_extof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms4_epd_eis_srvy_l2_extof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms4_epd_eis_srvy_l2_extof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms4_epd_eis_srvy_l2_extof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms4_epd_eis_srvy_l2_extof_proton_P6_flux_t5]
      
      
      MMS4 ExTOF-Survey helium_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_extof_helium_P6_counts_t0]
      
      
      ---> helium_P6_counts_t1 [mms4_epd_eis_srvy_l2_extof_helium_P6_counts_t1]
      
      
      ---> helium_P6_counts_t2 [mms4_epd_eis_srvy_l2_extof_helium_P6_counts_t2]
      
      
      ---> helium_P6_counts_t3 [mms4_epd_eis_srvy_l2_extof_helium_P6_counts_t3]
      
      
      ---> helium_P6_counts_t4 [mms4_epd_eis_srvy_l2_extof_helium_P6_counts_t4]
      
      
      ---> helium_P6_counts_t5 [mms4_epd_eis_srvy_l2_extof_helium_P6_counts_t5]
      
      
      MMS4 ExTOF-Survey helium_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_extof_helium_P6_cps_t0]
      
      
      ---> helium_P6_cps_t1 [mms4_epd_eis_srvy_l2_extof_helium_P6_cps_t1]
      
      
      ---> helium_P6_cps_t2 [mms4_epd_eis_srvy_l2_extof_helium_P6_cps_t2]
      
      
      ---> helium_P6_cps_t3 [mms4_epd_eis_srvy_l2_extof_helium_P6_cps_t3]
      
      
      ---> helium_P6_cps_t4 [mms4_epd_eis_srvy_l2_extof_helium_P6_cps_t4]
      
      
      ---> helium_P6_cps_t5 [mms4_epd_eis_srvy_l2_extof_helium_P6_cps_t5]
      
      
      MMS4 ExTOF-Survey helium_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_extof_helium_P6_flux_t0]
      
      
      ---> helium_P6_flux_t1 [mms4_epd_eis_srvy_l2_extof_helium_P6_flux_t1]
      
      
      ---> helium_P6_flux_t2 [mms4_epd_eis_srvy_l2_extof_helium_P6_flux_t2]
      
      
      ---> helium_P6_flux_t3 [mms4_epd_eis_srvy_l2_extof_helium_P6_flux_t3]
      
      
      ---> helium_P6_flux_t4 [mms4_epd_eis_srvy_l2_extof_helium_P6_flux_t4]
      
      
      ---> helium_P6_flux_t5 [mms4_epd_eis_srvy_l2_extof_helium_P6_flux_t5]
      
      
      MMS4 ExTOF-Survey oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_extof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_counts_t5]
      
      
      MMS4 ExTOF-Survey oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_extof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_cps_t5]
      
      
      MMS4 ExTOF-Survey oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_extof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms4_epd_eis_srvy_l2_extof_oxygen_P6_flux_t5]
      
      
      MMS4 ExTOF-Survey dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_extof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms4_epd_eis_srvy_l2_extof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms4_epd_eis_srvy_l2_extof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms4_epd_eis_srvy_l2_extof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms4_epd_eis_srvy_l2_extof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms4_epd_eis_srvy_l2_extof_dump_P6_counts_t5]
      
      
      MMS4 ExTOF-Survey dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_extof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms4_epd_eis_srvy_l2_extof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms4_epd_eis_srvy_l2_extof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms4_epd_eis_srvy_l2_extof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms4_epd_eis_srvy_l2_extof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms4_epd_eis_srvy_l2_extof_dump_P6_cps_t5]
      
      
      MMS4 ExTOF-Survey dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_extof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms4_epd_eis_srvy_l2_extof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms4_epd_eis_srvy_l2_extof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms4_epd_eis_srvy_l2_extof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms4_epd_eis_srvy_l2_extof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms4_epd_eis_srvy_l2_extof_dump_P6_flux_t5]
      
      
      MMS4 ExTOF-Survey proton_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms4_epd_eis_srvy_l2_extof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms4_epd_eis_srvy_l2_extof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms4_epd_eis_srvy_l2_extof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms4_epd_eis_srvy_l2_extof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms4_epd_eis_srvy_l2_extof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms4_epd_eis_srvy_l2_extof_proton_P5_counts_t5]
      
      
      MMS4 ExTOF-Survey proton_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms4_epd_eis_srvy_l2_extof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms4_epd_eis_srvy_l2_extof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms4_epd_eis_srvy_l2_extof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms4_epd_eis_srvy_l2_extof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms4_epd_eis_srvy_l2_extof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms4_epd_eis_srvy_l2_extof_proton_P5_cps_t5]
      
      
      MMS4 ExTOF-Survey proton_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms4_epd_eis_srvy_l2_extof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms4_epd_eis_srvy_l2_extof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms4_epd_eis_srvy_l2_extof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms4_epd_eis_srvy_l2_extof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms4_epd_eis_srvy_l2_extof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms4_epd_eis_srvy_l2_extof_proton_P5_flux_t5]
      
      
      MMS4 ExTOF-Survey oxygen_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms4_epd_eis_srvy_l2_extof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_counts_t5]
      
      
      MMS4 ExTOF-Survey oxygen_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms4_epd_eis_srvy_l2_extof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_cps_t5]
      
      
      MMS4 ExTOF-Survey oxygen_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms4_epd_eis_srvy_l2_extof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms4_epd_eis_srvy_l2_extof_oxygen_P5_flux_t5]
      
      
      MMS4 ExTOF-Survey helium_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms4_epd_eis_srvy_l2_extof_helium_P5_counts_t0]
      
      
      ---> helium_P5_counts_t1 [mms4_epd_eis_srvy_l2_extof_helium_P5_counts_t1]
      
      
      ---> helium_P5_counts_t2 [mms4_epd_eis_srvy_l2_extof_helium_P5_counts_t2]
      
      
      ---> helium_P5_counts_t3 [mms4_epd_eis_srvy_l2_extof_helium_P5_counts_t3]
      
      
      ---> helium_P5_counts_t4 [mms4_epd_eis_srvy_l2_extof_helium_P5_counts_t4]
      
      
      ---> helium_P5_counts_t5 [mms4_epd_eis_srvy_l2_extof_helium_P5_counts_t5]
      
      
      MMS4 ExTOF-Survey helium_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms4_epd_eis_srvy_l2_extof_helium_P5_cps_t0]
      
      
      ---> helium_P5_cps_t1 [mms4_epd_eis_srvy_l2_extof_helium_P5_cps_t1]
      
      
      ---> helium_P5_cps_t2 [mms4_epd_eis_srvy_l2_extof_helium_P5_cps_t2]
      
      
      ---> helium_P5_cps_t3 [mms4_epd_eis_srvy_l2_extof_helium_P5_cps_t3]
      
      
      ---> helium_P5_cps_t4 [mms4_epd_eis_srvy_l2_extof_helium_P5_cps_t4]
      
      
      ---> helium_P5_cps_t5 [mms4_epd_eis_srvy_l2_extof_helium_P5_cps_t5]
      
      
      MMS4 ExTOF-Survey helium_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms4_epd_eis_srvy_l2_extof_helium_P5_flux_t0]
      
      
      ---> helium_P5_flux_t1 [mms4_epd_eis_srvy_l2_extof_helium_P5_flux_t1]
      
      
      ---> helium_P5_flux_t2 [mms4_epd_eis_srvy_l2_extof_helium_P5_flux_t2]
      
      
      ---> helium_P5_flux_t3 [mms4_epd_eis_srvy_l2_extof_helium_P5_flux_t3]
      
      
      ---> helium_P5_flux_t4 [mms4_epd_eis_srvy_l2_extof_helium_P5_flux_t4]
      
      
      ---> helium_P5_flux_t5 [mms4_epd_eis_srvy_l2_extof_helium_P5_flux_t5]
      
      
      MMS4 ExTOF-Survey proton_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms4_epd_eis_srvy_l2_extof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms4_epd_eis_srvy_l2_extof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms4_epd_eis_srvy_l2_extof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms4_epd_eis_srvy_l2_extof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms4_epd_eis_srvy_l2_extof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms4_epd_eis_srvy_l2_extof_proton_P4_counts_t5]
      
      
      MMS4 ExTOF-Survey proton_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms4_epd_eis_srvy_l2_extof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms4_epd_eis_srvy_l2_extof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms4_epd_eis_srvy_l2_extof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms4_epd_eis_srvy_l2_extof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms4_epd_eis_srvy_l2_extof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms4_epd_eis_srvy_l2_extof_proton_P4_cps_t5]
      
      
      MMS4 ExTOF-Survey proton_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms4_epd_eis_srvy_l2_extof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms4_epd_eis_srvy_l2_extof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms4_epd_eis_srvy_l2_extof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms4_epd_eis_srvy_l2_extof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms4_epd_eis_srvy_l2_extof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms4_epd_eis_srvy_l2_extof_proton_P4_flux_t5]
      
      
      MMS4 ExTOF-Survey alpha_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms4_epd_eis_srvy_l2_extof_helium_P4_counts_t0]
      
      
      ---> alpha_P4_counts_t1 [mms4_epd_eis_srvy_l2_extof_helium_P4_counts_t1]
      
      
      ---> alpha_P4_counts_t2 [mms4_epd_eis_srvy_l2_extof_helium_P4_counts_t2]
      
      
      ---> alpha_P4_counts_t3 [mms4_epd_eis_srvy_l2_extof_helium_P4_counts_t3]
      
      
      ---> alpha_P4_counts_t4 [mms4_epd_eis_srvy_l2_extof_helium_P4_counts_t4]
      
      
      ---> alpha_P4_counts_t5 [mms4_epd_eis_srvy_l2_extof_helium_P4_counts_t5]
      
      
      MMS4 ExTOF-Survey alpha_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms4_epd_eis_srvy_l2_extof_helium_P4_cps_t0]
      
      
      ---> alpha_P4_cps_t1 [mms4_epd_eis_srvy_l2_extof_helium_P4_cps_t1]
      
      
      ---> alpha_P4_cps_t2 [mms4_epd_eis_srvy_l2_extof_helium_P4_cps_t2]
      
      
      ---> alpha_P4_cps_t3 [mms4_epd_eis_srvy_l2_extof_helium_P4_cps_t3]
      
      
      ---> alpha_P4_cps_t4 [mms4_epd_eis_srvy_l2_extof_helium_P4_cps_t4]
      
      
      ---> alpha_P4_cps_t5 [mms4_epd_eis_srvy_l2_extof_helium_P4_cps_t5]
      
      
      MMS4 ExTOF-Survey alpha_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms4_epd_eis_srvy_l2_extof_helium_P4_flux_t0]
      
      
      ---> alpha_P4_flux_t1 [mms4_epd_eis_srvy_l2_extof_helium_P4_flux_t1]
      
      
      ---> alpha_P4_flux_t2 [mms4_epd_eis_srvy_l2_extof_helium_P4_flux_t2]
      
      
      ---> alpha_P4_flux_t3 [mms4_epd_eis_srvy_l2_extof_helium_P4_flux_t3]
      
      
      ---> alpha_P4_flux_t4 [mms4_epd_eis_srvy_l2_extof_helium_P4_flux_t4]
      
      
      ---> alpha_P4_flux_t5 [mms4_epd_eis_srvy_l2_extof_helium_P4_flux_t5]
      
      
      MMS4 ExTOF-Survey oxygen_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms4_epd_eis_srvy_l2_extof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_counts_t5]
      
      
      MMS4 ExTOF-Survey oxygen_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms4_epd_eis_srvy_l2_extof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_cps_t5]
      
      
      MMS4 ExTOF-Survey oxygen_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms4_epd_eis_srvy_l2_extof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms4_epd_eis_srvy_l2_extof_oxygen_P4_flux_t5]
      
      
      MMS4 ExTOF-Survey proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_extof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms4_epd_eis_srvy_l2_extof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms4_epd_eis_srvy_l2_extof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms4_epd_eis_srvy_l2_extof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms4_epd_eis_srvy_l2_extof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms4_epd_eis_srvy_l2_extof_proton_P3_counts_t5]
      
      
      MMS4 ExTOF-Survey proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_extof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms4_epd_eis_srvy_l2_extof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms4_epd_eis_srvy_l2_extof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms4_epd_eis_srvy_l2_extof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms4_epd_eis_srvy_l2_extof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms4_epd_eis_srvy_l2_extof_proton_P3_cps_t5]
      
      
      MMS4 ExTOF-Survey proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_extof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms4_epd_eis_srvy_l2_extof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms4_epd_eis_srvy_l2_extof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms4_epd_eis_srvy_l2_extof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms4_epd_eis_srvy_l2_extof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms4_epd_eis_srvy_l2_extof_proton_P3_flux_t5]
      
      
      MMS4 ExTOF-Survey alpha_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_extof_helium_P3_counts_t0]
      
      
      ---> alpha_P3_counts_t1 [mms4_epd_eis_srvy_l2_extof_helium_P3_counts_t1]
      
      
      ---> alpha_P3_counts_t2 [mms4_epd_eis_srvy_l2_extof_helium_P3_counts_t2]
      
      
      ---> alpha_P3_counts_t3 [mms4_epd_eis_srvy_l2_extof_helium_P3_counts_t3]
      
      
      ---> alpha_P3_counts_t4 [mms4_epd_eis_srvy_l2_extof_helium_P3_counts_t4]
      
      
      ---> alpha_P3_counts_t5 [mms4_epd_eis_srvy_l2_extof_helium_P3_counts_t5]
      
      
      MMS4 ExTOF-Survey alpha_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_extof_helium_P3_cps_t0]
      
      
      ---> alpha_P3_cps_t1 [mms4_epd_eis_srvy_l2_extof_helium_P3_cps_t1]
      
      
      ---> alpha_P3_cps_t2 [mms4_epd_eis_srvy_l2_extof_helium_P3_cps_t2]
      
      
      ---> alpha_P3_cps_t3 [mms4_epd_eis_srvy_l2_extof_helium_P3_cps_t3]
      
      
      ---> alpha_P3_cps_t4 [mms4_epd_eis_srvy_l2_extof_helium_P3_cps_t4]
      
      
      ---> alpha_P3_cps_t5 [mms4_epd_eis_srvy_l2_extof_helium_P3_cps_t5]
      
      
      MMS4 ExTOF-Survey alpha_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_extof_helium_P3_flux_t0]
      
      
      ---> alpha_P3_flux_t1 [mms4_epd_eis_srvy_l2_extof_helium_P3_flux_t1]
      
      
      ---> alpha_P3_flux_t2 [mms4_epd_eis_srvy_l2_extof_helium_P3_flux_t2]
      
      
      ---> alpha_P3_flux_t3 [mms4_epd_eis_srvy_l2_extof_helium_P3_flux_t3]
      
      
      ---> alpha_P3_flux_t4 [mms4_epd_eis_srvy_l2_extof_helium_P3_flux_t4]
      
      
      ---> alpha_P3_flux_t5 [mms4_epd_eis_srvy_l2_extof_helium_P3_flux_t5]
      
      
      MMS4 ExTOF-Survey oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_extof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_counts_t5]
      
      
      MMS4 ExTOF-Survey oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_extof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_cps_t5]
      
      
      MMS4 ExTOF-Survey oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_extof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms4_epd_eis_srvy_l2_extof_oxygen_P3_flux_t5]
      
      
      MMS4 ExTOF-Survey dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_extof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms4_epd_eis_srvy_l2_extof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms4_epd_eis_srvy_l2_extof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms4_epd_eis_srvy_l2_extof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms4_epd_eis_srvy_l2_extof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms4_epd_eis_srvy_l2_extof_dump_P3_counts_t5]
      
      
      MMS4 ExTOF-Survey dump_P4_counts_t0 [data available from 2016/09/29 to 2020/02/03] [mms4_epd_eis_srvy_l2_extof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms4_epd_eis_srvy_l2_extof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms4_epd_eis_srvy_l2_extof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms4_epd_eis_srvy_l2_extof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms4_epd_eis_srvy_l2_extof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms4_epd_eis_srvy_l2_extof_dump_P4_counts_t5]
      
      
      MMS4 ExTOF-Survey dump_P5_counts_t0 [data available from 2020/02/04 to 2025/01/06] [mms4_epd_eis_srvy_l2_extof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms4_epd_eis_srvy_l2_extof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms4_epd_eis_srvy_l2_extof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms4_epd_eis_srvy_l2_extof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms4_epd_eis_srvy_l2_extof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms4_epd_eis_srvy_l2_extof_dump_P5_counts_t5]
      
      
      MMS4 ExTOF-Survey dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_extof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms4_epd_eis_srvy_l2_extof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms4_epd_eis_srvy_l2_extof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms4_epd_eis_srvy_l2_extof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms4_epd_eis_srvy_l2_extof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms4_epd_eis_srvy_l2_extof_dump_P3_cps_t5]
      
      
      MMS4 ExTOF-Survey dump_P4_cps_t0 [data available from 2016/09/29 to 2020/02/03] [mms4_epd_eis_srvy_l2_extof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms4_epd_eis_srvy_l2_extof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms4_epd_eis_srvy_l2_extof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms4_epd_eis_srvy_l2_extof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms4_epd_eis_srvy_l2_extof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms4_epd_eis_srvy_l2_extof_dump_P4_cps_t5]
      
      
      MMS4 ExTOF-Survey dump_P5_cps_t0 [data available from 2020/02/04 to 2025/01/06] [mms4_epd_eis_srvy_l2_extof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms4_epd_eis_srvy_l2_extof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms4_epd_eis_srvy_l2_extof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms4_epd_eis_srvy_l2_extof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms4_epd_eis_srvy_l2_extof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms4_epd_eis_srvy_l2_extof_dump_P5_cps_t5]
      
      
      MMS4 ExTOF-Survey dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_extof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms4_epd_eis_srvy_l2_extof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms4_epd_eis_srvy_l2_extof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms4_epd_eis_srvy_l2_extof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms4_epd_eis_srvy_l2_extof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms4_epd_eis_srvy_l2_extof_dump_P3_flux_t5]
      
      
      MMS4 ExTOF-Survey dump_P4_flux_t0 [data available from 2016/09/29 to 2020/02/03] [mms4_epd_eis_srvy_l2_extof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms4_epd_eis_srvy_l2_extof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms4_epd_eis_srvy_l2_extof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms4_epd_eis_srvy_l2_extof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms4_epd_eis_srvy_l2_extof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms4_epd_eis_srvy_l2_extof_dump_P4_flux_t5]
      
      
      MMS4 ExTOF-Survey dump_P5_flux_t0 [data available from 2020/02/04 to 2025/01/06] [mms4_epd_eis_srvy_l2_extof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms4_epd_eis_srvy_l2_extof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms4_epd_eis_srvy_l2_extof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms4_epd_eis_srvy_l2_extof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms4_epd_eis_srvy_l2_extof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms4_epd_eis_srvy_l2_extof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS4 [mms4_epd_eis_srvy_l2_extof_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS4 [mms4_epd_eis_srvy_l2_extof_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS4 [mms4_epd_eis_srvy_l2_extof_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS4 [mms4_epd_eis_srvy_l2_extof_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS4 [mms4_epd_eis_srvy_l2_extof_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS4 [mms4_epd_eis_srvy_l2_extof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS4 [mms4_epd_eis_srvy_l2_extof_look_t0]
      
      
      Look Direction for Telescope 1 MMS4 [mms4_epd_eis_srvy_l2_extof_look_t1]
      
      
      Look Direction for Telescope 2 MMS4 [mms4_epd_eis_srvy_l2_extof_look_t2]
      
      
      Look Direction for Telescope 3 MMS4 [mms4_epd_eis_srvy_l2_extof_look_t3]
      
      
      Look Direction for Telescope 4 MMS4 [mms4_epd_eis_srvy_l2_extof_look_t4]
      
      
      Look Direction for Telescope 5 MMS4 [mms4_epd_eis_srvy_l2_extof_look_t5]
      
      
      Magnetic Field BCS MMS4 [mms4_epd_eis_srvy_l2_extof_b]
      
      
      Spacecraft position GSE MMS4 [mms4_epd_eis_srvy_l2_extof_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS4 [mms4_epd_eis_srvy_l2_extof_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS4 [mms4_epd_eis_srvy_l2_extof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS4 [mms4_epd_eis_srvy_l2_extof_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS4 [mms4_epd_eis_srvy_l2_extof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS4 [mms4_epd_eis_srvy_l2_extof_r]
      
      
      Dipole L-shell MMS4 [mms4_epd_eis_srvy_l2_extof_l]
      
      
      Latitude in GSE Frame MMS4 [mms4_epd_eis_srvy_l2_extof_gse_lat]
      
      
      Longitude in GSE Frame MMS4 [mms4_epd_eis_srvy_l2_extof_gse_lon]
      
      
      Latitude in GSM Frame MMS4 [mms4_epd_eis_srvy_l2_extof_gsm_lat]
      
      
      Longitude in GSM Frame MMS4 [mms4_epd_eis_srvy_l2_extof_gsm_lon]
      
      
      Latitude in SM Frame MMS4 [mms4_epd_eis_srvy_l2_extof_sm_lat]
      
      
      Longitude in SM Frame MMS4 [mms4_epd_eis_srvy_l2_extof_sm_lon]
      
      
      Orbit number MMS4 [mms4_epd_eis_srvy_l2_extof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS4 [mms4_epd_eis_srvy_l2_extof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS4 [mms4_epd_eis_srvy_l2_extof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS4 [mms4_epd_eis_srvy_l2_extof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS4 [mms4_epd_eis_srvy_l2_extof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS4 [mms4_epd_eis_srvy_l2_extof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS4 [mms4_epd_eis_srvy_l2_extof_ssd5]
      
      
      Valid Events Processed per second MMS4 [mms4_epd_eis_srvy_l2_extof_vep]
      
      
      Start 0 Anode Count Rate MMS4 [mms4_epd_eis_srvy_l2_extof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS4 [mms4_epd_eis_srvy_l2_extof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS4 [mms4_epd_eis_srvy_l2_extof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS4 [mms4_epd_eis_srvy_l2_extof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS4 [mms4_epd_eis_srvy_l2_extof_vtofxphe]
      
      
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MMS4_EPD-EIS_SRVY_L2_PHXTOF (spase://NASA/NumericalData/MMS/4/EnergeticParticleDetector/EIS/Survey/Level2/PulseHeightByTimeOfFlight/PT2.42S)
Description
empty
Modification History
Constantly modifying this code
 
  • Data Variable Descriptions
      Total Exposure Time for Accumulation [mms4_epd_eis_srvy_l2_phxtof_duration]
      
      
      Instrument Deadtime [mms4_epd_eis_srvy_l2_phxtof_deadtime]
      
      
      Instrument Large Pixel in Use [mms4_epd_eis_srvy_l2_phxtof_largepixel]
      
      
      Spin [mms4_epd_eis_srvy_l2_phxtof_spin]
      
      
      Sector [mms4_epd_eis_srvy_l2_phxtof_sector]
      
      
      Quality Word [mms4_epd_eis_srvy_l2_phxtof_quality]
      
      
      MMS4 PhxTOF-Survey proton_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_proton_P6_counts_t0]
      
      
      ---> proton_P6_counts_t1 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_counts_t1]
      
      
      ---> proton_P6_counts_t2 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_counts_t2]
      
      
      ---> proton_P6_counts_t3 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_counts_t3]
      
      
      ---> proton_P6_counts_t4 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_counts_t4]
      
      
      ---> proton_P6_counts_t5 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_counts_t5]
      
      
      MMS4 PhxTOF-Survey proton_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_proton_P6_cps_t0]
      
      
      ---> proton_P6_cps_t1 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_cps_t1]
      
      
      ---> proton_P6_cps_t2 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_cps_t2]
      
      
      ---> proton_P6_cps_t3 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_cps_t3]
      
      
      ---> proton_P6_cps_t4 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_cps_t4]
      
      
      ---> proton_P6_cps_t5 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_cps_t5]
      
      
      MMS4 PhxTOF-Survey proton_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_proton_P6_flux_t0]
      
      
      ---> proton_P6_flux_t1 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_flux_t1]
      
      
      ---> proton_P6_flux_t2 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_flux_t2]
      
      
      ---> proton_P6_flux_t3 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_flux_t3]
      
      
      ---> proton_P6_flux_t4 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_flux_t4]
      
      
      ---> proton_P6_flux_t5 [mms4_epd_eis_srvy_l2_phxtof_proton_P6_flux_t5]
      
      
      MMS4 PhxTOF-Survey oxygen_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t0]
      
      
      ---> oxygen_P6_counts_t1 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t1]
      
      
      ---> oxygen_P6_counts_t2 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t2]
      
      
      ---> oxygen_P6_counts_t3 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t3]
      
      
      ---> oxygen_P6_counts_t4 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t4]
      
      
      ---> oxygen_P6_counts_t5 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_counts_t5]
      
      
      MMS4 PhxTOF-Survey oxygen_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t0]
      
      
      ---> oxygen_P6_cps_t1 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t1]
      
      
      ---> oxygen_P6_cps_t2 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t2]
      
      
      ---> oxygen_P6_cps_t3 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t3]
      
      
      ---> oxygen_P6_cps_t4 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t4]
      
      
      ---> oxygen_P6_cps_t5 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_cps_t5]
      
      
      MMS4 PhxTOF-Survey oxygen_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t0]
      
      
      ---> oxygen_P6_flux_t1 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t1]
      
      
      ---> oxygen_P6_flux_t2 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t2]
      
      
      ---> oxygen_P6_flux_t3 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t3]
      
      
      ---> oxygen_P6_flux_t4 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t4]
      
      
      ---> oxygen_P6_flux_t5 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P6_flux_t5]
      
      
      MMS4 PhxTOF-Survey dump_P6_counts_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_dump_P6_counts_t0]
      
      
      ---> dump_P6_counts_t1 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_counts_t1]
      
      
      ---> dump_P6_counts_t2 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_counts_t2]
      
      
      ---> dump_P6_counts_t3 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_counts_t3]
      
      
      ---> dump_P6_counts_t4 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_counts_t4]
      
      
      ---> dump_P6_counts_t5 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_counts_t5]
      
      
      MMS4 PhxTOF-Survey dump_P6_cps_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_dump_P6_cps_t0]
      
      
      ---> dump_P6_cps_t1 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_cps_t1]
      
      
      ---> dump_P6_cps_t2 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_cps_t2]
      
      
      ---> dump_P6_cps_t3 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_cps_t3]
      
      
      ---> dump_P6_cps_t4 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_cps_t4]
      
      
      ---> dump_P6_cps_t5 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_cps_t5]
      
      
      MMS4 PhxTOF-Survey dump_P6_flux_t0 [data available beginning on 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_dump_P6_flux_t0]
      
      
      ---> dump_P6_flux_t1 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_flux_t1]
      
      
      ---> dump_P6_flux_t2 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_flux_t2]
      
      
      ---> dump_P6_flux_t3 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_flux_t3]
      
      
      ---> dump_P6_flux_t4 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_flux_t4]
      
      
      ---> dump_P6_flux_t5 [mms4_epd_eis_srvy_l2_phxtof_dump_P6_flux_t5]
      
      
      MMS4 PhxTOF-Survey proton_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_proton_P5_counts_t0]
      
      
      ---> proton_P5_counts_t1 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_counts_t1]
      
      
      ---> proton_P5_counts_t2 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_counts_t2]
      
      
      ---> proton_P5_counts_t3 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_counts_t3]
      
      
      ---> proton_P5_counts_t4 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_counts_t4]
      
      
      ---> proton_P5_counts_t5 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_counts_t5]
      
      
      MMS4 PhxTOF-Survey proton_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_proton_P5_cps_t0]
      
      
      ---> proton_P5_cps_t1 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_cps_t1]
      
      
      ---> proton_P5_cps_t2 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_cps_t2]
      
      
      ---> proton_P5_cps_t3 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_cps_t3]
      
      
      ---> proton_P5_cps_t4 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_cps_t4]
      
      
      ---> proton_P5_cps_t5 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_cps_t5]
      
      
      MMS4 PhxTOF-Survey proton_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_proton_P5_flux_t0]
      
      
      ---> proton_P5_flux_t1 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_flux_t1]
      
      
      ---> proton_P5_flux_t2 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_flux_t2]
      
      
      ---> proton_P5_flux_t3 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_flux_t3]
      
      
      ---> proton_P5_flux_t4 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_flux_t4]
      
      
      ---> proton_P5_flux_t5 [mms4_epd_eis_srvy_l2_phxtof_proton_P5_flux_t5]
      
      
      MMS4 PhxTOF-Survey oxygen_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t0]
      
      
      ---> oxygen_P5_counts_t1 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t1]
      
      
      ---> oxygen_P5_counts_t2 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t2]
      
      
      ---> oxygen_P5_counts_t3 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t3]
      
      
      ---> oxygen_P5_counts_t4 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t4]
      
      
      ---> oxygen_P5_counts_t5 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_counts_t5]
      
      
      MMS4 PhxTOF-Survey oxygen_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t0]
      
      
      ---> oxygen_P5_cps_t1 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t1]
      
      
      ---> oxygen_P5_cps_t2 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t2]
      
      
      ---> oxygen_P5_cps_t3 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t3]
      
      
      ---> oxygen_P5_cps_t4 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t4]
      
      
      ---> oxygen_P5_cps_t5 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_cps_t5]
      
      
      MMS4 PhxTOF-Survey oxygen_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t0]
      
      
      ---> oxygen_P5_flux_t1 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t1]
      
      
      ---> oxygen_P5_flux_t2 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t2]
      
      
      ---> oxygen_P5_flux_t3 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t3]
      
      
      ---> oxygen_P5_flux_t4 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t4]
      
      
      ---> oxygen_P5_flux_t5 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P5_flux_t5]
      
      
      MMS4 PhxTOF-Survey proton_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_phxtof_proton_P4_counts_t0]
      
      
      ---> proton_P4_counts_t1 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_counts_t1]
      
      
      ---> proton_P4_counts_t2 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_counts_t2]
      
      
      ---> proton_P4_counts_t3 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_counts_t3]
      
      
      ---> proton_P4_counts_t4 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_counts_t4]
      
      
      ---> proton_P4_counts_t5 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_counts_t5]
      
      
      MMS4 PhxTOF-Survey proton_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_phxtof_proton_P4_cps_t0]
      
      
      ---> proton_P4_cps_t1 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_cps_t1]
      
      
      ---> proton_P4_cps_t2 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_cps_t2]
      
      
      ---> proton_P4_cps_t3 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_cps_t3]
      
      
      ---> proton_P4_cps_t4 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_cps_t4]
      
      
      ---> proton_P4_cps_t5 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_cps_t5]
      
      
      MMS4 PhxTOF-Survey proton_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_phxtof_proton_P4_flux_t0]
      
      
      ---> proton_P4_flux_t1 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_flux_t1]
      
      
      ---> proton_P4_flux_t2 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_flux_t2]
      
      
      ---> proton_P4_flux_t3 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_flux_t3]
      
      
      ---> proton_P4_flux_t4 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_flux_t4]
      
      
      ---> proton_P4_flux_t5 [mms4_epd_eis_srvy_l2_phxtof_proton_P4_flux_t5]
      
      
      MMS4 PhxTOF-Survey oxygen_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t0]
      
      
      ---> oxygen_P4_counts_t1 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t1]
      
      
      ---> oxygen_P4_counts_t2 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t2]
      
      
      ---> oxygen_P4_counts_t3 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t3]
      
      
      ---> oxygen_P4_counts_t4 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t4]
      
      
      ---> oxygen_P4_counts_t5 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_counts_t5]
      
      
      MMS4 PhxTOF-Survey oxygen_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t0]
      
      
      ---> oxygen_P4_cps_t1 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t1]
      
      
      ---> oxygen_P4_cps_t2 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t2]
      
      
      ---> oxygen_P4_cps_t3 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t3]
      
      
      ---> oxygen_P4_cps_t4 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t4]
      
      
      ---> oxygen_P4_cps_t5 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_cps_t5]
      
      
      MMS4 PhxTOF-Survey oxygen_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t0]
      
      
      ---> oxygen_P4_flux_t1 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t1]
      
      
      ---> oxygen_P4_flux_t2 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t2]
      
      
      ---> oxygen_P4_flux_t3 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t3]
      
      
      ---> oxygen_P4_flux_t4 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t4]
      
      
      ---> oxygen_P4_flux_t5 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P4_flux_t5]
      
      
      MMS4 PhxTOF-Survey proton_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_phxtof_proton_P3_counts_t0]
      
      
      ---> proton_P3_counts_t1 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_counts_t1]
      
      
      ---> proton_P3_counts_t2 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_counts_t2]
      
      
      ---> proton_P3_counts_t3 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_counts_t3]
      
      
      ---> proton_P3_counts_t4 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_counts_t4]
      
      
      ---> proton_P3_counts_t5 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_counts_t5]
      
      
      MMS4 PhxTOF-Survey proton_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_phxtof_proton_P3_cps_t0]
      
      
      ---> proton_P3_cps_t1 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_cps_t1]
      
      
      ---> proton_P3_cps_t2 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_cps_t2]
      
      
      ---> proton_P3_cps_t3 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_cps_t3]
      
      
      ---> proton_P3_cps_t4 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_cps_t4]
      
      
      ---> proton_P3_cps_t5 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_cps_t5]
      
      
      MMS4 PhxTOF-Survey proton_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_phxtof_proton_P3_flux_t0]
      
      
      ---> proton_P3_flux_t1 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_flux_t1]
      
      
      ---> proton_P3_flux_t2 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_flux_t2]
      
      
      ---> proton_P3_flux_t3 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_flux_t3]
      
      
      ---> proton_P3_flux_t4 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_flux_t4]
      
      
      ---> proton_P3_flux_t5 [mms4_epd_eis_srvy_l2_phxtof_proton_P3_flux_t5]
      
      
      MMS4 PhxTOF-Survey oxygen_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t0]
      
      
      ---> oxygen_P3_counts_t1 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t1]
      
      
      ---> oxygen_P3_counts_t2 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t2]
      
      
      ---> oxygen_P3_counts_t3 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t3]
      
      
      ---> oxygen_P3_counts_t4 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t4]
      
      
      ---> oxygen_P3_counts_t5 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_counts_t5]
      
      
      MMS4 PhxTOF-Survey oxygen_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t0]
      
      
      ---> oxygen_P3_cps_t1 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t1]
      
      
      ---> oxygen_P3_cps_t2 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t2]
      
      
      ---> oxygen_P3_cps_t3 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t3]
      
      
      ---> oxygen_P3_cps_t4 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t4]
      
      
      ---> oxygen_P3_cps_t5 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_cps_t5]
      
      
      MMS4 PhxTOF-Survey oxygen_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t0]
      
      
      ---> oxygen_P3_flux_t1 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t1]
      
      
      ---> oxygen_P3_flux_t2 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t2]
      
      
      ---> oxygen_P3_flux_t3 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t3]
      
      
      ---> oxygen_P3_flux_t4 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t4]
      
      
      ---> oxygen_P3_flux_t5 [mms4_epd_eis_srvy_l2_phxtof_oxygen_P3_flux_t5]
      
      
      MMS4 PhxTOF-Survey dump_P3_counts_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_phxtof_dump_P3_counts_t0]
      
      
      ---> dump_P3_counts_t1 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_counts_t1]
      
      
      ---> dump_P3_counts_t2 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_counts_t2]
      
      
      ---> dump_P3_counts_t3 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_counts_t3]
      
      
      ---> dump_P3_counts_t4 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_counts_t4]
      
      
      ---> dump_P3_counts_t5 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_counts_t5]
      
      
      MMS4 PhxTOF-Survey dump_P4_counts_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_phxtof_dump_P4_counts_t0]
      
      
      ---> dump_P4_counts_t1 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_counts_t1]
      
      
      ---> dump_P4_counts_t2 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_counts_t2]
      
      
      ---> dump_P4_counts_t3 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_counts_t3]
      
      
      ---> dump_P4_counts_t4 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_counts_t4]
      
      
      ---> dump_P4_counts_t5 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_counts_t5]
      
      
      MMS4 PhxTOF-Survey dump_P5_counts_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_dump_P5_counts_t0]
      
      
      ---> dump_P5_counts_t1 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_counts_t1]
      
      
      ---> dump_P5_counts_t2 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_counts_t2]
      
      
      ---> dump_P5_counts_t3 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_counts_t3]
      
      
      ---> dump_P5_counts_t4 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_counts_t4]
      
      
      ---> dump_P5_counts_t5 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_counts_t5]
      
      
      MMS4 PhxTOF-Survey dump_P3_cps_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_phxtof_dump_P3_cps_t0]
      
      
      ---> dump_P3_cps_t1 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_cps_t1]
      
      
      ---> dump_P3_cps_t2 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_cps_t2]
      
      
      ---> dump_P3_cps_t3 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_cps_t3]
      
      
      ---> dump_P3_cps_t4 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_cps_t4]
      
      
      ---> dump_P3_cps_t5 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_cps_t5]
      
      
      MMS4 PhxTOF-Survey dump_P4_cps_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_phxtof_dump_P4_cps_t0]
      
      
      ---> dump_P4_cps_t1 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_cps_t1]
      
      
      ---> dump_P4_cps_t2 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_cps_t2]
      
      
      ---> dump_P4_cps_t3 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_cps_t3]
      
      
      ---> dump_P4_cps_t4 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_cps_t4]
      
      
      ---> dump_P4_cps_t5 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_cps_t5]
      
      
      MMS4 PhxTOF-Survey dump_P5_cps_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_dump_P5_cps_t0]
      
      
      ---> dump_P5_cps_t1 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_cps_t1]
      
      
      ---> dump_P5_cps_t2 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_cps_t2]
      
      
      ---> dump_P5_cps_t3 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_cps_t3]
      
      
      ---> dump_P5_cps_t4 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_cps_t4]
      
      
      ---> dump_P5_cps_t5 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_cps_t5]
      
      
      MMS4 PhxTOF-Survey dump_P3_flux_t0 [data available from 2015/07/02 to 2016/09/28] [mms4_epd_eis_srvy_l2_phxtof_dump_P3_flux_t0]
      
      
      ---> dump_P3_flux_t1 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_flux_t1]
      
      
      ---> dump_P3_flux_t2 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_flux_t2]
      
      
      ---> dump_P3_flux_t3 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_flux_t3]
      
      
      ---> dump_P3_flux_t4 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_flux_t4]
      
      
      ---> dump_P3_flux_t5 [mms4_epd_eis_srvy_l2_phxtof_dump_P3_flux_t5]
      
      
      MMS4 PhxTOF-Survey dump_P4_flux_t0 [data available from 2016/09/29 to 2019/12/19] [mms4_epd_eis_srvy_l2_phxtof_dump_P4_flux_t0]
      
      
      ---> dump_P4_flux_t1 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_flux_t1]
      
      
      ---> dump_P4_flux_t2 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_flux_t2]
      
      
      ---> dump_P4_flux_t3 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_flux_t3]
      
      
      ---> dump_P4_flux_t4 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_flux_t4]
      
      
      ---> dump_P4_flux_t5 [mms4_epd_eis_srvy_l2_phxtof_dump_P4_flux_t5]
      
      
      MMS4 PhxTOF-Survey dump_P5_flux_t0 [data available from 2019/12/20 to 2025/01/06] [mms4_epd_eis_srvy_l2_phxtof_dump_P5_flux_t0]
      
      
      ---> dump_P5_flux_t1 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_flux_t1]
      
      
      ---> dump_P5_flux_t2 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_flux_t2]
      
      
      ---> dump_P5_flux_t3 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_flux_t3]
      
      
      ---> dump_P5_flux_t4 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_flux_t4]
      
      
      ---> dump_P5_flux_t5 [mms4_epd_eis_srvy_l2_phxtof_dump_P5_flux_t5]
      
      
      Pitch Angle for Telescope 0 MMS4 [mms4_epd_eis_srvy_l2_phxtof_pitch_angle_t0]
      
      
      Pitch Angle for Telescope 1 MMS4 [mms4_epd_eis_srvy_l2_phxtof_pitch_angle_t1]
      
      
      Pitch Angle for Telescope 2 MMS4 [mms4_epd_eis_srvy_l2_phxtof_pitch_angle_t2]
      
      
      Pitch Angle for Telescope 3 MMS4 [mms4_epd_eis_srvy_l2_phxtof_pitch_angle_t3]
      
      
      Pitch Angle for Telescope 4 MMS4 [mms4_epd_eis_srvy_l2_phxtof_pitch_angle_t4]
      
      
      Pitch Angle for Telescope 5 MMS4 [mms4_epd_eis_srvy_l2_phxtof_pitch_angle_t5]
      
      
      Look Direction for Telescope 0 MMS4 [mms4_epd_eis_srvy_l2_phxtof_look_t0]
      
      
      Look Direction for Telescope 1 MMS4 [mms4_epd_eis_srvy_l2_phxtof_look_t1]
      
      
      Look Direction for Telescope 2 MMS4 [mms4_epd_eis_srvy_l2_phxtof_look_t2]
      
      
      Look Direction for Telescope 3 MMS4 [mms4_epd_eis_srvy_l2_phxtof_look_t3]
      
      
      Look Direction for Telescope 4 MMS4 [mms4_epd_eis_srvy_l2_phxtof_look_t4]
      
      
      Look Direction for Telescope 5 MMS4 [mms4_epd_eis_srvy_l2_phxtof_look_t5]
      
      
      Magnetic Field BCS MMS4 [mms4_epd_eis_srvy_l2_phxtof_b]
      
      
      Spacecraft position GSE MMS4 [mms4_epd_eis_srvy_l2_phxtof_position_gse]
      
      
      Spacecraft position in GSM coordinates MMS4 [mms4_epd_eis_srvy_l2_phxtof_position_gsm]
      
      
      Spacecraft-Moon vector in GSE coordinates MMS4 [mms4_epd_eis_srvy_l2_phxtof_moon_gse]
      
      
      Transformation Matrix BCS to GSE Frame MMS4 [mms4_epd_eis_srvy_l2_phxtof_sc_to_gse]
      
      
      Transformation Matrix GSE to GSM Frame MMS4 [mms4_epd_eis_srvy_l2_phxtof_gse_to_gsm]
      
      
      Spacecraft Position: Radius MMS4 [mms4_epd_eis_srvy_l2_phxtof_r]
      
      
      Dipole L-shell MMS4 [mms4_epd_eis_srvy_l2_phxtof_l]
      
      
      Latitude in GSE Frame MMS4 [mms4_epd_eis_srvy_l2_phxtof_gse_lat]
      
      
      Longitude in GSE Frame MMS4 [mms4_epd_eis_srvy_l2_phxtof_gse_lon]
      
      
      Latitude in GSM Frame MMS4 [mms4_epd_eis_srvy_l2_phxtof_gsm_lat]
      
      
      Longitude in GSM Frame MMS4 [mms4_epd_eis_srvy_l2_phxtof_gsm_lon]
      
      
      Latitude in SM Frame MMS4 [mms4_epd_eis_srvy_l2_phxtof_sm_lat]
      
      
      Longitude in SM Frame MMS4 [mms4_epd_eis_srvy_l2_phxtof_sm_lon]
      
      
      Orbit number MMS4 [mms4_epd_eis_srvy_l2_phxtof_orbit_num]
      
      
      Solid State Energy Detector 0 Count Rate MMS4 [mms4_epd_eis_srvy_l2_phxtof_ssd0]
      
      
      Solid State Energy Detector 1 Count Rate MMS4 [mms4_epd_eis_srvy_l2_phxtof_ssd1]
      
      
      Solid State Energy Detector 2 Count Rate MMS4 [mms4_epd_eis_srvy_l2_phxtof_ssd2]
      
      
      Solid State Energy Detector 3 Count Rate MMS4 [mms4_epd_eis_srvy_l2_phxtof_ssd3]
      
      
      Solid State Energy Detector 4 Count Rate MMS4 [mms4_epd_eis_srvy_l2_phxtof_ssd4]
      
      
      Solid State Energy Detector 5 Count Rate MMS4 [mms4_epd_eis_srvy_l2_phxtof_ssd5]
      
      
      Valid Events Processed per second MMS4 [mms4_epd_eis_srvy_l2_phxtof_vep]
      
      
      Start 0 Anode Count Rate MMS4 [mms4_epd_eis_srvy_l2_phxtof_start0anode]
      
      
      Stop 0 Anode Count Rate MMS4 [mms4_epd_eis_srvy_l2_phxtof_stop0anode]
      
      
      Events above TOF Pulse Height Threshold MMS4 [mms4_epd_eis_srvy_l2_phxtof_pulseheight]
      
      
      Valid Time of Flight by Energy Events per second MMS4 [mms4_epd_eis_srvy_l2_phxtof_vtofxee]
      
      
      Valid Time of Flight by Pulse Height Energy Events per second MMS4 [mms4_epd_eis_srvy_l2_phxtof_vtofxphe]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS4_FEEPS_BRST_L2_ELECTRON (spase://NASA/NumericalData/MMS/4/EnergeticParticleDetector/FEEPS/Burst/Level2/Electron/PT0.3025S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms4_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms4_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms4_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms4_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms4_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms4_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms4_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms4_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms4_epd_feeps_brst_l2_electron_top_quality_indicator_sensorid_12]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms4_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms4_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms4_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms4_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms4_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms4_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms4_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms4_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms4_epd_feeps_brst_l2_electron_bottom_quality_indicator_sensorid_12]
      
      
      MMS4 FEEPS top side burst mode electron count rate sensor 1 [mms4_epd_feeps_brst_l2_electron_top_count_rate_sensorid_1]
      
      
      MMS4 FEEPS top side burst mode electron count rate sensor 2 [mms4_epd_feeps_brst_l2_electron_top_count_rate_sensorid_2]
      
      
      MMS4 FEEPS top side burst mode electron count rate sensor 3 [mms4_epd_feeps_brst_l2_electron_top_count_rate_sensorid_3]
      
      
      MMS4 FEEPS top side burst mode electron count rate sensor 4 [mms4_epd_feeps_brst_l2_electron_top_count_rate_sensorid_4]
      
      
      MMS4 FEEPS top side burst mode electron count rate sensor 5 [mms4_epd_feeps_brst_l2_electron_top_count_rate_sensorid_5]
      
      
      MMS4 FEEPS top side burst mode electron count rate sensor 9 [mms4_epd_feeps_brst_l2_electron_top_count_rate_sensorid_9]
      
      
      MMS4 FEEPS top side burst mode electron count rate sensor 10 [mms4_epd_feeps_brst_l2_electron_top_count_rate_sensorid_10]
      
      
      MMS4 FEEPS top side burst mode electron count rate sensor 11 [mms4_epd_feeps_brst_l2_electron_top_count_rate_sensorid_11]
      
      
      MMS4 FEEPS top side burst mode electron count rate sensor 12 [mms4_epd_feeps_brst_l2_electron_top_count_rate_sensorid_12]
      
      
      MMS4 FEEPS bottom side burst mode electron count rate sensor 1 [mms4_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_1]
      
      
      MMS4 FEEPS bottom side burst mode electron count rate sensor 2 [mms4_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_2]
      
      
      MMS4 FEEPS bottom side burst mode electron count rate sensor 3 [mms4_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_3]
      
      
      MMS4 FEEPS bottom side burst mode electron count rate sensor 4 [mms4_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_4]
      
      
      MMS4 FEEPS bottom side burst mode electron count rate sensor 5 [mms4_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_5]
      
      
      MMS4 FEEPS bottom side burst mode electron count rate sensor 9 [mms4_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_9]
      
      
      MMS4 FEEPS bottom side burst mode electron count rate sensor 10 [mms4_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_10]
      
      
      MMS4 FEEPS bottom side burst mode electron count rate sensor 11 [mms4_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_11]
      
      
      MMS4 FEEPS bottom side burst mode electron count rate sensor 12 [mms4_epd_feeps_brst_l2_electron_bottom_count_rate_sensorid_12]
      
      
      MMS4 FEEPS top side burst mode electron intensity sensor 1 [mms4_epd_feeps_brst_l2_electron_top_intensity_sensorid_1]
      
      
      MMS4 FEEPS top side burst mode electron intensity sensor 2 [mms4_epd_feeps_brst_l2_electron_top_intensity_sensorid_2]
      
      
      MMS4 FEEPS top side burst mode electron intensity sensor 3 [mms4_epd_feeps_brst_l2_electron_top_intensity_sensorid_3]
      
      
      MMS4 FEEPS top side burst mode electron intensity sensor 4 [mms4_epd_feeps_brst_l2_electron_top_intensity_sensorid_4]
      
      
      MMS4 FEEPS top side burst mode electron intensity sensor 5 [mms4_epd_feeps_brst_l2_electron_top_intensity_sensorid_5]
      
      
      MMS4 FEEPS top side burst mode electron intensity sensor 9 [mms4_epd_feeps_brst_l2_electron_top_intensity_sensorid_9]
      
      
      MMS4 FEEPS top side burst mode electron intensity sensor 10 [mms4_epd_feeps_brst_l2_electron_top_intensity_sensorid_10]
      
      
      MMS4 FEEPS top side burst mode electron intensity sensor 11 [mms4_epd_feeps_brst_l2_electron_top_intensity_sensorid_11]
      
      
      MMS4 FEEPS top side burst mode electron intensity sensor 12 [mms4_epd_feeps_brst_l2_electron_top_intensity_sensorid_12]
      
      
      MMS4 FEEPS bottom side burst mode electron intensity sensor 1 [mms4_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_1]
      
      
      MMS4 FEEPS bottom side burst mode electron intensity sensor 2 [mms4_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_2]
      
      
      MMS4 FEEPS bottom side burst mode electron intensity sensor 3 [mms4_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_3]
      
      
      MMS4 FEEPS bottom side burst mode electron intensity sensor 4 [mms4_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_4]
      
      
      MMS4 FEEPS bottom side burst mode electron intensity sensor 5 [mms4_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_5]
      
      
      MMS4 FEEPS bottom side burst mode electron intensity sensor 9 [mms4_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_9]
      
      
      MMS4 FEEPS bottom side burst mode electron intensity sensor 10 [mms4_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_10]
      
      
      MMS4 FEEPS bottom side burst mode electron intensity sensor 11 [mms4_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_11]
      
      
      MMS4 FEEPS bottom side burst mode electron intensity sensor 12 [mms4_epd_feeps_brst_l2_electron_bottom_intensity_sensorid_12]
      
      
      MMS4 FEEPS top side burst mode electron count error statistics sensor 1 [mms4_epd_feeps_brst_l2_electron_top_percent_error_sensorid_1]
      
      
      MMS4 FEEPS top side burst mode electron count error statistics sensor 2 [mms4_epd_feeps_brst_l2_electron_top_percent_error_sensorid_2]
      
      
      MMS4 FEEPS top side burst mode electron count error statistics sensor 3 [mms4_epd_feeps_brst_l2_electron_top_percent_error_sensorid_3]
      
      
      MMS4 FEEPS top side burst mode electron count error statistics sensor 4 [mms4_epd_feeps_brst_l2_electron_top_percent_error_sensorid_4]
      
      
      MMS4 FEEPS top side burst mode electron count error statistics sensor 5 [mms4_epd_feeps_brst_l2_electron_top_percent_error_sensorid_5]
      
      
      MMS4 FEEPS top side burst mode electron count error statistics sensor 9 [mms4_epd_feeps_brst_l2_electron_top_percent_error_sensorid_9]
      
      
      MMS4 FEEPS top side burst mode electron count error statistics sensor 10 [mms4_epd_feeps_brst_l2_electron_top_percent_error_sensorid_10]
      
      
      MMS4 FEEPS top side burst mode electron count error statistics sensor 11 [mms4_epd_feeps_brst_l2_electron_top_percent_error_sensorid_11]
      
      
      MMS4 FEEPS top side burst mode electron count error statistics sensor 12 [mms4_epd_feeps_brst_l2_electron_top_percent_error_sensorid_12]
      
      
      MMS4 FEEPS bottom side burst mode electron count error statistics sensor 1 [mms4_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_1]
      
      
      MMS4 FEEPS bottom side burst mode electron count error statistics sensor 2 [mms4_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_2]
      
      
      MMS4 FEEPS bottom side burst mode electron count error statistics sensor 3 [mms4_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_3]
      
      
      MMS4 FEEPS bottom side burst mode electron count error statistics sensor 4 [mms4_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_4]
      
      
      MMS4 FEEPS bottom side burst mode electron count error statistics sensor 5 [mms4_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_5]
      
      
      MMS4 FEEPS bottom side burst mode electron count error statistics sensor 9 [mms4_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_9]
      
      
      MMS4 FEEPS bottom side burst mode electron count error statistics sensor 10 [mms4_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_10]
      
      
      MMS4 FEEPS bottom side burst mode electron count error statistics sensor 11 [mms4_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_11]
      
      
      MMS4 FEEPS bottom side burst mode electron count error statistics sensor 12 [mms4_epd_feeps_brst_l2_electron_bottom_percent_error_sensorid_12]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms4_epd_feeps_brst_l2_electron_pitch_angle]
      
      
      Latitude [mms4_epd_feeps_brst_l2_electron_lat_gse]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS4_FEEPS_BRST_L2_ION (spase://NASA/NumericalData/MMS/4/EnergeticParticleDetector/FEEPS/Burst/Level2/Ion/PT0.3025S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms4_epd_feeps_brst_l2_ion_top_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms4_epd_feeps_brst_l2_ion_top_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms4_epd_feeps_brst_l2_ion_top_quality_indicator_sensorid_8]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms4_epd_feeps_brst_l2_ion_bottom_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms4_epd_feeps_brst_l2_ion_bottom_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms4_epd_feeps_brst_l2_ion_bottom_quality_indicator_sensorid_8]
      
      
      MMS4 FEEPS top side burst mode ion count rate sensor 6 [mms4_epd_feeps_brst_l2_ion_top_count_rate_sensorid_6]
      
      
      MMS4 FEEPS top side burst mode ion count rate sensor 7 [mms4_epd_feeps_brst_l2_ion_top_count_rate_sensorid_7]
      
      
      MMS4 FEEPS top side burst mode ion count rate sensor 8 [mms4_epd_feeps_brst_l2_ion_top_count_rate_sensorid_8]
      
      
      MMS4 FEEPS bottom side burst mode ion count rate sensor 6 [mms4_epd_feeps_brst_l2_ion_bottom_count_rate_sensorid_6]
      
      
      MMS4 FEEPS bottom side burst mode ion count rate sensor 7 [mms4_epd_feeps_brst_l2_ion_bottom_count_rate_sensorid_7]
      
      
      MMS4 FEEPS bottom side burst mode ion count rate sensor 8 [mms4_epd_feeps_brst_l2_ion_bottom_count_rate_sensorid_8]
      
      
      MMS4 FEEPS top side burst mode ion intensity sensor 6 [mms4_epd_feeps_brst_l2_ion_top_intensity_sensorid_6]
      
      
      MMS4 FEEPS top side burst mode ion intensity sensor 7 [mms4_epd_feeps_brst_l2_ion_top_intensity_sensorid_7]
      
      
      MMS4 FEEPS top side burst mode ion intensity sensor 8 [mms4_epd_feeps_brst_l2_ion_top_intensity_sensorid_8]
      
      
      MMS4 FEEPS bottom side burst mode ion intensity sensor 6 [mms4_epd_feeps_brst_l2_ion_bottom_intensity_sensorid_6]
      
      
      MMS4 FEEPS bottom side burst mode ion intensity sensor 7 [mms4_epd_feeps_brst_l2_ion_bottom_intensity_sensorid_7]
      
      
      MMS4 FEEPS bottom side burst mode ion intensity sensor 8 [mms4_epd_feeps_brst_l2_ion_bottom_intensity_sensorid_8]
      
      
      MMS4 FEEPS top side burst mode ion count error statistics sensor 6 [mms4_epd_feeps_brst_l2_ion_top_percent_error_sensorid_6]
      
      
      MMS4 FEEPS top side burst mode ion count error statistics sensor 7 [mms4_epd_feeps_brst_l2_ion_top_percent_error_sensorid_7]
      
      
      MMS4 FEEPS top side burst mode ion count error statistics sensor 8 [mms4_epd_feeps_brst_l2_ion_top_percent_error_sensorid_8]
      
      
      MMS4 FEEPS bottom side burst mode ion count error statistics sensor 6 [mms4_epd_feeps_brst_l2_ion_bottom_percent_error_sensorid_6]
      
      
      MMS4 FEEPS bottom side burst mode ion count error statistics sensor 7 [mms4_epd_feeps_brst_l2_ion_bottom_percent_error_sensorid_7]
      
      
      MMS4 FEEPS bottom side burst mode ion count error statistics sensor 8 [mms4_epd_feeps_brst_l2_ion_bottom_percent_error_sensorid_8]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms4_epd_feeps_brst_l2_ion_pitch_angle]
      
      
      Latitude [mms4_epd_feeps_brst_l2_ion_lat_gse]
      
      
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Data Access Code Examples written in Python and IDL®.
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MMS4_FEEPS_SRVY_L2_ELECTRON (spase://NASA/NumericalData/MMS/4/EnergeticParticleDetector/FEEPS/Survey/Level2/Electron/PT2.42S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms4_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms4_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms4_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms4_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms4_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms4_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms4_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms4_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms4_epd_feeps_srvy_l2_electron_top_quality_indicator_sensorid_12]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 1 [mms4_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_1]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 2 [mms4_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_2]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 3 [mms4_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_3]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 4 [mms4_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_4]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 5 [mms4_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_5]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 9 [mms4_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_9]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 10 [mms4_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_10]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 11 [mms4_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_11]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 12 [mms4_epd_feeps_srvy_l2_electron_bottom_quality_indicator_sensorid_12]
      
      
      MMS4 FEEPS top side survey mode electron count rate sensor 1 [mms4_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_1]
      
      
      MMS4 FEEPS top side survey mode electron count rate sensor 2 [mms4_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_2]
      
      
      MMS4 FEEPS top side survey mode electron count rate sensor 3 [mms4_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_3]
      
      
      MMS4 FEEPS top side survey mode electron count rate sensor 4 [mms4_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_4]
      
      
      MMS4 FEEPS top side survey mode electron count rate sensor 5 [mms4_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_5]
      
      
      MMS4 FEEPS top side survey mode electron count rate sensor 9 [mms4_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_9]
      
      
      MMS4 FEEPS top side survey mode electron count rate sensor 10 [mms4_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_10]
      
      
      MMS4 FEEPS top side survey mode electron count rate sensor 11 [mms4_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_11]
      
      
      MMS4 FEEPS top side survey mode electron count rate sensor 12 [mms4_epd_feeps_srvy_l2_electron_top_count_rate_sensorid_12]
      
      
      MMS4 FEEPS bottom side survey mode electron count rate sensor 1 [mms4_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_1]
      
      
      MMS4 FEEPS bottom side survey mode electron count rate sensor 2 [mms4_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_2]
      
      
      MMS4 FEEPS bottom side survey mode electron count rate sensor 3 [mms4_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_3]
      
      
      MMS4 FEEPS bottom side survey mode electron count rate sensor 4 [mms4_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_4]
      
      
      MMS4 FEEPS bottom side survey mode electron count rate sensor 5 [mms4_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_5]
      
      
      MMS4 FEEPS bottom side survey mode electron count rate sensor 9 [mms4_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_9]
      
      
      MMS4 FEEPS bottom side survey mode electron count rate sensor 10 [mms4_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_10]
      
      
      MMS4 FEEPS bottom side survey mode electron count rate sensor 11 [mms4_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_11]
      
      
      MMS4 FEEPS bottom side survey mode electron count rate sensor 12 [mms4_epd_feeps_srvy_l2_electron_bottom_count_rate_sensorid_12]
      
      
      MMS4 FEEPS top side survey mode electron intensity sensor 1 [mms4_epd_feeps_srvy_l2_electron_top_intensity_sensorid_1]
      
      
      MMS4 FEEPS top side survey mode electron intensity sensor 2 [mms4_epd_feeps_srvy_l2_electron_top_intensity_sensorid_2]
      
      
      MMS4 FEEPS top side survey mode electron intensity sensor 3 [mms4_epd_feeps_srvy_l2_electron_top_intensity_sensorid_3]
      
      
      MMS4 FEEPS top side survey mode electron intensity sensor 4 [mms4_epd_feeps_srvy_l2_electron_top_intensity_sensorid_4]
      
      
      MMS4 FEEPS top side survey mode electron intensity sensor 5 [mms4_epd_feeps_srvy_l2_electron_top_intensity_sensorid_5]
      
      
      MMS4 FEEPS top side survey mode electron intensity sensor 9 [mms4_epd_feeps_srvy_l2_electron_top_intensity_sensorid_9]
      
      
      MMS4 FEEPS top side survey mode electron intensity sensor 10 [mms4_epd_feeps_srvy_l2_electron_top_intensity_sensorid_10]
      
      
      MMS4 FEEPS top side survey mode electron intensity sensor 11 [mms4_epd_feeps_srvy_l2_electron_top_intensity_sensorid_11]
      
      
      MMS4 FEEPS top side survey mode electron intensity sensor 12 [mms4_epd_feeps_srvy_l2_electron_top_intensity_sensorid_12]
      
      
      MMS4 FEEPS bottom side survey mode electron intensity sensor 1 [mms4_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_1]
      
      
      MMS4 FEEPS bottom side survey mode electron intensity sensor 2 [mms4_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_2]
      
      
      MMS4 FEEPS bottom side survey mode electron intensity sensor 3 [mms4_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_3]
      
      
      MMS4 FEEPS bottom side survey mode electron intensity sensor 4 [mms4_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_4]
      
      
      MMS4 FEEPS bottom side survey mode electron intensity sensor 5 [mms4_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_5]
      
      
      MMS4 FEEPS bottom side survey mode electron intensity sensor 9 [mms4_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_9]
      
      
      MMS4 FEEPS bottom side survey mode electron intensity sensor 10 [mms4_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_10]
      
      
      MMS4 FEEPS bottom side survey mode electron intensity sensor 11 [mms4_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_11]
      
      
      MMS4 FEEPS bottom side survey mode electron intensity sensor 12 [mms4_epd_feeps_srvy_l2_electron_bottom_intensity_sensorid_12]
      
      
      MMS4 FEEPS top side survey mode electron count error statistics sensor 1 [mms4_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_1]
      
      
      MMS4 FEEPS top side survey mode electron count error statistics sensor 2 [mms4_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_2]
      
      
      MMS4 FEEPS top side survey mode electron count error statistics sensor 3 [mms4_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_3]
      
      
      MMS4 FEEPS top side survey mode electron count error statistics sensor 4 [mms4_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_4]
      
      
      MMS4 FEEPS top side survey mode electron count error statistics sensor 5 [mms4_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_5]
      
      
      MMS4 FEEPS top side survey mode electron count error statistics sensor 9 [mms4_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_9]
      
      
      MMS4 FEEPS top side survey mode electron count error statistics sensor 10 [mms4_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_10]
      
      
      MMS4 FEEPS top side survey mode electron count error statistics sensor 11 [mms4_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_11]
      
      
      MMS4 FEEPS top side survey mode electron count error statistics sensor 12 [mms4_epd_feeps_srvy_l2_electron_top_percent_error_sensorid_12]
      
      
      MMS4 FEEPS bottom side survey mode electron count error statistics sensor 1 [mms4_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_1]
      
      
      MMS4 FEEPS bottom side survey mode electron count error statistics sensor 2 [mms4_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_2]
      
      
      MMS4 FEEPS bottom side survey mode electron count error statistics sensor 3 [mms4_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_3]
      
      
      MMS4 FEEPS bottom side survey mode electron count error statistics sensor 4 [mms4_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_4]
      
      
      MMS4 FEEPS bottom side survey mode electron count error statistics sensor 5 [mms4_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_5]
      
      
      MMS4 FEEPS bottom side survey mode electron count error statistics sensor 9 [mms4_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_9]
      
      
      MMS4 FEEPS bottom side survey mode electron count error statistics sensor 10 [mms4_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_10]
      
      
      MMS4 FEEPS bottom side survey mode electron count error statistics sensor 11 [mms4_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_11]
      
      
      MMS4 FEEPS bottom side survey mode electron count error statistics sensor 12 [mms4_epd_feeps_srvy_l2_electron_bottom_percent_error_sensorid_12]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms4_epd_feeps_srvy_l2_electron_pitch_angle]
      
      
      Latitude [mms4_epd_feeps_srvy_l2_electron_lat_gse]
      
      
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MMS4_FEEPS_SRVY_L2_ION (spase://NASA/NumericalData/MMS/4/EnergeticParticleDetector/FEEPS/Survey/Level2/Ion/PT2.42S)
Description
http://www.lasp.colorado.edu
Modification History
Generated at LASP
 
  • Data Variable Descriptions
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms4_epd_feeps_srvy_l2_ion_top_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms4_epd_feeps_srvy_l2_ion_top_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms4_epd_feeps_srvy_l2_ion_top_quality_indicator_sensorid_8]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 6 [mms4_epd_feeps_srvy_l2_ion_bottom_quality_indicator_sensorid_6]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 7 [mms4_epd_feeps_srvy_l2_ion_bottom_quality_indicator_sensorid_7]
      
      
      Quality Indicator (0=VALID FOR SCIENCE, 1=CAUTION, 2=PROBLEMATIC, 3=NOT VALID FOR SCIENCE, 4=CALIBRATION) sensor 8 [mms4_epd_feeps_srvy_l2_ion_bottom_quality_indicator_sensorid_8]
      
      
      MMS4 FEEPS top side survey mode ion count rate sensor 6 [mms4_epd_feeps_srvy_l2_ion_top_count_rate_sensorid_6]
      
      
      MMS4 FEEPS top side survey mode ion count rate sensor 7 [mms4_epd_feeps_srvy_l2_ion_top_count_rate_sensorid_7]
      
      
      MMS4 FEEPS top side survey mode ion count rate sensor 8 [mms4_epd_feeps_srvy_l2_ion_top_count_rate_sensorid_8]
      
      
      MMS4 FEEPS bottom side survey mode ion count rate sensor 6 [mms4_epd_feeps_srvy_l2_ion_bottom_count_rate_sensorid_6]
      
      
      MMS4 FEEPS bottom side survey mode ion count rate sensor 7 [mms4_epd_feeps_srvy_l2_ion_bottom_count_rate_sensorid_7]
      
      
      MMS4 FEEPS bottom side survey mode ion count rate sensor 8 [mms4_epd_feeps_srvy_l2_ion_bottom_count_rate_sensorid_8]
      
      
      MMS4 FEEPS top side survey mode ion intensity sensor 6 [mms4_epd_feeps_srvy_l2_ion_top_intensity_sensorid_6]
      
      
      MMS4 FEEPS top side survey mode ion intensity sensor 7 [mms4_epd_feeps_srvy_l2_ion_top_intensity_sensorid_7]
      
      
      MMS4 FEEPS top side survey mode ion intensity sensor 8 [mms4_epd_feeps_srvy_l2_ion_top_intensity_sensorid_8]
      
      
      MMS4 FEEPS bottom side survey mode ion intensity sensor 6 [mms4_epd_feeps_srvy_l2_ion_bottom_intensity_sensorid_6]
      
      
      MMS4 FEEPS bottom side survey mode ion intensity sensor 7 [mms4_epd_feeps_srvy_l2_ion_bottom_intensity_sensorid_7]
      
      
      MMS4 FEEPS bottom side survey mode ion intensity sensor 8 [mms4_epd_feeps_srvy_l2_ion_bottom_intensity_sensorid_8]
      
      
      MMS4 FEEPS top side survey mode ion count error statistics sensor 6 [mms4_epd_feeps_srvy_l2_ion_top_percent_error_sensorid_6]
      
      
      MMS4 FEEPS top side survey mode ion count error statistics sensor 7 [mms4_epd_feeps_srvy_l2_ion_top_percent_error_sensorid_7]
      
      
      MMS4 FEEPS top side survey mode ion count error statistics sensor 8 [mms4_epd_feeps_srvy_l2_ion_top_percent_error_sensorid_8]
      
      
      MMS4 FEEPS bottom side survey mode ion count error statistics sensor 6 [mms4_epd_feeps_srvy_l2_ion_bottom_percent_error_sensorid_6]
      
      
      MMS4 FEEPS bottom side survey mode ion count error statistics sensor 7 [mms4_epd_feeps_srvy_l2_ion_bottom_percent_error_sensorid_7]
      
      
      MMS4 FEEPS bottom side survey mode ion count error statistics sensor 8 [mms4_epd_feeps_srvy_l2_ion_bottom_percent_error_sensorid_8]
      
      
      The angle formed by the normal vector of the sensor plane and the magnetic field (BField) [mms4_epd_feeps_srvy_l2_ion_pitch_angle]
      
      
      Latitude [mms4_epd_feeps_srvy_l2_ion_lat_gse]
      
      
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MMS4_FGM_BRST_L2 (spase://NASA/NumericalData/MMS/4/FIELDS/FGM/Burst/Level2/PT0.0078125S)
Description
The Fluxgate Magnetometers (FGM) on Magnetospheric Multiscale consist of a
traditional Analog Fluxgate Magnetometer (AFG), and a Digital Fluxgate
magnetometer (DFG). The dual magnetometers are operated as a single instrument
providing a single intercalibrated data product. Range changes occur at
different times on the two instruments so the gains checked each periapsis can
be carried out unambiguously to apoapsis. Cross correlation of calibration
parameters can separate causes of the any apparent calibration changes. Use of
Electron Drift Instrument (EDI) to determine the field along the rotation axis
allows accurate monitoring of the zero levels along the rotation axis.  Prior to
launch the magnetometers were calibrated at the Technical University,
Braunschweig, except for the AFG magnetometers on MMS3 and MMS4, which were
calibrated at UCLA.  Both sets of sensors are operated for the entire MMS orbit,
with slow survey (8 samples per second) outside of the Region of Interest (ROI),
and fast survey (16 samples per second) inside the ROI. Within the ROI burst
mode data (128 samples per second) are also acquired.  A detailed description of
the MMS fluxgate magnetometers, including science objectives, instrument
description, calibration, magnetic cleanliness program, and data flow can be
found at http://link.springer.com/article/10.1007%2Fs11214-014-0057-3 (DOI 
10.1007/s11214-014-0057-3).Additional information can also be found at
http://www-spc.igpp.ucla.edu/ssc/mms (UCLA),and http://www.iwf.oeaw.ac.at (IWF,
Graz).
For the purpose of creating a unified FGM Level2 data product, burst mode data
is taken from DFG and survey mode data is taken from AFG.  Because AFG and DFG
are cross-calibrated on an orbit-averaged basis, small differences in offset may
be observed between Level2 burst and survey mode data.  Consequently, any
differences are within the error of the measurement. Based on preliminary
analysis of the data, the absolute error within the Region of Interest (ROI) is
estimated to be no more than 0.1 nT in the spin-plane, 0.15 nT along the
spin-axis and 0.2 nT in total magnitude.
Modification History
version X=5:  * Y-version number comes from cal file entries. 
              *
Ensures there are 2 ephemeris points before/after data to enable proper spline. 

              * Fix to depend_0 of rdeltahalf:  fixes bug when reading position
data.
              * L-vector for DMPA2GSE transformation is smoothed with a
gaussian filter, instead 
                of using a single average value for
the day.  This short-term filter avoids  
                introduding artificial
jumps at 00:00 UTC and removes 7-minute 'wobble' after  
               
maneuvers in the GSE result.   
              * Fixes error with DEFATT file
selection found when choosing the 
                daily DEFATT files to be used
in Phase 2.
              * Fixed bug where reference Etemp was used for high
range gain.  Now uses measured Etemp.
version X=4:  First version for public
release of L2.
              Renamed variables to conform with new MMS variable
name guidelines 
              (obs_instr_paramName[_coordSys]_mode_level):  
  
             Mag field parameters include 'b' for paramName.  
               
Use 'r' instead of 'pos' for S/C position paramName.  
               
Eliminated 'rate', replaced with 'bdeltahalf'.  Added 'rdeltahalf'.
            
   l1a_mode is now just 'mode'.
version X=3:  fixed removal of overlap between
modes.
              fixed a bug that caused stemp and etemp to be
empty.
version X=2:  flag parameter name corrected: was 'status'
               
        added bits 4, 5, 6 to flag saturation on B1, B2, and B3, respectively
  
                     added bit 7 to flag bad data at range changes
             
Added etemp and l1a_mode parameters.  
              rate, hirange, and stemp
parameters now comply with MMS CDF Guidlelines, e.g.
              FILLVAL now
defined for stemp and etemp, and is set to !values.f_nan
              No longer
use Var_Parents attribute in stemp -- see Parents instead
              In this
version, temperature-corrected gains are applied.  Reference temperatures are
used when 
              stemp or etemp are set to FILLVAL. 
             
Non-linearity correction is applied to high rage DFG data.
version X=1:  added
'flag', rate and hirange parameters (but 'flag' is actually called 'status')
 
  • Data Variable Descriptions
      Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (128 S/s) [mms4_fgm_b_gse_brst_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms4_fgm_b_gse_brst_l2]
      
      
      Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (128 S/s) [mms4_fgm_b_gsm_brst_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms4_fgm_b_gsm_brst_l2]
      
      
      Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (128 S/s) [mms4_fgm_b_dmpa_brst_l2_clean]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      ---> Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (128 S/s), including flagged data [mms4_fgm_b_dmpa_brst_l2]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (128 S/s) [mms4_fgm_b_bcs_brst_l2_clean]
      
      
      ---> Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (128 S/s), including flagged data [mms4_fgm_b_bcs_brst_l2]
      
      
      Quality Flag: 0 = No identified problems, non-zero = blank out the data [mms4_fgm_flag_brst_l2]
      bit definitions: .    0: TBD, 1: TBD, 2: user flagged, 3: TBD, .    4: B1
      saturated, 5: B2 saturated, 6: B3 saturated, 7: range-change glitch, .    8-31:
      TBD
      
      Definitive Position in GSE coordinates, 30 second [mms4_fgm_r_gse_brst_l2]
      
      
      Definitive Position in GSM coordinates, 30 second [mms4_fgm_r_gsm_brst_l2]
      
      
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MMS4_FGM_SRVY_L2 (spase://NASA/NumericalData/MMS/4/FIELDS/FGM/Survey/Level2/PT0.125S)
Description
The Fluxgate Magnetometers (FGM) on Magnetospheric Multiscale consist of a
traditional Analog Fluxgate Magnetometer (AFG), and a Digital Fluxgate
magnetometer (DFG). The dual magnetometers are operated as a single instrument
providing a single intercalibrated data product. Range changes occur at
different times on the two instruments so the gains checked each periapsis can
be carried out unambiguously to apoapsis. Cross correlation of calibration
parameters can separate causes of the any apparent calibration changes. Use of
Electron Drift Instrument (EDI) to determine the field along the rotation axis
allows accurate monitoring of the zero levels along the rotation axis.  Prior to
launch the magnetometers were calibrated at the Technical University,
Braunschweig, except for the AFG magnetometers on MMS3 and MMS4, which were
calibrated at UCLA.  Both sets of sensors are operated for the entire MMS orbit,
with slow survey (8 samples per second) outside of the Region of Interest (ROI),
and fast survey (16 samples per second) inside the ROI. Within the ROI burst
mode data (128 samples per second) are also acquired.  A detailed description of
the MMS fluxgate magnetometers, including science objectives, instrument
description, calibration, magnetic cleanliness program, and data flow can be
found at http://link.springer.com/article/10.1007%2Fs11214-014-0057-3 (DOI 
10.1007/s11214-014-0057-3).Additional information can also be found at
http://www-spc.igpp.ucla.edu/ssc/mms (UCLA),and http://www.iwf.oeaw.ac.at (IWF,
Graz).
For the purpose of creating a unified FGM Level2 data product, burst mode data
is taken from DFG and survey mode data is taken from AFG.  Because AFG and DFG
are cross-calibrated on an orbit-averaged basis, small differences in offset may
be observed between Level2 burst and survey mode data.  Consequently, any
differences are within the error of the measurement. Based on preliminary
analysis of the data, the absolute error within the Region of Interest (ROI) is
estimated to be no more than 0.1 nT in the spin-plane, 0.15 nT along the
spin-axis and 0.2 nT in total magnitude.
Modification History
version X=5:  * Y-version number comes from cal file entries. 
              *
Ensures there are 2 ephemeris points before/after data to enable proper spline. 

              * Fix to depend_0 of rdeltahalf:  fixes bug when reading position
data.
              * L-vector for DMPA2GSE transformation is smoothed with a
gaussian filter, instead 
                of using a single average value for
the day.  This short-term filter avoids  
                introduding artificial
jumps at 00:00 UTC and removes 7-minute 'wobble' after  
               
maneuvers in the GSE result.   
              * Fixes error with DEFATT file
selection found when choosing the 
                daily DEFATT files to be used
in Phase 2.
              * Fixed bug where reference Etemp was used for high
range gain.  Now uses measured Etemp.
version X=4:  First version for public
release of L2.
              Renamed variables to conform with new MMS variable
name guidelines 
              (obs_instr_paramName[_coordSys]_mode_level):  
  
             Mag field parameters include 'b' for paramName.  
               
Use 'r' instead of 'pos' for S/C position paramName.  
               
Eliminated 'rate', replaced with 'bdeltahalf'.  Added 'rdeltahalf'.
            
   l1a_mode is now just 'mode'.
version X=3:  fixed removal of overlap between
modes.
              fixed a bug that caused stemp and etemp to be
empty.
version X=2:  flag parameter name corrected: was 'status'
               
        added bits 4, 5, 6 to flag saturation on B1, B2, and B3, respectively
  
                     added bit 7 to flag bad data at range changes
             
Added etemp and l1a_mode parameters.  
              rate, hirange, and stemp
parameters now comply with MMS CDF Guidlelines, e.g.
              FILLVAL now
defined for stemp and etemp, and is set to !values.f_nan
              No longer
use Var_Parents attribute in stemp -- see Parents instead
              In this
version, temperature-corrected gains are applied.  Reference temperatures are
used when 
              stemp or etemp are set to FILLVAL. 
             
Non-linearity correction is applied to high rage DFG data.
version X=1:  added
'flag', rate and hirange parameters (but 'flag' is actually called 'status')
 
  • Data Variable Descriptions
      Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (8 or 16 S/s) [mms4_fgm_b_gse_srvy_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Ecliptic (GSE) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms4_fgm_b_gse_srvy_l2]
      
      
      Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (8 or 16 S/s) [mms4_fgm_b_gsm_srvy_l2_clean]
      
      
      ---> Magnetic field vector in Geocentric Solar Magnetospheric (GSM) cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms4_fgm_b_gsm_srvy_l2]
      
      
      Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (8 or 16 S/s) [mms4_fgm_b_dmpa_srvy_l2_clean]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      ---> Magnetic field vector in Despun MPA-aligned cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms4_fgm_b_dmpa_srvy_l2]
      During nominal operatins in the region of interest, DMPA is within 3 degrees of
      GSE.  
      
      Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (8 or 16 S/s) [mms4_fgm_b_bcs_srvy_l2_clean]
      
      
      ---> Magnetic field vector in Body Coordinate System cartesian coordinates plus Btotal (8 or 16 S/s), including flagged data [mms4_fgm_b_bcs_srvy_l2]
      
      
      Quality Flag: 0 = No identified problems, non-zero = blank out the data [mms4_fgm_flag_srvy_l2]
      bit definitions: .    0: TBD, 1: TBD, 2: user flagged, 3: TBD, .    4: B1
      saturated, 5: B2 saturated, 6: B3 saturated, 7: range-change glitch, .    8-31:
      TBD
      
      Definitive Position in GSE coordinates, 30 second [mms4_fgm_r_gse_srvy_l2]
      
      
      Definitive Position in GSM coordinates, 30 second [mms4_fgm_r_gsm_srvy_l2]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MMS4_FPI_BRST_L2_DES-DIST (spase://NASA/NumericalData/MMS/4/FastPlasmaInvestigation/DES/Burst/Level2/Distribution/PT0.03S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data are taken at burst (30/150 ms for DES/DIS)
resolution in this mode.  Data are also made available at survey (4.5 s, etc)
resolution; these form a separate product from this.  Per mission design, not
all burst-resolution data are downlinked.  This product contains phase-space
distribution maps of those burst-resolution data selected for downlink.  In
particular, the (highest possible quality at the time of release)
corrected/converted "Burst SkyMap" distributions are reported with time-stamps
and other annotation characterizing the state of the instrument system at the
indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      [CDAWeb List/Download/Create ONLY] MMS4 FPI/DES burst sky-map instrument distribution [mms4_des_dist_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 10.9 eV (E1/even) [mms4_des_dist_brst1_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 12.4 eV (E1/odd) [mms4_des_dist_brst1_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~11.6 eV (E1 even-odd) [mms4_des_dist_brst1_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 10.9 eV (E1/even) [mms4_des_dist_brst1_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 12.4 eV (E1/odd) [mms4_des_dist_brst1_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 37.9 eV (E6/even) [mms4_des_dist_brst6_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 42.9 eV (E6/odd) [mms4_des_dist_brst6_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~40.4 eV (E6 even-odd) [mms4_des_dist_brst6_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 37.9 eV (E6/even) [mms4_des_dist_brst6_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 42.9 eV (E6/odd) [mms4_des_dist_brst6_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 80.0 eV (E9/even) [mms4_des_dist_brst9_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 90.6 eV (E9/odd) [mms4_des_dist_brst9_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~85 eV (E9 even-odd) [mms4_des_dist_brst9_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 80.0 eV (E9/even) [mms4_des_dist_brst9_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 90.6 eV (E9/odd) [mms4_des_dist_brst9_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 169 eV (E12/even) [mms4_des_dist_brst12_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 191 eV (E12/odd) [mms4_des_dist_brst12_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~180 eV (E12 even-odd) [mms4_des_dist_brst12_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 169 eV (E12/even) [mms4_des_dist_brst12_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 191 eV (E12/odd) [mms4_des_dist_brst12_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 277 eV (E14/even) [mms4_des_dist_brst14_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 314 eV (E14/odd) [mms4_des_dist_brst14_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~295 eV (E14 even-odd) [mms4_des_dist_brst14_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 277 eV (E14/even) [mms4_des_dist_brst14_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 314 eV (E14/odd) [mms4_des_dist_brst14_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 456 eV (E16/even) [mms4_des_dist_brst16_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 517 eV (E16/odd) [mms4_des_dist_brst16_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~485 eV (E16 even-odd) [mms4_des_dist_brst16_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 456 eV (E16/even) [mms4_des_dist_brst16_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 517 eV (E16/odd) [mms4_des_dist_brst16_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 750 eV (E18/even) [mms4_des_dist_brst18_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 850 eV (E18/odd) [mms4_des_dist_brst18_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~800 eV (E18 even-odd) [mms4_des_dist_brst18_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 750 eV (E18/even) [mms4_des_dist_brst18_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 850 eV (E18/odd) [mms4_des_dist_brst18_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 1230 eV (E20/even) [mms4_des_dist_brst20_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 1400 eV (E20/odd) [mms4_des_dist_brst20_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~1310 eV (E20 even-odd) [mms4_des_dist_brst20_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1230 eV (E20/even) [mms4_des_dist_brst20_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1400 eV (E20/odd) [mms4_des_dist_brst20_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 2600 eV (E23/even) [mms4_des_dist_brst23_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 2950 eV (E23/odd) [mms4_des_dist_brst23_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~2770 eV (E23 even-odd) [mms4_des_dist_brst23_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2600 eV (E23/even) [mms4_des_dist_brst23_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2950 eV (E23/odd) [mms4_des_dist_brst23_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 5490 eV (E26/even) [mms4_des_dist_brst26_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 6210 eV (E26/odd) [mms4_des_dist_brst26_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~5840 eV (E26 even-odd) [mms4_des_dist_brst26_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5490 eV (E26/even) [mms4_des_dist_brst26_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 6210 eV (E26/odd) [mms4_des_dist_brst26_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 24400 eV (E32/even) [mms4_des_dist_brst32_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES burst sky-map instrument distribution - 27600 eV (E32/odd) [mms4_des_dist_brst32_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~26000 eV (E32 even-odd) [mms4_des_dist_brst32_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 24400 eV (E32/even) [mms4_des_dist_brst32_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 27600 eV (E32/odd) [mms4_des_dist_brst32_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [List/Create only in CDAWeb] 1-sigma error: MMS4 FPI/DES burst sky-map instrument distribution [mms4_des_disterr_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES vector of data-quality indicators at burst-start time [mms4_des_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS4 FPI/DES compression lossless/lossy indicator at survey-start time [mms4_des_compressionloss_brst]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS4 FPI/DES step table parity, this burst [mms4_des_steptable_parity_brst]
      FPI/DES alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS4 FPI/DES Del-Phi (obs spin-phase) count at burst-start time [mms4_des_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS4 FPI/DES Del-Phi (obs spin-phase) angle at burst-start time [mms4_des_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS4 FPI/DES burst average f1 count values [mms4_des_avgf1counts_brst]
      Average f1-count level as a function of energy
      
      MMS4 FPI/DES burst sky-map microsecond offsets from Epoch [mms4_des_steptimeoffsets_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order. Offsets reflect 128 steps over the 30 msec sweep
      period. See FPI docs for details.
      
      ---> MMS4 FPI/DES sector de-Spin P value, this burst [mms4_des_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS4 FPI/DES burst sky-map instrument azimuthal angles [mms4_des_phi_brst]
      see FPI docs for details
      
      MMS FPI/DES burst sky-map parity 0/1 energies [mms4_des_energy_brst]
      Energies (parity 0/1) in the 64-step FPI energy table
      
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MMS4_FPI_BRST_L2_DES-MOMS (spase://NASA/NumericalData/MMS/4/FastPlasmaInvestigation/DES/Burst/Level2/Moments/PT0.03S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode.  Data are also made available at survey (4.5
s, etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked.  Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available.  This product contains results from
integrating the standard moments of phase-space distributions formed from the
indicated data type (DES/DIS burst, FS or SS).  For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DES 32-bit vector of data-quality indicators at burst-start time [mms4_des_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>25%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied
      
      ---> MMS4 FPI/DES compression lossless/lossy indicator at survey-start time [mms4_des_compressionloss_brst]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS4 FPI/DES step table parity, this burst [mms4_des_steptable_parity_brst]
      FPI/DES alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS4 FPI/DES Del-Phi (obs spin-phase) count at burst-start time [mms4_des_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS4 FPI/DES Del-Phi (obs spin-phase) angle at burst-start time [mms4_des_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      ---> MMS4 FPI/DES sector de-Spin P value, this burst [mms4_des_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS4 FPI/DES electron pitch-angle distribution for "low" energies during this burst [mms4_des_pitchangdist_lowen_brst]
      low energy bin: 0 eV - 200 eV.  pitch-angle bin size: 6 deg.
      
      ---> MMS4 FPI/DES electron pitch-angle distribution for "mid" energies during this burst [mms4_des_pitchangdist_miden_brst]
      mid energy bin: 200 eV - 2 keV.  pitch-angle bin size: 6 deg.
      
      ---> MMS4 FPI/DES electron pitch-angle distribution for "high" energies during this burst [mms4_des_pitchangdist_highen_brst]
      high energy bin: 2 keV - 30 keV.  pitch-angle bin size: 6 deg.
      
      MMS4 FPI/DES electron energy spectrum "near" +X_DSC during this burst [mms4_des_energyspectr_px_brst]
      Counts, summed over DSC velocity-dirs closest to +X_DSC, by energy bin.
      
      ---> MMS4 FPI/DES electron energy spectrum "near" -X_DSC during this burst [mms4_des_energyspectr_mx_brst]
      Counts, summed over DSC velocity-dirs closest to -X_DSC, by energy bin.
      
      ---> MMS4 FPI/DES electron energy spectrum "near" +Y_DSC during this burst [mms4_des_energyspectr_py_brst]
      Counts, summed over DSC velocity-dirs closest to +Y_DSC, by energy bin.
      
      ---> MMS4 FPI/DES electron energy spectrum "near" -Y_DSC during this burst [mms4_des_energyspectr_my_brst]
      Counts, summed over DSC velocity-dirs closest to -Y_DSC, by energy bin.
      
      ---> MMS4 FPI/DES electron energy spectrum "near" +Z_DSC during this burst [mms4_des_energyspectr_pz_brst]
      Counts, summed over DSC velocity-dirs closest to +Z_DSC, by energy bin.
      
      ---> MMS4 FPI/DES electron energy spectrum "near" -Z_DSC during this burst [mms4_des_energyspectr_mz_brst]
      Counts, summed over DSC velocity-dirs closest to -Z_DSC, by energy bin.
      
      MMS4 FPI/DES electron energy parallel spectrum 30 degrees parallel to B during this burst [mms4_des_energyspectr_par_brst]
      Counts, summed within 30 degrees parallel bentPipe magnetic field.
      
      ---> MMS4 FPI/DES electron energy anti-parallel spectrum 30 degrees anti-parallel to B during this burst [mms4_des_energyspectr_anti_brst]
      Counts, summed within 30 degrees antiparallel to bentPipe magnetic field.
      
      ---> MMS4 FPI/DES electron energy perpendicular spectrum 60 degrees perpendicular to B during this burst [mms4_des_energyspectr_perp_brst]
      Counts, summed within 60 degrees perpendicular to bentPipe magnetic field.
      
      MMS4 FPI/DES omni-directional electron energy spectrum during this burst [mms4_des_energyspectr_omni_brst]
      Differential energy flux, averaged (weighted by solid angle) over all look
      directions, by energy bin.
      
      MMS4 FPI/DES electron number density during this burst [mms4_des_numberdensity_brst]
      
      
      ---> (no error bars displayed) MMS4 FPI/DES electron number density during this burst [mms4_des_numberdensity_brst_noerr]
      
      
      ---> MMS4 FPI/DES electron number density error during this burst [mms4_des_numberdensity_err_brst]
      
      
      MMS4 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms4_des_densityextrapolation_low_brst]
      
      
      MMS4 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms4_des_densityextrapolation_high_brst]
      
      
      MMS4 FPI/DES electron bulk-velocity DBCS vector during this burst [mms4_des_bulkv_dbcs_brst]
      
      
      MMS4 FPI/DES electron bulk-velocity estimated spintone vector in DBCS during this burst [mms4_des_bulkv_spintone_dbcs_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS4 FPI/DES electron bulk-velocity DBCS vector during this burst [mms4_des_bulkv_dbcs_brst_noerr]
      
      
      MMS4 FPI/DES electron bulk-velocity GSE vector during this burst [mms4_des_bulkv_gse_brst]
      
      
      MMS4 FPI/DES electron bulk-velocity estimated spintone vector in GSE during this burst [mms4_des_bulkv_spintone_gse_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS4 FPI/DES electron bulk-velocity GSE vector during this burst [mms4_des_bulkv_gse_brst_noerr]
      
      
      MMS4 FPI/DES electron bulk-velocity spintone vector in DBCS during this burst [mms4_des_bulkv_spin_dbcs_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS4 FPI/DES electron bulk-velocity spintone vector in GSE during this burst [mms4_des_bulkv_spin_gse_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS4 FPI/DES electron pressure tensor DBCS matrix during this burst [mms4_des_prestensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES electron pressure tensor GSE matrix during this burst [mms4_des_prestensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES electron temperature tensor DBCS matrix during this burst [mms4_des_temptensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES electron temperature tensor GSE matrix during this burst [mms4_des_temptensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES electron heat-flux DBCS vector during this burst [mms4_des_heatq_dbcs_brst]
      
      
      MMS4 FPI/DES electron heat-flux GSE vector during this burst [mms4_des_heatq_gse_brst]
      
      
      MMS4 FPI/DES electron parallel temperature during this BP [mms4_des_temppara_brst]
      
      
      MMS4 FPI/DES electron perpendicular temperature during this BP [mms4_des_tempperp_brst]
      
      
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MMS4_FPI_BRST_L2_DES-PARTMOMS (spase://NASA/NumericalData/MMS/4/FastPlasmaInvestigation/DES/Burst/Level2/PartialMoments/PT0.03S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s,
etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked. Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available. This product contains partial moments that
come from performing the standard moment integrals over a limited portion of
velocity space. The resulting quantities are named similarly to their
corresponding standard moments, but are decorated with 'part' to differentiate.
For example, density_part is the density moment integrated from a particular
energy step to infinity. These partial moments are formed from the indicated
data type (DES/DIS burst, FS or SS). For convenience, some additional parameters
are included to augment those most commonly found in a moments product of this
sort, plus time-stamps and other annotation characterizing the state of the
instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DES vector of data-quality indicators at burst-start time [mms4_des_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only)
      
      MMS4 FPI/DES partial electron number density during this burst [mms4_des_numberdensity_part_brst]
      
      
      MMS4 FPI/DES partial electron bulk-velocity vector in DBCS during this burst [mms4_des_bulkv_part_dbcs_brst]
      
      
      MMS4 FPI/DES partial electron bulk-velocity vector in GSE during this burst [mms4_des_bulkv_part_gse_brst]
      
      
      MMS4 FPI/DES partial electron pressure tensor in DBCS during this burst [mms4_des_prestensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES partial electron pressure tensor in GSE during this burst [mms4_des_prestensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES partial electron temperature tensor in DBCS during this burst [mms4_des_temptensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES partial electron temperature tensor in GSE during this burst [mms4_des_temptensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES partial electron parallel temperature during this burst [mms4_des_temppara_part_brst]
      
      
      MMS4 FPI/DES partial electron perpendicular temperature during this burst [mms4_des_tempperp_part_brst]
      
      
      MMS4 FPI/DES recommended energy index during this burst [mms4_des_part_index_brst]
      Recommended energy index during this burst
      
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MMS4_FPI_BRST_L2_DIS-DIST (spase://NASA/NumericalData/MMS/4/FastPlasmaInvestigation/DIS/Burst/Level2/Distribution/PT0.15S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data are taken at burst (30/150 ms for DES/DIS)
resolution in this mode.  Data are also made available at survey (4.5 s, etc)
resolution; these form a separate product from this.  Per mission design, not
all burst-resolution data are downlinked.  This product contains phase-space
distribution maps of those burst-resolution data selected for downlink.  In
particular, the (highest possible quality at the time of release)
corrected/converted "Burst SkyMap" distributions are reported with time-stamps
and other annotation characterizing the state of the instrument system at the
indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      [CDAWeb List/Download/Create ONLY] MMS4 FPI/DIS burst sky-map instrument distribution [mms4_dis_dist_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 10.6 eV (E1/even) [mms4_dis_dist_brst1_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 12.0 eV (E1/odd) [mms4_dis_dist_brst1_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~11.3 eV (E1 even-odd) [mms4_dis_dist_brst1_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 10.6 eV (E1/even) [mms4_dis_dist_brst1_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 12.0 eV (E1/odd) [mms4_dis_dist_brst1_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 37.2 eV (E6/even) [mms4_dis_dist_brst6_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 42.1 eV (E6/odd) [mms4_dis_dist_brst6_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~39.6 eV (E6 even-odd) [mms4_dis_dist_brst6_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 37.2 eV (E6/even) [mms4_dis_dist_brst6_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 42.1 eV (E6/odd) [mms4_dis_dist_brst6_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 78.8 eV (E9/even) [mms4_dis_dist_brst9_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 89.3 eV (E9/odd) [mms4_dis_dist_brst9_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~83.9 eV (E9 even-odd) [mms4_dis_dist_brst9_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 78.8 eV (E9/even) [mms4_dis_dist_brst9_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 89.3 eV (E9/odd) [mms4_dis_dist_brst9_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 167 eV (E12/even) [mms4_dis_dist_brst12_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 189 eV (E12/odd) [mms4_dis_dist_brst12_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~178 eV (E12 even-odd) [mms4_dis_dist_brst12_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 167 eV (E12/even) [mms4_dis_dist_brst12_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 189 eV (E12/odd) [mms4_dis_dist_brst12_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 275 eV (E14/even) [mms4_dis_dist_brst14_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 312 eV (E14/odd) [mms4_dis_dist_brst14_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~293 eV (E14 even-odd) [mms4_dis_dist_brst14_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 275 eV (E14/even) [mms4_dis_dist_brst14_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 312 eV (E14/odd) [mms4_dis_dist_brst14_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 455 eV (E16/even) [mms4_dis_dist_brst16_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 515 eV (E16/odd) [mms4_dis_dist_brst16_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~484 eV (E16 even-odd) [mms4_dis_dist_brst16_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 455 eV (E16/even) [mms4_dis_dist_brst16_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 515 eV (E16/odd) [mms4_dis_dist_brst16_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 750 eV (E18/even) [mms4_dis_dist_brst18_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 850 eV (E18/odd) [mms4_dis_dist_brst18_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~800 eV (E18 even-odd) [mms4_dis_dist_brst18_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 750 eV (E18/even) [mms4_dis_dist_brst18_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 850 eV (E18/odd) [mms4_dis_dist_brst18_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 1240 eV (E20/even) [mms4_dis_dist_brst20_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 1400 eV (E20/odd) [mms4_dis_dist_brst20_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~1320 eV (E20 even-odd) [mms4_dis_dist_brst20_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1240 eV (E20/even) [mms4_dis_dist_brst20_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1400 eV (E20/odd) [mms4_dis_dist_brst20_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 2620 eV (E23/even) [mms4_dis_dist_brst23_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 2970 eV (E23/odd) [mms4_dis_dist_brst23_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~2800 eV (E23 even-odd) [mms4_dis_dist_brst23_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2620 eV (E23/even) [mms4_dis_dist_brst23_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2970 eV (E23/odd) [mms4_dis_dist_brst23_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 5560 eV (E26/even) [mms4_dis_dist_brst26_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 6300 eV (E26/odd) [mms4_dis_dist_brst26_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~5920 eV (E26 even-odd) [mms4_dis_dist_brst26_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5560 eV (E26/even) [mms4_dis_dist_brst26_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 6300 eV (E26/odd) [mms4_dis_dist_brst26_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 25000 eV (E32/even) [mms4_dis_dist_brst32_even]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS burst sky-map instrument distribution - 28300 eV (E32/odd) [mms4_dis_dist_brst32_odd]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - ~26600 eV (E32 even-odd) [mms4_dis_dist_brst32_evenodd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 25000 eV (E32/even) [mms4_dis_dist_brst32_even_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 28300 eV (E32/odd) [mms4_dis_dist_brst32_odd_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [List/Create only in CDAWeb] 1-sigma error: MMS4 FPI/DIS burst sky-map instrument distribution [mms4_dis_disterr_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS vector of data-quality indicators at burst-start time [mms4_dis_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS4 FPI/DIS compression lossless/lossy indicator at survey-start time [mms4_dis_compressionloss_brst]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS4 FPI/DIS step table parity, this burst [mms4_dis_steptable_parity_brst]
      FPI/DIS alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS4 FPI/DIS Del-Phi (obs spin-phase) count at burst-start time [mms4_dis_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS4 FPI/DIS Del-Phi (obs spin-phase) angle at burst-start time [mms4_dis_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS4 FPI/DIS burst average f1 count values [mms4_dis_avgf1counts_brst]
      Average f1-count level as a function of energy
      
      MMS4 FPI/DIS burst sky-map microsecond offsets from Epoch [mms4_dis_steptimeoffsets_brst]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order. Offsets reflect 128 steps over the 150 msec sweep
      period. See FPI docs for details.
      
      ---> MMS4 FPI/DIS sector de-Spin P value, this burst [mms4_dis_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS4 FPI/DIS burst sky-map instrument azimuthal angles [mms4_dis_phi_brst]
      see FPI docs for details
      
      MMS FPI/DIS burst sky-map parity 0/1 energies [mms4_dis_energy_brst]
      Energies (parity 0/1) in the 64-step FPI energy table
      
Dataset in CDAWeb
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MMS4_FPI_BRST_L2_DIS-MOMS (spase://NASA/NumericalData/MMS/4/FastPlasmaInvestigation/DIS/Burst/Level2/Moments/PT0.15S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode.  Data are also made available at survey (4.5
s, etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked.  Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available.  This product contains results from
integrating the standard moments of phase-space distributions formed from the
indicated data type (DES/DIS burst, FS or SS).  For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DIS 32-bit vector of data-quality indicators at burst-start time [mms4_dis_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>25%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied
      
      ---> MMS4 FPI/DIS compression lossless/lossy indicator at survey-start time [mms4_dis_compressionloss_brst]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS4 FPI/DIS step table parity, this burst [mms4_dis_steptable_parity_brst]
      FPI/DIS alternates between two tables, designated "even" (0) and "odd" (1).
      
      ---> MMS4 FPI/DIS Del-Phi (obs spin-phase) count at burst-start time [mms4_dis_startdelphi_count_brst]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS4 FPI/DIS Del-Phi (obs spin-phase) angle at burst-start time [mms4_dis_startdelphi_angle_brst]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      ---> MMS4 FPI/DIS sector de-Spin P value, this burst [mms4_dis_sector_despinp_brst]
      Records P-value used to de-spin this burst sky-map on board.  See FPI docs for
      details.
      
      MMS4 FPI/DIS ion energy spectrum "near" +X_DSC during this burst [mms4_dis_energyspectr_px_brst]
      Counts, summed over DSC velocity-dirs closest to +X_DSC, by energy bin.
      
      ---> MMS4 FPI/DIS ion energy spectrum "near" -X_DSC during this burst [mms4_dis_energyspectr_mx_brst]
      Counts, summed over DSC velocity-dirs closest to -X_DSC, by energy bin.
      
      ---> MMS4 FPI/DIS ion energy spectrum "near" +Y_DSC during this burst [mms4_dis_energyspectr_py_brst]
      Counts, summed over DSC velocity-dirs closest to +Y_DSC, by energy bin.
      
      ---> MMS4 FPI/DIS ion energy spectrum "near" -Y_DSC during this burst [mms4_dis_energyspectr_my_brst]
      Counts, summed over DSC velocity-dirs closest to -Y_DSC, by energy bin.
      
      ---> MMS4 FPI/DIS ion energy spectrum "near" +Z_DSC during this burst [mms4_dis_energyspectr_pz_brst]
      Counts, summed over DSC velocity-dirs closest to +Z_DSC, by energy bin.
      
      ---> MMS4 FPI/DIS ion energy spectrum "near" -Z_DSC during this burst [mms4_dis_energyspectr_mz_brst]
      Counts, summed over DSC velocity-dirs closest to -Z_DSC, by energy bin.
      
      MMS4 FPI/DIS omni-directional ion energy spectrum during this burst [mms4_dis_energyspectr_omni_brst]
      Differential energy flux, averaged (weighted by solid angle) over all look
      directions, by energy bin.
      
      MMS4 FPI/DIS ion background energy during this burst [mms4_dis_spectr_bg_brst]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look) background level.
      
      MMS4 FPI/DIS ion background number density during this burst [mms4_dis_numberdensity_bg_brst]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS4 FPI/DIS ion number density during this burst [mms4_dis_numberdensity_brst]
      
      
      ---> (no error bars displayed) MMS4 FPI/DIS ion number density during this burst [mms4_dis_numberdensity_brst_noerr]
      
      
      ---> MMS4 FPI/DIS ion number density error during this burst [mms4_dis_numberdensity_err_brst]
      
      
      MMS4 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms4_dis_densityextrapolation_low_brst]
      
      
      MMS4 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms4_dis_densityextrapolation_high_brst]
      
      
      MMS4 FPI/DIS ion bulk-velocity DBCS vector during this burst [mms4_dis_bulkv_dbcs_brst]
      
      
      MMS4 FPI/DIS ion bulk-velocity estimated spintone vector in DBCS during this burst [mms4_dis_bulkv_spintone_dbcs_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS4 FPI/DIS ion bulk-velocity DBCS vector during this burst [mms4_dis_bulkv_dbcs_brst_noerr]
      
      
      MMS4 FPI/DIS ion bulk-velocity GSE vector during this burst [mms4_dis_bulkv_gse_brst]
      
      
      MMS4 FPI/DIS ion bulk-velocity estimated spintone vector in GSE during this burst [mms4_dis_bulkv_spintone_gse_brst]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS4 FPI/DIS ion bulk-velocity GSE vector during this burst [mms4_dis_bulkv_gse_brst_noerr]
      
      
      MMS4 FPI/DIS ion bulk-velocity spintone vector in DBCS during this burst [mms4_dis_bulkv_spin_dbcs_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS4 FPI/DIS ion bulk-velocity spintone vector in GSE during this burst [mms4_dis_bulkv_spin_gse_brst]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS4 FPI/DIS ion pressure tensor DBCS matrix during this burst [mms4_dis_prestensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS ion pressure tensor GSE matrix during this burst [mms4_dis_prestensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS ion background pressure during this survey [mms4_dis_pres_bg_brst]
      
      
      MMS4 FPI/DIS ion temperature tensor DBCS matrix during this burst [mms4_dis_temptensor_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS ion temperature tensor GSE matrix during this burst [mms4_dis_temptensor_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS ion heat-flux DBCS vector during this burst [mms4_dis_heatq_dbcs_brst]
      
      
      MMS4 FPI/DIS ion heat-flux GSE vector during this burst [mms4_dis_heatq_gse_brst]
      
      
      MMS4 FPI/DIS ion parallel temperature during this BP [mms4_dis_temppara_brst]
      
      
      MMS4 FPI/DIS ion perpendicular temperature during this BP [mms4_dis_tempperp_brst]
      
      
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MMS4_FPI_BRST_L2_DIS-PARTMOMS (spase://NASA/NumericalData/MMS/4/FastPlasmaInvestigation/DIS/Burst/Level2/PartialMoments/PT0.15S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s,
etc) resolution.  Per mission design, not all burst-resolution data are
downlinked, but all survey data are downlinked. Planning around calibration
activities, avoidance of Earth radiation belts, etc, when possible, FPI usually
operates in Slow Survey (SS) Mode outside of ROI, and then only the 60 s
resolution survey data are available. This product contains partial moments that
come from performing the standard moment integrals over a limited portion of
velocity space. The resulting quantities are named similarly to their
corresponding standard moments, but are decorated with 'part' to differentiate.
For example, density_part is the density moment integrated from a particular
energy step to infinity. These partial moments are formed from the indicated
data type (DES/DIS burst, FS or SS). For convenience, some additional parameters
are included to augment those most commonly found in a moments product of this
sort, plus time-stamps and other annotation characterizing the state of the
instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DIS vector of data-quality indicators at burst-start time [mms4_dis_errorflags_brst]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation
      
      MMS4 FPI/DIS partial ion number density during this burst [mms4_dis_numberdensity_part_brst]
      
      
      MMS4 FPI/DIS partial ion bulk-velocity vector in DBCS during this burst [mms4_dis_bulkv_part_dbcs_brst]
      
      
      MMS4 FPI/DIS partial ion bulk-velocity vector in GSE during this burst [mms4_dis_bulkv_part_gse_brst]
      
      
      MMS4 FPI/DIS partial ion pressure tensor in DBCS during this burst [mms4_dis_prestensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS partial ion pressure tensor in GSE during this burst [mms4_dis_prestensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS partial ion temperature tensor in DBCS during this burst [mms4_dis_temptensor_part_dbcs_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS partial ion temperature tensor in GSE during this burst [mms4_dis_temptensor_part_gse_brst]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS partial ion parallel temperature during this burst [mms4_dis_temppara_part_brst]
      
      
      MMS4 FPI/DIS partial ion perpendicular temperature during this burst [mms4_dis_tempperp_part_brst]
      
      
      MMS4 FPI/DIS recommended energy index during this burst [mms4_dis_part_index_brst]
      Recommended energy index during this burst
      
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MMS4_FPI_FAST_L2_DES-DIST (spase://NASA/NumericalData/MMS/4/FastPlasmaInvestigation/DES/Fast/Level2/Distribution/PT4.5S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data taken at burst (30/150 ms for DES/DIS)
resolution are aggregated on board and made available at survey (4.5 s)
resolution in this mode.  This product contains phase-space distribution maps of
results from surveying the high-resolution observations during each 4.5 s
period.  In particular, the (highest possible quality at the time of release)
corrected/converted "Fast Survey SkyMap" distributions are reported with
time-stamps and other annotation characterizing the state of the instrument
system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DES fast sky-map instrument distribution - 11.6 eV (E1) using averaged even/odd steps [mms4_des_dist_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 11.6 eV [mms4_des_dist_fast1_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES fast sky-map instrument distribution - 40.4 eV (E6) using averaged even/odd steps [mms4_des_dist_fast6]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 40.4 eV [mms4_des_dist_fast6_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES fast sky-map instrument distribution - 85.1 eV (E9) using averaged even/odd steps [mms4_des_dist_fast9]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 85.1 eV [mms4_des_dist_fast9_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES fast sky-map instrument distribution - 179 eV (E12) using averaged even/odd steps [mms4_des_dist_fast12]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 179 eV [mms4_des_dist_fast12_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES fast sky-map instrument distribution - 295 eV (E14) using averaged even/odd steps [mms4_des_dist_fast14]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 295 eV [mms4_des_dist_fast14_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES fast sky-map instrument distribution - 485 eV (E16) using averaged even/odd steps [mms4_des_dist_fast16]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 485 eV [mms4_des_dist_fast16_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES fast sky-map instrument distribution - 798 eV (E18) using averaged even/odd steps [mms4_des_dist_fast18]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 798 eV [mms4_des_dist_fast18_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES fast sky-map instrument distribution - 1310 eV (E20) using averaged even/odd steps [mms4_des_dist_fast20]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1310 eV [mms4_des_dist_fast20_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES fast sky-map instrument distribution - 2770 eV (E23) using averaged even/odd steps [mms4_des_dist_fast23]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2770 eV [mms4_des_dist_fast23_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES fast sky-map instrument distribution - 5840 eV (E26) using averaged even/odd steps [mms4_des_dist_fast26]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5840 eV [mms4_des_dist_fast26_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES fast sky-map instrument distribution - 26000 eV (E32) using averaged even/odd steps [mms4_des_dist_fast32]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 26000 eV [mms4_des_dist_fast32_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [Only List/Create in CDAWeb] MMS4 FPI/DES fast sky-map instrument distribution 1-sigma error [mms4_des_disterr_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES vector of data-quality indicators at fast survey-start time - 32-bit error flags [mms4_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS4 FPI/DES compression lossless/lossy indicator at survey-start time [mms4_des_compressionloss_fast]
      FPI/DES compression loss indicator,0=lossless, 1=lossy
      
      ---> MMS4 FPI/DES Del-Phi (obs spin-phase) count at fast survey-start time [mms4_des_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS4 FPI/DES Del-Phi (obs spin-phase) angle at fast survey-start time [mms4_des_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS4 FPI/DES fast survey average f1 count values [mms4_des_avgf1counts_fast]
      Average f1-count level as a function of energy
      
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MMS4_FPI_FAST_L2_DES-MOMS (spase://NASA/NumericalData/MMS/4/FastPlasmaInvestigation/DES/Fast/Level2/Moments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution.  Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This moments product
contains results from integrating the standard moments of phase-space
distributions formed from the indicated data type (DES/DIS burst, FS or SS). For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotation characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DES 32-bit vector of data-quality indicators at survey-start time [mms4_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>25%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of brst l2pre
      magnetic field, Bit-9 = srvy l2pre magnetic field used instead of brst l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied
      
      ---> MMS4 FPI/DES compression lossless/lossy indicator at survey-start time [mms4_des_compressionloss_fast]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS4 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms4_des_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS4 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms4_des_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS4 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms4_des_pitchangdist_lowen_fast]
      low energy bin: 0 eV - 200 eV.  pitch-angle bin size: 6 deg.
      
      ---> MMS4 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms4_des_pitchangdist_miden_fast]
      mid energy bin: 200 eV - 2 keV.  pitch-angle bin size: 6 deg.
      
      ---> MMS4 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms4_des_pitchangdist_highen_fast]
      high energy bin: 2 keV - 30 keV.  pitch-angle bin size: 6 deg.
      
      MMS4 FPI/DES electron energy spectrum "near" +X_DSC during this survey [mms4_des_energyspectr_px_fast]
      Counts, summed over DSC velocity-dirs closest to +X_DSC, by energy bin.
      
      ---> MMS4 FPI/DES electron energy spectrum "near" -X_DSC during this survey [mms4_des_energyspectr_mx_fast]
      Counts, summed over DSC velocity-dirs closest to -X_DSC, by energy bin.
      
      ---> MMS4 FPI/DES electron energy spectrum "near" +Y_DSC during this survey [mms4_des_energyspectr_py_fast]
      Counts, summed over DSC velocity-dirs closest to +Y_DSC, by energy bin.
      
      ---> MMS4 FPI/DES electron energy spectrum "near" -Y_DSC during this survey [mms4_des_energyspectr_my_fast]
      Counts, summed over DSC velocity-dirs closest to -Y_DSC, by energy bin.
      
      ---> MMS4 FPI/DES electron energy spectrum "near" +Z_DSC during this survey [mms4_des_energyspectr_pz_fast]
      Counts, summed over DSC velocity-dirs closest to +Z_DSC, by energy bin.
      
      ---> MMS4 FPI/DES electron energy spectrum "near" -Z_DSC during this survey [mms4_des_energyspectr_mz_fast]
      Counts, summed over DSC velocity-dirs closest to -Z_DSC, by energy bin.
      
      MMS4 FPI/DES electron energy parallel spectrum 30 degrees parallel to B during this survey [mms4_des_energyspectr_par_fast]
      Counts, summed within 30 degrees parallel bentPipe magnetic field.
      
      ---> MMS4 FPI/DES electron energy anti-parallel spectrum 30 degrees anti-parallel to B during this survey [mms4_des_energyspectr_anti_fast]
      Counts, summed within 30 degrees antiparallel to bentPipe magnetic field.
      
      ---> MMS4 FPI/DES electron energy perpendicular spectrum 60 degrees perpendicular to B during this survey [mms4_des_energyspectr_perp_fast]
      Counts, summed within 60 degrees perpendicular to bentPipe magnetic field.
      
      MMS4 FPI/DES omni-directional electron energy spectrum during this survey [mms4_des_energyspectr_omni_fast]
      Differential energy flux, averaged (weighted by solid angle) over all look
      directions, by energy bin.
      
      MMS4 FPI/DES electron number density during this survey [mms4_des_numberdensity_fast]
      
      
      ---> (no error bars displayed) MMS4 FPI/DES electron number density during this survey [mms4_des_numberdensity_fast_noerr]
      
      
      ---> MMS4 FPI/DES electron number density error during this survey [mms4_des_numberdensity_err_fast]
      
      
      MMS4 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms4_des_densityextrapolation_low_fast]
      
      
      MMS4 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms4_des_densityextrapolation_high_fast]
      
      
      MMS4 FPI/DES electron bulk-velocity DBCS vector during this survey [mms4_des_bulkv_dbcs_fast]
      
      
      MMS4 FPI/DES electron bulk-velocity estimated spintone vector in DBCS during this survey [mms4_des_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS4 FPI/DES electron bulk-velocity DBCS vector during this survey [mms4_des_bulkv_dbcs_fast_noerr]
      
      
      MMS4 FPI/DES electron bulk-velocity GSE vector during this survey [mms4_des_bulkv_gse_fast]
      
      
      MMS4 FPI/DES electron bulk-velocity estimated spintone vector in GSE during this survey [mms4_des_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS4 FPI/DES electron bulk-velocity GSE vector during this survey [mms4_des_bulkv_gse_fast_noerr]
      
      
      MMS4 FPI/DES electron bulk-velocity spintone vector in DBCS during this survey [mms4_des_bulkv_spin_dbcs_fast]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS4 FPI/DES electron bulk-velocity spintone vector in GSE during this survey [mms4_des_bulkv_spin_gse_fast]
      Estimated error in spin-plane bulk velocity (km/s) due to imperfect sensor suite
      flat-fielding
      
      MMS4 FPI/DES electron pressure tensor DBCS matrix during this survey [mms4_des_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES electron pressure tensor GSE matrix during this survey [mms4_des_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES electron temperature tensor DBCS matrix during this survey [mms4_des_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES electron temperature tensor GSE matrix during this survey [mms4_des_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES electron heat-flux DBCS vector during this survey [mms4_des_heatq_dbcs_fast]
      
      
      MMS4 FPI/DES electron heat-flux GSE vector during this survey [mms4_des_heatq_gse_fast]
      
      
      MMS4 FPI/DES electron parallel temperature during this BP [mms4_des_temppara_fast]
      
      
      MMS4 FPI/DES electron perpendicular temperature during this BP [mms4_des_tempperp_fast]
      
      
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MMS4_FPI_FAST_L2_DES-MOMSAUX
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DES vector of data-quality indicators at survey-start time [mms4_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only)
      
      MMS4 FPI/DES partial electron number density during this survey [mms4_des_numberdensity_part_fast]
      
      
      MMS4 FPI/DES partial electron bulk-velocity vector in DBCS during this survey [mms4_des_bulkv_part_dbcs_fast]
      
      
      MMS4 FPI/DES partial electron bulk-velocity vector in GSE during this survey [mms4_des_bulkv_part_gse_fast]
      
      
      MMS4 FPI/DES partial electron pressure tensor in DBCS during this survey [mms4_des_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES partial electron pressure tensor in GSE during this survey [mms4_des_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES partial electron temperature tensor in DBCS during this survey [mms4_des_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES partial electron temperature tensor in GSE during this survey [mms4_des_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES partial electron parallel temperature during this survey [mms4_des_temppara_part_fast]
      
      
      MMS4 FPI/DES partial electron perpendicular temperature during this survey [mms4_des_tempperp_part_fast]
      
      
      MMS4 FPI/DES recommended energy index for partial moments during this survey [mms4_des_part_index_fast]
      Recommended energy index during this survey
      
      MMS4 FPI/DES compression lossless/lossy indicator at survey-start time [mms4_des_compressionloss_fast]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS4 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms4_des_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS4 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms4_des_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS4 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms4_des_pitchangdist_lowen_fast]
      Low energy bin: energy steps 0-10 (of total steps 0-31). Pitch-angle bin size: 6
      deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS4 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms4_des_pitchangdist_miden_fast]
      Mid energy bin: energy steps 11-20 (of total steps 0-31). Pitch-angle bin size:
      6 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS4 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms4_des_pitchangdist_highen_fast]
      High energy bin: energy steps 21-31 (of total steps 0-31). Pitch-angle bin size:
      6 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS4 FPI/DES electron energy spectrum "near" +X_DBCS during this survey [mms4_des_energyspectr_px_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS4 FPI/DES electron energy spectrum "near" -X_DBCS during this survey [mms4_des_energyspectr_mx_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS4 FPI/DES electron energy spectrum "near" +Y_DBCS during this survey [mms4_des_energyspectr_py_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS4 FPI/DES electron energy spectrum "near" -Y_DBCS during this survey [mms4_des_energyspectr_my_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS4 FPI/DES electron energy spectrum "near" +Z_DBCS during this survey [mms4_des_energyspectr_pz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS4 FPI/DES electron energy spectrum "near" -Z_DBCS during this survey [mms4_des_energyspectr_mz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS4 FPI/DES electron energy parallel to the magnetic field direction during this survey [mms4_des_energyspectr_par_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within 30
      degrees of the magnetic field direction.
      
      MMS4 FPI/DES electron energy anti-parallel to the magnetic field direction during this survey [mms4_des_energyspectr_anti_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      150 degrees of the magnetic field direction.
      
      MMS4 FPI/DES electron energy perpendicular to the magnetic field direction during this survey [mms4_des_energyspectr_perp_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      60-120 degrees of the magnetic field direction.
      
      MMS4 FPI/DES omni-directional electron energy spectrum during this survey [mms4_des_energyspectr_omni_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS4 FPI/DES electron number density during this survey [mms4_des_numberdensity_fast]
      
      
      MMS4 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms4_des_densityextrapolation_low_fast]
      
      
      MMS4 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms4_des_densityextrapolation_high_fast]
      
      
      MMS4 FPI/DES electron bulk-velocity vector in DBCS during this survey [mms4_des_bulkv_dbcs_fast]
      
      
      MMS4 FPI/DES electron bulk-velocity estimated spintone vector in DBCS during this survey [mms4_des_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS4 FPI/DES electron bulk-velocity vector in GSE during this survey [mms4_des_bulkv_gse_fast]
      
      
      MMS4 FPI/DES electron bulk-velocity estimated spintone vector in GSE during this survey [mms4_des_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS4 FPI/DES electron pressure tensor in DBCS during this survey [mms4_des_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES electron pressure tensor in GSE during this survey [mms4_des_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES electron temperature tensor in DBCS during this survey [mms4_des_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES electron temperature tensor in GSE during this survey [mms4_des_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES electron heat-flux vector in DBCS during this survey [mms4_des_heatq_dbcs_fast]
      
      
      MMS4 FPI/DES electron heat-flux vector in GSE during this survey [mms4_des_heatq_gse_fast]
      
      
      MMS4 FPI/DES electron parallel temperature during this BP [mms4_des_temppara_fast]
      
      
      MMS4 FPI/DES electron perpendicular temperature during this BP [mms4_des_tempperp_fast]
      
      
      MMS4 FPI/DES S/C potential mean [mms4_des_scpot_mean_fast]
      Average spacecraft potential during this FP used to shift the measure energies.
      
      MMS4 FPI/DES S/C potential max [mms4_des_scpot_max_fast]
      Maximum spacecraft potential during this FP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      MMS4 FPI/DES Mag data X,Y,Z,Norm DSC components [nT] at survey-start time [mms4_des_fpibentpipe_dsc_fast]
      X, Y, Z are unit vector components.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms4_des_fpib_gse_srvy_fast]
      Averaged survey magnetic field data during this FP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms4_des_fpib_dmpa_srvy_fast]
      Averaged survey magnetic field data during this FP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms4_des_pos_gse_fast]
      
      
      Position in GSM coordinates, 30 second [mms4_des_pos_gsm_fast]
      
      
      MMS4 number density integrands [mms4_des_numberdensity_int_fast]
      Integrand terms used in normalized energy integration for number density
      
      number flux [mms4_des_numberflux_int_dbcs_fast]
      Integrand terms used in normalized energy integration for number flux
      
      MMS4 pressure tensor integrands [mms4_des_prestensor_int_dbcs_fast]
      Integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms4_des_ugrid_int_fast]
      
      
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MMS4_FPI_FAST_L2_DES-PARTMOMS (spase://NASA/NumericalData/MMS/4/FastPlasmaInvestigation/DES/Fast/Level2/PartialMoments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DES vector of data-quality indicators at survey-start time [mms4_des_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only)
      
      MMS4 FPI/DES partial electron number density during this survey [mms4_des_numberdensity_part_fast]
      
      
      MMS4 FPI/DES partial electron bulk-velocity vector in DBCS during this survey [mms4_des_bulkv_part_dbcs_fast]
      
      
      MMS4 FPI/DES partial electron bulk-velocity vector in GSE during this survey [mms4_des_bulkv_part_gse_fast]
      
      
      MMS4 FPI/DES partial electron pressure tensor in DBCS during this survey [mms4_des_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES partial electron pressure tensor in GSE during this survey [mms4_des_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES partial electron temperature tensor in DBCS during this survey [mms4_des_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES partial electron temperature tensor in GSE during this survey [mms4_des_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES partial electron parallel temperature during this survey [mms4_des_temppara_part_fast]
      
      
      MMS4 FPI/DES partial electron perpendicular temperature during this survey [mms4_des_tempperp_part_fast]
      
      
      MMS4 FPI/DES recommended energy index during this survey [mms4_des_part_index_fast]
      Recommended energy index during this survey
      
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MMS4_FPI_FAST_L2_DIS-DIST (spase://NASA/NumericalData/MMS/4/FastPlasmaInvestigation/DIS/Fast/Level2/Distribution/PT4.5S)
Description
FPI usually operates in Fast Survey Mode in the MMS Region Of Interest (ROI) for
the current Mission Phase.  Data taken at burst (30/150 ms for DES/DIS)
resolution are aggregated on board and made available at survey (4.5 s)
resolution in this mode.  This product contains phase-space distribution maps of
results from surveying the high-resolution observations during each 4.5 s
period.  In particular, the (highest possible quality at the time of release)
corrected/converted "Fast Survey SkyMap" distributions are reported with
time-stamps and other annotation characterizing the state of the instrument
system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DIS fast sky-map instrument distribution - 11.3 eV (E1) using averaged even/odd steps [mms4_dis_dist_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 11.3 eV [mms4_dis_dist_fast1_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS fast sky-map instrument distribution - 39.6 eV (E6) using averaged even/odd steps [mms4_dis_dist_fast6]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 39.6 eV [mms4_dis_dist_fast6_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS fast sky-map instrument distribution - 83.9 eV (E9 using averaged even/odd steps) [mms4_dis_dist_fast9]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 83.9 eV [mms4_dis_dist_fast9_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS fast sky-map instrument distribution - 178 eV (E12) using averaged even/odd steps [mms4_dis_dist_fast12]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 178 eV [mms4_dis_dist_fast12_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS fast sky-map instrument distribution - 293 eV (E14) using averaged even/odd steps [mms4_dis_dist_fast14]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 293 eV [mms4_dis_dist_fast14_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS fast sky-map instrument distribution - 484 eV (E16) using averaged even/odd steps [mms4_dis_dist_fast16]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 484 eV [mms4_dis_dist_fast16_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS fast sky-map instrument distribution - 799 eV (E18) using averaged even/odd steps [mms4_dis_dist_fast18]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 799 eV [mms4_dis_dist_fast18_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS fast sky-map instrument distribution - 1320 eV (E20) using averaged even/odd steps [mms4_dis_dist_fast20]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 1320 eV [mms4_dis_dist_fast20_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS fast sky-map instrument distribution - 2800 eV (E23) using averaged even/odd steps [mms4_dis_dist_fast23]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 2800 eV [mms4_dis_dist_fast23_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS fast sky-map instrument distribution - 5920 eV (E26) using averaged even/odd steps [mms4_dis_dist_fast26]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 5920 eV [mms4_dis_dist_fast26_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS fast sky-map instrument distribution - 26600 eV (E32) using averaged even/odd steps [mms4_dis_dist_fast32]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      ---> Movie - 26600 eV [mms4_dis_dist_fast32_movie]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      [Only List/Create in CDAWeb] MMS4 FPI/DIS fast sky-map instrument distribution 1-sigma error [mms4_dis_disterr_fast]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=31 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS vector of data-quality indicators at fast survey-start time - 32-bit error flags [mms4_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap
      
      ---> MMS4 FPI/DIS compression lossless/lossy indicator at survey-start time [mms4_dis_compressionloss_fast]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      ---> MMS4 FPI/DIS Del-Phi (obs spin-phase) count at fast survey-start time [mms4_dis_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase count indicates
      obs +X-axis aligned with Sun.
      
      ---> MMS4 FPI/DIS Del-Phi (obs spin-phase) angle at fast survey-start time [mms4_dis_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with Sun.
      
      MMS4 FPI/DIS fast survey average f1 count values [mms4_dis_avgf1counts_fast]
      Average f1-count level as a function of energy
      
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MMS4_FPI_FAST_L2_DIS-MOMS (spase://NASA/NumericalData/MMS/4/FastPlasmaInvestigation/DIS/Fast/Level2/Moments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution.  Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This moments product
contains results from integrating the standard moments of phase-space
distributions formed from the indicated data type (DES/DIS burst, FS or SS). For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotation characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DIS vector of data-quality indicators at survey-start time [mms4_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation, Bit-14 =
      high MMS3 spintone due to DIS008 anomaly
      
      ---> MMS4 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms4_dis_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      ---> MMS4 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms4_dis_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS4 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms4_dis_energyspectr_px_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      ---> MMS4 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms4_dis_energyspectr_mx_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      ---> MMS4 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms4_dis_energyspectr_py_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      ---> MMS4 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms4_dis_energyspectr_my_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      ---> MMS4 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms4_dis_energyspectr_pz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      ---> MMS4 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms4_dis_energyspectr_mz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS4 FPI/DIS omni-directional ion energy spectrum during this survey [mms4_dis_energyspectr_omni_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS4 FPI/DIS ion background energy during this survey [mms4_dis_spectr_bg_fast]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS4 FPI/DIS ion background number density during this survey [mms4_dis_numberdensity_bg_fast]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS4 FPI/DIS ion number density during this survey [mms4_dis_numberdensity_fast]
      
      
      ---> (no error bars displayed) MMS4 FPI/DIS ion number density during this survey [mms4_dis_numberdensity_fast_noerr]
      
      
      MMS4 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms4_dis_densityextrapolation_low_fast]
      
      
      MMS4 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms4_dis_densityextrapolation_high_fast]
      
      
      MMS4 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms4_dis_bulkv_dbcs_fast]
      
      
      ---> (no error bars displayed) MMS4 FPI/DIS ion bulk-velocity DBCS vector during this survey [mms4_dis_bulkv_dbcs_fast_noerr]
      
      
      MMS4 FPI/DIS ion bulk-velocity estimated spintone vector in DBCS during this survey [mms4_dis_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS4 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms4_dis_bulkv_gse_fast]
      
      
      MMS4 FPI/DIS ion bulk-velocity estimated spintone vector in GSE during this survey [mms4_dis_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      ---> (no error bars displayed) MMS4 FPI/DIS ion bulk-velocity GSE vector during this survey [mms4_dis_bulkv_gse_fast_noerr]
      
      
      MMS4 FPI/DIS ion pressure tensor in DBCS during this survey [mms4_dis_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS ion pressure tensor in GSE during this survey [mms4_dis_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS ion background pressure during this survey [mms4_dis_pres_bg_fast]
      
      
      MMS4 FPI/DIS ion temperature tensor in DBCS during this survey [mms4_dis_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS ion temperature tensor in GSE during this survey [mms4_dis_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS ion heat-flux vector in DBCS during this survey [mms4_dis_heatq_dbcs_fast]
      
      
      MMS4 FPI/DIS ion heat-flux vector in GSE during this survey [mms4_dis_heatq_gse_fast]
      
      
      MMS4 FPI/DIS ion parallel temperature during this BP [mms4_dis_temppara_fast]
      
      
      MMS4 FPI/DIS ion perpendicular temperature during this BP [mms4_dis_tempperp_fast]
      
      
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MMS4_FPI_FAST_L2_DIS-MOMSAUX
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DIS vector of data-quality indicators at survey-start time [mms4_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation
      
      MMS4 FPI/DIS partial ion number density during this survey [mms4_dis_numberdensity_part_fast]
      
      
      MMS4 FPI/DIS partial ion bulk-velocity vector in DBCS during this survey [mms4_dis_bulkv_part_dbcs_fast]
      
      
      MMS4 FPI/DIS partial ion bulk-velocity vector in GSE during this survey [mms4_dis_bulkv_part_gse_fast]
      
      
      MMS4 FPI/DIS partial ion pressure tensor in DBCS during this survey [mms4_dis_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS partial ion pressure tensor in GSE during this survey [mms4_dis_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS partial ion temperature tensor in DBCS during this survey [mms4_dis_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS partial ion temperature tensor in GSE during this survey [mms4_dis_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS partial ion parallel temperature during this survey [mms4_dis_temppara_part_fast]
      
      
      MMS4 FPI/DIS partial ion perpendicular temperature during this survey [mms4_dis_tempperp_part_fast]
      
      
      MMS4 FPI/DIS recommended energy index for partial moments during this survey [mms4_dis_part_index_fast]
      Recommended energy index during this survey
      
      MMS4 FPI/DIS compression lossless/lossy indicator at survey-start time [mms4_dis_compressionloss_fast]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS4 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms4_dis_startdelphi_count_fast]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS4 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms4_dis_startdelphi_angle_fast]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS4 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms4_dis_energyspectr_px_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms4_dis_energyspectr_mx_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms4_dis_energyspectr_py_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms4_dis_energyspectr_my_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms4_dis_energyspectr_pz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms4_dis_energyspectr_mz_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS4 FPI/DIS omni-directional ion energy spectrum during this survey [mms4_dis_energyspectr_omni_fast]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS4 FPI/DIS ion background energy during this survey [mms4_dis_spectr_bg_fast]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS4 FPI/DIS ion background number density during this survey [mms4_dis_numberdensity_bg_fast]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS4 FPI/DIS ion number density during this survey [mms4_dis_numberdensity_fast]
      
      
      MMS4 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms4_dis_densityextrapolation_low_fast]
      
      
      MMS4 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms4_dis_densityextrapolation_high_fast]
      
      
      MMS4 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms4_dis_bulkv_dbcs_fast]
      
      
      MMS4 FPI/DIS ion bulk-velocity estimated spintone vector in DBCS during this survey [mms4_dis_bulkv_spintone_dbcs_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS4 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms4_dis_bulkv_gse_fast]
      
      
      MMS4 FPI/DIS ion bulk-velocity estimated spintone vector in GSE during this survey [mms4_dis_bulkv_spintone_gse_fast]
      Estimated systematic error (positive or negative) in spin-plane bulk velocity
      (km/s) due to imperfect sensor suite flat-fielding. This can be subtracted from
      bulk velocity to obtain the corrected velocity vector.
      
      MMS4 FPI/DIS ion pressure tensor in DBCS during this survey [mms4_dis_prestensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS ion pressure tensor in GSE during this survey [mms4_dis_prestensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS ion background pressure during this survey [mms4_dis_pres_bg_fast]
      
      
      MMS4 FPI/DIS ion temperature tensor in DBCS during this survey [mms4_dis_temptensor_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS ion temperature tensor in GSE during this survey [mms4_dis_temptensor_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS ion heat-flux vector in DBCS during this survey [mms4_dis_heatq_dbcs_fast]
      
      
      MMS4 FPI/DIS ion heat-flux vector in GSE during this survey [mms4_dis_heatq_gse_fast]
      
      
      MMS4 FPI/DIS ion parallel temperature during this BP [mms4_dis_temppara_fast]
      
      
      MMS4 FPI/DIS ion perpendicular temperature during this BP [mms4_dis_tempperp_fast]
      
      
      MMS4 FPI/DIS S/C potential mean [mms4_dis_scpot_mean_fast]
      Average spacecraft potential during this FP used to shift the measure energies.
      
      MMS4 FPI/DIS S/C potential max [mms4_dis_scpot_max_fast]
      Maximum spacecraft potential during this FP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      MMS4 FPI/DIS Mag data X,Y,Z,Norm DSC components [nT] at survey-start time [mms4_dis_fpibentpipe_dsc_fast]
      X, Y, Z are unit vector components.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms4_dis_fpib_gse_srvy_fast]
      Averaged survey magnetic field data during this FP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms4_dis_fpib_dmpa_srvy_fast]
      Averaged survey magnetic field data during this FP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms4_dis_pos_gse_fast]
      
      
      Position in GSM coordinates, 30 second [mms4_dis_pos_gsm_fast]
      
      
      MMS4 number density integrands [mms4_dis_numberdensity_int_fast]
      integrand terms used in normalized energy integration for number density
      
      number flux [mms4_dis_numberflux_int_dbcs_fast]
      integrand terms used in normalized energy integration for number flux
      
      MMS4 pressure tensor integrands [mms4_dis_prestensor_int_dbcs_fast]
      integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms4_dis_ugrid_int_fast]
      
      
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MMS4_FPI_FAST_L2_DIS-PARTMOMS (spase://NASA/NumericalData/MMS/4/FastPlasmaInvestigation/DIS/Fast/Level2/PartialMoments/PT4.5S)
Description
FPI usually operates in Fast Survey (FS) Mode in the MMS Region Of Interest
(ROI) for the current Mission Phase. Data are taken at burst (30/150 ms for
DES/DIS) resolution in this mode. Data are also made available at survey (4.5 s)
resolution. Per mission design, not all burst-resolution data are downlinked,
but all survey data are downlinked. Planning around calibration activities,
avoidance of Earth radiation belts, etc, when possible, FPI usually operates in
Slow Survey (SS) Mode (60 s resolution) outside of ROI. This product contains
partial moments that come from performing the standard moment integrals over a
limited portion of velocity space. The resulting quantities are named similarly
to their corresponding standard moments, but are decorated with 'part' to
differentiate. For example, density_part is the density moment integrated from a
particular energy step to infinity. These partial moments are formed from the
indicated data type (DES/DIS burst, FS or SS). For convenience, some additional
parameters are included to augment those most commonly found in a moments
product of this sort, plus time-stamps and other annotation characterizing the
state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DIS vector of data-quality indicators at survey-start time [mms4_dis_errorflags_fast]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = bentPipe magnetic field used instead of srvy l2pre
      magnetic field, Bit-10 = no internally generated photoelectron correction
      applied, Bit-11 = compression pipeline error, Bit-12 = spintone calculation
      error (DBCS only), Bit-13 = significant (>=20%) penetrating radiation
      
      MMS4 FPI/DIS partial ion number density during this survey [mms4_dis_numberdensity_part_fast]
      
      
      MMS4 FPI/DIS partial ion bulk-velocity vector in DBCS during this survey [mms4_dis_bulkv_part_dbcs_fast]
      
      
      MMS4 FPI/DIS partial ion bulk-velocity vector in GSE during this survey [mms4_dis_bulkv_part_gse_fast]
      
      
      MMS4 FPI/DIS partial ion pressure tensor in DBCS during this survey [mms4_dis_prestensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS partial ion pressure tensor in GSE during this survey [mms4_dis_prestensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS partial ion temperature tensor in DBCS during this survey [mms4_dis_temptensor_part_dbcs_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS partial ion temperature tensor in GSE during this survey [mms4_dis_temptensor_part_gse_fast]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS partial ion parallel temperature during this survey [mms4_dis_temppara_part_fast]
      
      
      MMS4 FPI/DIS partial ion perpendicular temperature during this survey [mms4_dis_tempperp_part_fast]
      
      
      MMS4 FPI/DIS recommended energy index during this survey [mms4_dis_part_index_fast]
      Recommended energy index during this survey
      
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MMS4_FPI_SLOW_L2_DES-DIST
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode.  This product contains phase-space distribution maps of those
survey-resolution data from Slow Mode.  In particular, the (highest possible
quality at the time of release) corrected/converted "Slow Survey SkyMap"
distributions are reported with time-stamps and other annotation characterizing
the state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DES vector of data-quality indicators at survey-start time [mms4_des_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = compression pipeline error
      
      MMS4 FPI/DES compression lossless/lossy indicator at survey-start time [mms4_des_compressionloss_slow]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS4 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms4_des_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS4 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms4_des_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS4 FPI/DES Slow Survey sky-map instrument distribution [mms4_des_dist_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES Slow Survey sky-map instrument distribution 1-sigma error [mms4_des_disterr_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DES slow survey average f1 count values [mms4_des_avgf1counts_slow]
      Average f1-count level as a function of energy
      
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MMS4_FPI_SLOW_L2_DES-MOMS
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DES vector of data-quality indicators at survey-start time [mms4_des_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only)
      
      MMS4 FPI/DES compression lossless/lossy indicator at survey-start time [mms4_des_compressionloss_slow]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS4 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms4_des_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS4 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms4_des_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS4 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms4_des_pitchangdist_lowen_slow]
      Low energy bin: energy steps 0-10 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS4 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms4_des_pitchangdist_miden_slow]
      Mid energy bin: energy steps 11-20 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS4 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms4_des_pitchangdist_highen_slow]
      High energy bin: energy steps 21-31 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS4 FPI/DES electron energy spectrum "near" +X_DBCS during this survey [mms4_des_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS4 FPI/DES electron energy spectrum "near" -X_DBCS during this survey [mms4_des_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS4 FPI/DES electron energy spectrum "near" +Y_DBCS during this survey [mms4_des_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS4 FPI/DES electron energy spectrum "near" -Y_DBCS during this survey [mms4_des_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS4 FPI/DES electron energy spectrum "near" +Z_DBCS during this survey [mms4_des_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS4 FPI/DES electron energy spectrum "near" -Z_DBCS during this survey [mms4_des_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS4 FPI/DES electron energy parallel to the magnetic field direction during this survey [mms4_des_energyspectr_par_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within 30
      degrees of the magnetic field direction.
      
      MMS4 FPI/DES electron energy anti-parallel to the magnetic field direction during this survey [mms4_des_energyspectr_anti_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      150 degrees of the magnetic field direction.
      
      MMS4 FPI/DES electron energy perpendicular to the magnetic field direction during this survey [mms4_des_energyspectr_perp_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      60-120 degrees of the magnetic field direction.
      
      MMS4 FPI/DES omni-directional electron energy spectrum during this survey [mms4_des_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS4 FPI/DES electron number density during this survey [mms4_des_numberdensity_slow]
      
      
      MMS4 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms4_des_densityextrapolation_low_slow]
      
      
      MMS4 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms4_des_densityextrapolation_high_slow]
      
      
      MMS4 FPI/DES electron bulk-velocity vector in DBCS during this survey [mms4_des_bulkv_dbcs_slow]
      
      
      MMS4 FPI/DES electron bulk-velocity vector in GSE during this survey [mms4_des_bulkv_gse_slow]
      
      
      MMS4 FPI/DES electron pressure tensor in DBCS during this survey [mms4_des_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES electron pressure tensor in GSE during this survey [mms4_des_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES electron temperature tensor in DBCS during this survey [mms4_des_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES electron temperature tensor in GSE during this survey [mms4_des_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES electron heat-flux vector in DBCS during this survey [mms4_des_heatq_dbcs_slow]
      
      
      MMS4 FPI/DES electron heat-flux vector in GSE during this survey [mms4_des_heatq_gse_slow]
      
      
      MMS4 FPI/DES electron parallel temperature during this BP [mms4_des_temppara_slow]
      
      
      MMS4 FPI/DES electron perpendicular temperature during this BP [mms4_des_tempperp_slow]
      
      
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MMS4_FPI_SLOW_L2_DES-MOMSAUX
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DES vector of data-quality indicators at survey-start time [mms4_des_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DES < 0.05 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only)
      
      MMS4 FPI/DES partial electron number density during this survey [mms4_des_numberdensity_part_slow]
      
      
      MMS4 FPI/DES partial electron bulk-velocity vector in DBCS during this survey [mms4_des_bulkv_part_dbcs_slow]
      
      
      MMS4 FPI/DES partial electron bulk-velocity vector in GSE during this survey [mms4_des_bulkv_part_gse_slow]
      
      
      MMS4 FPI/DES partial electron pressure tensor in DBCS during this survey [mms4_des_prestensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES partial electron pressure tensor in GSE during this survey [mms4_des_prestensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES partial electron temperature tensor in DBCS during this survey [mms4_des_temptensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES partial electron temperature tensor in GSE during this survey [mms4_des_temptensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES partial electron parallel temperature during this survey [mms4_des_temppara_part_slow]
      
      
      MMS4 FPI/DES partial electron perpendicular temperature during this survey [mms4_des_tempperp_part_slow]
      
      
      MMS4 FPI/DES recommended energy index for partial moments during this survey [mms4_des_part_index_slow]
      Recommended energy index during this survey
      
      MMS4 FPI/DES compression lossless/lossy indicator at survey-start time [mms4_des_compressionloss_slow]
      FPI/DES compression loss indicator, 0=lossless, 1=lossy
      
      MMS4 FPI/DES Del-Phi (obs spin-phase) count at survey-start time [mms4_des_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS4 FPI/DES Del-Phi (obs spin-phase) angle at survey-start time [mms4_des_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS4 FPI/DES electron pitch-angle distribution for "low" energies during this survey [mms4_des_pitchangdist_lowen_slow]
      Low energy bin: energy steps 0-10 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS4 FPI/DES electron pitch-angle distribution for "mid" energies during this survey [mms4_des_pitchangdist_miden_slow]
      Mid energy bin: energy steps 11-20 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS4 FPI/DES electron pitch-angle distribution for "high" energies during this survey [mms4_des_pitchangdist_highen_slow]
      High energy bin: energy steps 21-31 (of total steps 0-31). Pitch-angle bin size:
      12 deg. Note that pitch angles are calculated in the spacecraft frame; i.e., not
      shifted by the bulk velocity.
      
      MMS4 FPI/DES electron energy spectrum "near" +X_DBCS during this survey [mms4_des_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS4 FPI/DES electron energy spectrum "near" -X_DBCS during this survey [mms4_des_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS4 FPI/DES electron energy spectrum "near" +Y_DBCS during this survey [mms4_des_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS4 FPI/DES electron energy spectrum "near" -Y_DBCS during this survey [mms4_des_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS4 FPI/DES electron energy spectrum "near" +Z_DBCS during this survey [mms4_des_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS4 FPI/DES electron energy spectrum "near" -Z_DBCS during this survey [mms4_des_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS4 FPI/DES electron energy parallel to the magnetic field direction during this survey [mms4_des_energyspectr_par_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within 30
      degrees of the magnetic field direction.
      
      MMS4 FPI/DES electron energy anti-parallel to the magnetic field direction during this survey [mms4_des_energyspectr_anti_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      150 degrees of the magnetic field direction.
      
      MMS4 FPI/DES electron energy perpendicular to the magnetic field direction during this survey [mms4_des_energyspectr_perp_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction (not instrument look direction) is within
      60-120 degrees of the magnetic field direction.
      
      MMS4 FPI/DES omni-directional electron energy spectrum during this survey [mms4_des_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS4 FPI/DES electron number density during this survey [mms4_des_numberdensity_slow]
      
      
      MMS4 FPI/DES estimated (via extrapolation to 0) contribution to density integral below 10eV [mms4_des_densityextrapolation_low_slow]
      
      
      MMS4 FPI/DES estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms4_des_densityextrapolation_high_slow]
      
      
      MMS4 FPI/DES electron bulk-velocity vector in DBCS during this survey [mms4_des_bulkv_dbcs_slow]
      
      
      MMS4 FPI/DES electron bulk-velocity vector in GSE during this survey [mms4_des_bulkv_gse_slow]
      
      
      MMS4 FPI/DES electron pressure tensor in DBCS during this survey [mms4_des_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES electron pressure tensor in GSE during this survey [mms4_des_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DES electron temperature tensor in DBCS during this survey [mms4_des_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES electron temperature tensor in GSE during this survey [mms4_des_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DES electron heat-flux vector in DBCS during this survey [mms4_des_heatq_dbcs_slow]
      
      
      MMS4 FPI/DES electron heat-flux vector in GSE during this survey [mms4_des_heatq_gse_slow]
      
      
      MMS4 FPI/DES electron parallel temperature during this BP [mms4_des_temppara_slow]
      
      
      MMS4 FPI/DES electron perpendicular temperature during this BP [mms4_des_tempperp_slow]
      
      
      MMS4 FPI/DES S/C potential mean [mms4_des_scpot_mean_slow]
      Average spacecraft potential during this SP used to shift the measure energies.
      
      MMS4 FPI/DES S/C potential max [mms4_des_scpot_max_slow]
      Maximum spacecraft potential during this SP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms4_des_fpib_gse_srvy_slow]
      Averaged survey magnetic field data during this SP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms4_des_fpib_dmpa_srvy_slow]
      Averaged survey magnetic field data during this SP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms4_des_pos_gse_slow]
      
      
      Position in GSM coordinates, 30 second [mms4_des_pos_gsm_slow]
      
      
      MMS4 number density integrands [mms4_des_numberdensity_int_slow]
      integrand terms used in normalized energy integration for number density
      
      number flux [mms4_des_numberflux_int_dbcs_slow]
      integrand terms used in normalized energy integration for number flux
      
      MMS4 pressure tensor integrands [mms4_des_prestensor_int_dbcs_slow]
      integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms4_des_ugrid_int_slow]
      
      
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MMS4_FPI_SLOW_L2_DIS-DIST
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode.  This product contains phase-space distribution maps of those
survey-resolution data from Slow Mode.  In particular, the (highest possible
quality at the time of release) corrected/converted "Slow Survey SkyMap"
distributions are reported with time-stamps and other annotation characterizing
the state of the instrument system at the indicated time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DIS vector of data-quality indicators at survey-start time [mms4_dis_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = compression pipeline error
      
      MMS4 FPI/DIS compression lossless/lossy indicator at survey-start time [mms4_dis_compressionloss_slow]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS4 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms4_dis_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS4 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms4_dis_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS4 FPI/DIS Slow Survey sky-map instrument distribution [mms4_dis_dist_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS Slow Survey sky-map instrument distribution 1-sigma error [mms4_dis_disterr_slow]
      Az bin: sector ind=00 looks "after" (spin-phase) Sun, ..., sector ind=15 looks
      "before" Sun dir.  Head field-of-view: pixel index=00 looks to zenith, ...,
      pixel index=15 looks to nadir.  FPI operations nominally bin data from 64 energy
      filters into 32 pairwise energy bins, indexed 0-31.  Nominally, bins are indexed
      in increasing energy order.  See FPI docs for details.
      
      MMS4 FPI/DIS slow survey average f1 count values [mms4_dis_avgf1counts_slow]
      Average f1-count level as a function of energy
      
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MMS4_FPI_SLOW_L2_DIS-MOMS
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DIS vector of data-quality indicators at survey-start time [mms4_dis_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only), Bit-13 =
      significant (>=20%) penetrating radiation, Bit-14 = high MMS3 spintone due to
      DIS008 anomaly
      
      MMS4 FPI/DIS compression lossless/lossy indicator at survey-start time [mms4_dis_compressionloss_slow]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS4 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms4_dis_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS4 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms4_dis_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS4 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms4_dis_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms4_dis_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms4_dis_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms4_dis_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms4_dis_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms4_dis_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS4 FPI/DIS omni-directional ion energy spectrum during this survey [mms4_dis_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS4 FPI/DIS ion background energy during this survey [mms4_dis_spectr_bg_slow]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS4 FPI/DIS ion background number density during this survey [mms4_dis_numberdensity_bg_slow]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS4 FPI/DIS ion number density during this survey [mms4_dis_numberdensity_slow]
      
      
      MMS4 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms4_dis_densityextrapolation_low_slow]
      
      
      MMS4 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms4_dis_densityextrapolation_high_slow]
      
      
      MMS4 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms4_dis_bulkv_dbcs_slow]
      
      
      MMS4 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms4_dis_bulkv_gse_slow]
      
      
      MMS4 FPI/DIS ion pressure tensor in DBCS during this survey [mms4_dis_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS ion pressure tensor in GSE during this survey [mms4_dis_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS ion background pressure during this survey [mms4_dis_pres_bg_slow]
      
      
      MMS4 FPI/DIS ion temperature tensor in DBCS during this survey [mms4_dis_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS ion temperature tensor in GSE during this survey [mms4_dis_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS ion heat-flux vector in DBCS during this survey [mms4_dis_heatq_dbcs_slow]
      
      
      MMS4 FPI/DIS ion heat-flux vector in GSE during this survey [mms4_dis_heatq_gse_slow]
      
      
      MMS4 FPI/DIS ion parallel temperature during this BP [mms4_dis_temppara_slow]
      
      
      MMS4 FPI/DIS ion perpendicular temperature during this BP [mms4_dis_tempperp_slow]
      
      
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MMS4_FPI_SLOW_L2_DIS-MOMSAUX
Description
FPI usually operates in Slow Survey Mode outside of the MMS Region Of Interest
(ROI) for the current Mission Phase.  Data captured from one of the four dual
spectrometers over three spacecraft spins are reported at about 60 s resolution
in this mode. This moments product contains results from integrating the
standard moments of phase-space distributions formed during Slow Mode. For
convenience, some additional parameters are included to augment those most
commonly found in a moments product of this sort, plus time-stamps and other
annotations characterizing the state of the instrument system at the indicated
time.
Modification History
See FPI Version Release Notes
(https://lasp.colorado.edu/mms/sdc/public/datasets/fpi/) for data set 
modification history.
 
  • Data Variable Descriptions
      MMS4 FPI/DIS vector of data-quality indicators at survey-start time [mms4_dis_errorflags_slow]
      Value of zero signifies no quality errors. For non-zero values: Bit-0 = manually
      flagged interval, Bit-1 = overcounting/saturation effects likely present in
      skymap, Bit-2 = reported spacecraft potential above 20V, Bit-3 =
      invalid/unavailable spacecraft potential, Bit-4 = significant (>10%) cold plasma
      (<10eV) component, Bit-5 = significant (>25%) hot plasma (>30keV) component,
      Bit-6 = high sonic Mach number (v/vth > 2.5), Bit-7 = low calculated density
      (n_DIS <= 0.0 cm^-3), Bit-8 = invalid/unavailable magnetic field data, Bit-10 =
      no internally generated photoelectron correction applied, Bit-11 = compression
      pipeline error, Bit-12 = spintone calculation error (DBCS only), Bit-13 =
      significant (>=20%) penetrating radiation, Bit-14 = high MMS3 spintone due to
      DIS008 anomaly
      
      MMS4 FPI/DIS partial ion number density during this survey [mms4_dis_numberdensity_part_slow]
      
      
      MMS4 FPI/DIS partial ion bulk-velocity vector in DBCS during this survey [mms4_dis_bulkv_part_dbcs_slow]
      
      
      MMS4 FPI/DIS partial ion bulk-velocity vector in GSE during this survey [mms4_dis_bulkv_part_gse_slow]
      
      
      MMS4 FPI/DIS partial ion pressure tensor in DBCS during this survey [mms4_dis_prestensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS partial ion pressure tensor in GSE during this survey [mms4_dis_prestensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS partial ion temperature tensor in DBCS during this survey [mms4_dis_temptensor_part_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS partial ion temperature tensor in GSE during this survey [mms4_dis_temptensor_part_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS partial ion parallel temperature during this survey [mms4_dis_temppara_part_slow]
      
      
      MMS4 FPI/DIS partial ion perpendicular temperature during this survey [mms4_dis_tempperp_part_slow]
      
      
      MMS4 FPI/DIS recommended energy index for partial moments during this survey [mms4_dis_part_index_slow]
      Recommended energy index during this survey
      
      MMS4 FPI/DIS compression lossless/lossy indicator at survey-start time [mms4_dis_compressionloss_slow]
      FPI/DIS compression loss indicator, 0=lossless, 1=lossy
      
      MMS4 FPI/DIS Del-Phi (obs spin-phase) count at survey-start time [mms4_dis_startdelphi_count_slow]
      Nominally, spin-phase counts range over [0000, 5759] cnts.  Each count
      represents 1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates
      obs +X-axis aligned with the sun-sensor axis.
      
      MMS4 FPI/DIS Del-Phi (obs spin-phase) angle at survey-start time [mms4_dis_startdelphi_angle_slow]
      Nominally, spin-phase angles range over [0, 360) deg.  Each count represents
      1/16 deg of observatory spin-phase.  Zero spin-phase angle indicates obs +X-axis
      aligned with the sun-sensor axis.
      
      MMS4 FPI/DIS ion energy spectrum "near" +X_DBCS during this survey [mms4_dis_energyspectr_px_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +x axis (instrument look angles: 45deg <= theta < 135deg and 135deg <=
      phi < 225deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" -X_DBCS during this survey [mms4_dis_energyspectr_mx_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -x axis (instrument look angles: 45deg <= theta < 135deg and phi >=
      315deg or phi < 45deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" +Y_DBCS during this survey [mms4_dis_energyspectr_py_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +y axis (instrument look angles: 45deg <= theta < 135deg and 225deg <=
      phi < 315deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" -Y_DBCS during this survey [mms4_dis_energyspectr_my_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -y axis (instrument look angles: 45deg <= theta < 135deg and 45deg <= phi
      < 135deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" +Z_DBCS during this survey [mms4_dis_energyspectr_pz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the +z axis (instrument look angles: 135deg <= theta < 180deg and 0deg <= phi
      < 360deg).
      
      MMS4 FPI/DIS ion energy spectrum "near" -Z_DBCS during this survey [mms4_dis_energyspectr_mz_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      particles whose DBCS flow direction is within 45 degrees (polar and azimuthal)
      of the -z axis (instrument look angles: 0deg <= theta < 45deg and 0deg <= phi <
      360deg).
      
      MMS4 FPI/DIS omni-directional ion energy spectrum during this survey [mms4_dis_energyspectr_omni_slow]
      Differential energy flux by energy bin, averaged (weighted by solid angle) over
      all directions (flow or look).
      
      MMS4 FPI/DIS ion background energy during this survey [mms4_dis_spectr_bg_slow]
      Background differential energy flux by energy bin, averaged (weighted by solid
      angle) over all directions (flow or look).
      
      MMS4 FPI/DIS ion background number density during this survey [mms4_dis_numberdensity_bg_slow]
      Background number density derived via integration of the estimated background
      differential energy flux.
      
      MMS4 FPI/DIS ion number density during this survey [mms4_dis_numberdensity_slow]
      
      
      MMS4 FPI/DIS estimated (via extrapolation to 0) contribution to density integral below 10eV [mms4_dis_densityextrapolation_low_slow]
      
      
      MMS4 FPI/DIS estimated (via extrapolation to infinity) contribution to density integral above 30keV [mms4_dis_densityextrapolation_high_slow]
      
      
      MMS4 FPI/DIS ion bulk-velocity vector in DBCS during this survey [mms4_dis_bulkv_dbcs_slow]
      
      
      MMS4 FPI/DIS ion bulk-velocity vector in GSE during this survey [mms4_dis_bulkv_gse_slow]
      
      
      MMS4 FPI/DIS ion pressure tensor in DBCS during this survey [mms4_dis_prestensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS ion pressure tensor in GSE during this survey [mms4_dis_prestensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Pxx Pxy Pxz, Row2) Pyx Pyy Pyz, Row3)
      Pzx Pzy Pzz. Note that Pij=Pji.
      
      MMS4 FPI/DIS ion background pressure during this survey [mms4_dis_pres_bg_slow]
      
      
      MMS4 FPI/DIS ion temperature tensor in DBCS during this survey [mms4_dis_temptensor_dbcs_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS ion temperature tensor in GSE during this survey [mms4_dis_temptensor_gse_slow]
      The 3x3 matrix is represented as: Row1) Txx Txy Txz, Row2) Tyx Tyy Tyz, Row3)
      Tzx Tzy Tzz. Note that Tij=Tji.
      
      MMS4 FPI/DIS ion heat-flux vector in DBCS during this survey [mms4_dis_heatq_dbcs_slow]
      
      
      MMS4 FPI/DIS ion heat-flux vector in GSE during this survey [mms4_dis_heatq_gse_slow]
      
      
      MMS4 FPI/DIS ion parallel temperature during this BP [mms4_dis_temppara_slow]
      
      
      MMS4 FPI/DIS ion perpendicular temperature during this BP [mms4_dis_tempperp_slow]
      
      
      MMS4 FPI/DIS S/C potential mean [mms4_dis_scpot_mean_slow]
      Average spacecraft potential during this SP used to shift the measure energies.
      
      MMS4 FPI/DIS S/C potential max [mms4_dis_scpot_max_slow]
      Maximum spacecraft potential during this SP used to exclude energies containing
      spacecraft photoelectron fluxes.
      
      Magnetic field vector X,Y,Z, and magnitude B [mms4_dis_fpib_gse_srvy_slow]
      Averaged survey magnetic field data during this SP
      
      Magnetic field vector X,Y,Z, and magnitude B [mms4_dis_fpib_dmpa_srvy_slow]
      Averaged survey magnetic field data during this SP. DMPA coordinates are within
      3 deg from DBCS coordinates and are used for pitch-angle determination. 
      
      Position in GSE coordinates, 30 second [mms4_dis_pos_gse_slow]
      
      
      Position in GSM coordinates, 30 second [mms4_dis_pos_gsm_slow]
      
      
      MMS4 number density integrands [mms4_dis_numberdensity_int_slow]
      integrand terms used in normalized energy integration for number density
      
      number flux [mms4_dis_numberflux_int_dbcs_slow]
      integrand terms used in normalized energy integration for number flux
      
      MMS4 pressure tensor integrands [mms4_dis_prestensor_int_dbcs_slow]
      integrand terms used in normalized energy integration for pressure tensor (L2
      bulk velocity taken into account)
      
      Normalized energies (E/(E+E0)) used in numerical integration of plasma moments [mms4_dis_ugrid_int_slow]
      
      
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MMS4_HPCA_BRST_L2_ION (spase://NASA/NumericalData/MMS/4/HotPlasmaCompositionAnalyzer/Burst/Level2/Ion/PT0.625S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Start Azimuth [mms4_hpca_start_azimuth]
      
      
      Science Mode Value as defined in the HPCA Science Algorithm Document [mms4_hpca_science_mode]
      
      
      H+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms4_hpca_hplus_data_quality]
      
      
      Hydrogen+ Flux for all Elevation Anodes across all energies [mms4_hpca_hplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_hplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_hplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_hplus_flux_byAnode_atE]
      
      
      Hydrogen+ Phase Space Density for all Elevation Anodes across all energies [mms4_hpca_hplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_hplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anodes [mms4_hpca_hplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_hplus_phase_space_density_byAnode_atE]
      
      
      He+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms4_hpca_heplus_data_quality]
      
      
      Helium+ Flux for all Elevation Anodes across all energies [mms4_hpca_heplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_heplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_heplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_heplus_flux_byAnode_atE]
      
      
      Helium+ Phase Space Density for all Elevation Anodes across all energies [mms4_hpca_heplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_heplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_heplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_heplus_phase_space_density_byAnode_atE]
      
      
      He++ per sweep status (0=bad): see Data_Quality_Key global attribute [mms4_hpca_heplusplus_data_quality]
      
      
      Helium++ Flux for all Elevation Anodes across all energies [mms4_hpca_heplusplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_heplusplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_heplusplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_heplusplus_flux_byAnode_atE]
      
      
      Helium++ Phase Space Density for all Elevation Anodes across all energies [mms4_hpca_heplusplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_heplusplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_heplusplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_heplusplus_phase_space_density_byAnode_atE]
      
      
      O+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms4_hpca_oplus_data_quality]
      
      
      Oxygen+ Flux for all Elevation Anodes across all energies [mms4_hpca_oplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_oplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_oplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_oplus_flux_byAnode_atE]
      
      
      Oxygen+ Phase Space Density for all Elevation Anodes across all energies [mms4_hpca_oplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_oplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_oplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_oplus_phase_space_density_byAnode_atE]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s), Despun MPA-aligned cartesian coordinates [mms4_hpca_B_GSE_sweep_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s), Geocentric Solar Magnetospheric (GSM) cartesian coordinates [mms4_hpca_B_GSM_sweep_avg]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms4_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms4_hpca_TOF_VMON_MIN_converted]
      
      
      Decimation Factor Index from mode config file [mms4_hpca_decimation_factor_index]
      
      
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MMS4_HPCA_BRST_L2_MOMENTS (spase://NASA/NumericalData/MMS/4/HotPlasmaCompositionAnalyzer/Burst/Level2/Moments/PT10S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Number Density Hydrogen+ for each HPCA half-spin [mms4_hpca_hplus_number_density]
      
      
      ---> Ion Bulk Velocity Hydrogen+ for each HPCA half-spin (x, y, z) [mms4_hpca_hplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Hydrogen+ for each HPCA half-spin [mms4_hpca_hplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_hplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_hplus_temperature_tensor]
      
      
      Number Density Helium+ for each HPCA half-spin [mms4_hpca_heplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium+ for each HPCA half-spin (x, y, z) [mms4_hpca_heplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium+ for each HPCA half-spin [mms4_hpca_heplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_heplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_heplus_temperature_tensor]
      
      
      Number Density Helium++ for each HPCA half-spin [mms4_hpca_heplusplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium++ for each HPCA half-spin (x, y, z) [mms4_hpca_heplusplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium++ for each HPCA half-spin [mms4_hpca_heplusplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_heplusplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_heplusplus_temperature_tensor]
      
      
      Number Density Oxygen+ for each HPCA half-spin [mms4_hpca_oplus_number_density]
      
      
      ---> Ion Bulk Velocity Oxygen+ for each HPCA half-spin (x, y, z) [mms4_hpca_oplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Oxygen+ for each HPCA half-spin [mms4_hpca_oplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_oplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_oplus_temperature_tensor]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms4_hpca_B_GSE_spin_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms4_hpca_B_GSM_spin_avg]
      
      
      Bulk Velocity in GSM for H+ for each HPCA half-spin (x, y, z) [mms4_hpca_hplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp H+ for each HPCA half-spin [mms4_hpca_hplus_tperp]
      
      
      ---> Tparallel H+ for each HPCA half-spin [mms4_hpca_hplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_hplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_hplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_hplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_hplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He+ for each HPCA half-spin (x, y, z) [mms4_hpca_heplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He+ for each HPCA half-spin [mms4_hpca_heplus_tperp]
      
      
      ---> Tparallel He+ for each HPCA half-spin [mms4_hpca_heplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He++ for each HPCA half-spin (x, y, z) [mms4_hpca_heplusplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He++ for each HPCA half-spin [mms4_hpca_heplusplus_tperp]
      
      
      ---> Tparallel He++ for each HPCA half-spin [mms4_hpca_heplusplus_tparallel]
      
      
      Vperp vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplusplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplusplus_vparallel]
      
      
      Vperp vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplusplus_vperp_GSM]
      
      
      Vparallel vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplusplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for O+ for each HPCA half-spin (x, y, z) [mms4_hpca_oplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp O+ for each HPCA half-spin [mms4_hpca_oplus_tperp]
      
      
      ---> Tparallel O+ for each HPCA half-spin [mms4_hpca_oplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_oplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_oplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_oplus_vperp_GSM]
      
      
      --->Vparallel vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_oplus_vparallel_GSM]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms4_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms4_hpca_TOF_VMON_MIN_converted]
      
      
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MMS4_HPCA_SRVY_L2_ION (spase://NASA/NumericalData/MMS/4/HotPlasmaCompositionAnalyzer/Survey/Level2/Ion/PT0.625S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Start Azimuth [mms4_hpca_start_azimuth]
      
      
      Science Mode Value as defined in the HPCA Science Algorithm Document [mms4_hpca_science_mode]
      
      
      H+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms4_hpca_hplus_data_quality]
      
      
      Hydrogen+ Flux for all Elevation Anodes across all energies [mms4_hpca_hplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_hplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_hplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_hplus_flux_byAnode_atE]
      
      
      Hydrogen+ Phase Space Density for all Elevation Anodes across all energies [mms4_hpca_hplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_hplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anodes [mms4_hpca_hplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_hplus_phase_space_density_byAnode_atE]
      
      
      He+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms4_hpca_heplus_data_quality]
      
      
      Helium+ Flux for all Elevation Anodes across all energies [mms4_hpca_heplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_heplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_heplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_heplus_flux_byAnode_atE]
      
      
      Helium+ Phase Space Density for all Elevation Anodes across all energies [mms4_hpca_heplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_heplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_heplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_heplus_phase_space_density_byAnode_atE]
      
      
      He++ per sweep status (0=bad): see Data_Quality_Key global attribute [mms4_hpca_heplusplus_data_quality]
      
      
      Helium++ Flux for all Elevation Anodes across all energies [mms4_hpca_heplusplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_heplusplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_heplusplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_heplusplus_flux_byAnode_atE]
      
      
      Helium++ Phase Space Density for all Elevation Anodes across all energies [mms4_hpca_heplusplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_heplusplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_heplusplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_heplusplus_phase_space_density_byAnode_atE]
      
      
      O+ per sweep status (0=bad): see Data_Quality_Key global attribute [mms4_hpca_oplus_data_quality]
      
      
      Oxygen+ Flux for all Elevation Anodes across all energies [mms4_hpca_oplus_flux]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_oplus_flux_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_oplus_flux_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_oplus_flux_byAnode_atE]
      
      
      Oxygen+ Phase Space Density for all Elevation Anodes across all energies [mms4_hpca_oplus_phase_space_density]
      
      
      ---> Movie display as function of energy and anode [mms4_hpca_oplus_phase_space_density_movie]
      
      
      ---> Spectrograms by energy at sample anode numbers [mms4_hpca_oplus_phase_space_density_byE_atAnode]
      
      
      ---> Spectrograms by anode number at sample energies [mms4_hpca_oplus_phase_space_density_byAnode_atE]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s), Despun MPA-aligned cartesian coordinates [mms4_hpca_B_GSE_sweep_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s), Geocentric Solar Magnetospheric (GSM) cartesian coordinates [mms4_hpca_B_GSM_sweep_avg]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms4_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms4_hpca_TOF_VMON_MIN_converted]
      
      
      Decimation Factor Index from mode config file [mms4_hpca_decimation_factor_index]
      
      
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MMS4_HPCA_SRVY_L2_MOMENTS (spase://NASA/NumericalData/MMS/4/HotPlasmaCompositionAnalyzer/Survey/Level2/Moments/PT10S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      Number Density Hydrogen+ for each HPCA half-spin [mms4_hpca_hplus_number_density]
      
      
      ---> Ion Bulk Velocity Hydrogen+ for each HPCA half-spin (x, y, z) [mms4_hpca_hplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Hydrogen+ for each HPCA half-spin [mms4_hpca_hplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_hplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Hydrogen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_hplus_temperature_tensor]
      
      
      Number Density Helium+ for each HPCA half-spin [mms4_hpca_heplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium+ for each HPCA half-spin (x, y, z) [mms4_hpca_heplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium+ for each HPCA half-spin [mms4_hpca_heplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_heplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_heplus_temperature_tensor]
      
      
      Number Density Helium++ for each HPCA half-spin [mms4_hpca_heplusplus_number_density]
      
      
      ---> Ion Bulk Velocity Helium++ for each HPCA half-spin (x, y, z) [mms4_hpca_heplusplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Helium++ for each HPCA half-spin [mms4_hpca_heplusplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_heplusplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Helium++ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_heplusplus_temperature_tensor]
      
      
      Number Density Oxygen+ for each HPCA half-spin [mms4_hpca_oplus_number_density]
      
      
      ---> Ion Bulk Velocity Oxygen+ for each HPCA half-spin (x, y, z) [mms4_hpca_oplus_ion_bulk_velocity]
      
      
      ---> Scalar Temperature Oxygen+ for each HPCA half-spin [mms4_hpca_oplus_scalar_temperature]
      
      
      ---> (no CDAWeb plots) Ion Pressure Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_oplus_ion_pressure]
      
      
      ---> (no CDAWeb plots) Ion Temp. Tensor Oxygen+ for each HPCA half-spin (xx,yx,zx,xy,yy,zy,xz,yz,zz) [mms4_hpca_oplus_temperature_tensor]
      
      
      Magnetic field vector in DMPA plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms4_hpca_B_GSE_spin_avg]
      
      
      ---> Magnetic field vector in GSM plus Btotal (8 or 16 S/s) for each HPCA half-spin (x, y, z, total) [mms4_hpca_B_GSM_spin_avg]
      
      
      Bulk Velocity in GSM for H+ for each HPCA half-spin (x, y, z) [mms4_hpca_hplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp H+ for each HPCA half-spin [mms4_hpca_hplus_tperp]
      
      
      ---> Tparallel H+ for each HPCA half-spin [mms4_hpca_hplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_hplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for H+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_hplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_hplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for H+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_hplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He+ for each HPCA half-spin (x, y, z) [mms4_hpca_heplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He+ for each HPCA half-spin [mms4_hpca_heplus_tperp]
      
      
      ---> Tparallel He+ for each HPCA half-spin [mms4_hpca_heplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplus_vperp_GSM]
      
      
      ---> Vparallel vector plus Magnitude in GSM for He+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for He++ for each HPCA half-spin (x, y, z) [mms4_hpca_heplusplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp He++ for each HPCA half-spin [mms4_hpca_heplusplus_tperp]
      
      
      ---> Tparallel He++ for each HPCA half-spin [mms4_hpca_heplusplus_tparallel]
      
      
      Vperp vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplusplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for He++ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplusplus_vparallel]
      
      
      Vperp vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplusplus_vperp_GSM]
      
      
      Vparallel vector plus Magnitude in GSM for He++ for each HPCA half-spin (x, y, z, total) [mms4_hpca_heplusplus_vparallel_GSM]
      
      
      Bulk Velocity in GSM for O+ for each HPCA half-spin (x, y, z) [mms4_hpca_oplus_ion_bulk_velocity_GSM]
      
      
      ---> Tperp O+ for each HPCA half-spin [mms4_hpca_oplus_tperp]
      
      
      ---> Tparallel O+ for each HPCA half-spin [mms4_hpca_oplus_tparallel]
      
      
      ---> Vperp vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_oplus_vperp]
      
      
      ---> Vparallel vector plus Magnitude for O+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_oplus_vparallel]
      
      
      ---> Vperp vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_oplus_vperp_GSM]
      
      
      --->Vparallel vector plus Magnitude in GSM for O+ for each HPCA half-spin (x, y, z, total) [mms4_hpca_oplus_vparallel_GSM]
      
      
      LIMITS - MCP_VMON_MIN_converted [mms4_hpca_MCP_VMON_MIN_converted]
      
      
      LIMITS - TOF_VMON_MIN_converted [mms4_hpca_TOF_VMON_MIN_converted]
      
      
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MMS4_HPCA_SRVY_L2_TOF-COUNTS (spase://NASA/NumericalData/MMS/4/HotPlasmaCompositionAnalyzer/Survey/Level2/TimeOfFlight/Counts/PT0.625S)
Description
References
Modification History
Initial Public Release
 
  • Data Variable Descriptions
      TOF Counts for all angles, across all energies [mms4_hpca_tof_counts]
      
      
      ---> Spectrograms all angles, at selected energies [mms4_hpca_tof_counts_allA_atE]
      
      
      ---> Spectrograms at select angles, for all energies [mms4_hpca_tof_counts_allE_atA]
      
      
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MMS4_MEC_BRST_L2_EPHT89D (spase://NASA/NumericalData/MMS/4/Ephemeris/Burst/Level2/Tsyganenko_89_Dynamic/PT0.030S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms4_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms4_mec_gmst]
      
      
      Magnetic Latitude. [mms4_mec_mlat]
      
      
      Magnetic Local Time. [mms4_mec_mlt]
      
      
      Dipole L-shell value. [mms4_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms4_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms4_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms4_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms4_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms4_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms4_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms4_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms4_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms4_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms4_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms4 (km) [mms4_mec_r_eci]
      
      
      Velocity of mms4 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms4_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms4 (km) [mms4_mec_r_gsm]
      
      
      Velocity of mms4 spacecraft in GSM coordinates (km/s) [mms4_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms4 (km) [mms4_mec_r_geo]
      
      
      Velocity of mms4 spacecraft in GEO coordinates (km/s) [mms4_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms4 (km) [mms4_mec_r_sm]
      
      
      Velocity of mms4 spacecraft in SM coordinates (km/s) [mms4_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms4 (km) [mms4_mec_r_gse]
      
      
      Velocity of mms4 spacecraft in GSE coordinates (km/s) [mms4_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms4 (km) [mms4_mec_r_gse2000]
      
      
      Velocity of mms4 spacecraft in GSE2000 coordinates (km/s) [mms4_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms4 spacecraft [mms4_mec_geod_lat]
      
      
      Geodetic longitude of mms4 spacecraft [mms4_mec_geod_lon]
      
      
      Geodetic height of mms4 spacecraft. (Height above WGS84 Spheroid.) [mms4_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms4_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms4_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms4_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms4 spacecraft [mms4_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms4_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms4_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms4 spacecraft [mms4_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms4 spacecraft [mms4_mec_bmin_gsm]
      
      
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MMS4_MEC_BRST_L2_EPHT89Q (spase://NASA/NumericalData/MMS/4/Ephemeris/Burst/Level2/Tsyganenko_89_Quiet/PT0.030S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms4_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms4_mec_gmst]
      
      
      Magnetic Latitude. [mms4_mec_mlat]
      
      
      Magnetic Local Time. [mms4_mec_mlt]
      
      
      Dipole L-shell value. [mms4_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms4_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms4_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms4_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms4_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms4_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms4_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms4_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms4_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms4_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms4_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms4 (km) [mms4_mec_r_eci]
      
      
      Velocity of mms4 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms4_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms4 (km) [mms4_mec_r_gsm]
      
      
      Velocity of mms4 spacecraft in GSM coordinates (km/s) [mms4_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms4 (km) [mms4_mec_r_geo]
      
      
      Velocity of mms4 spacecraft in GEO coordinates (km/s) [mms4_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms4 (km) [mms4_mec_r_sm]
      
      
      Velocity of mms4 spacecraft in SM coordinates (km/s) [mms4_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms4 (km) [mms4_mec_r_gse]
      
      
      Velocity of mms4 spacecraft in GSE coordinates (km/s) [mms4_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms4 (km) [mms4_mec_r_gse2000]
      
      
      Velocity of mms4 spacecraft in GSE2000 coordinates (km/s) [mms4_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms4 spacecraft [mms4_mec_geod_lat]
      
      
      Geodetic longitude of mms4 spacecraft [mms4_mec_geod_lon]
      
      
      Geodetic height of mms4 spacecraft. (Height above WGS84 Spheroid.) [mms4_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms4_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms4_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms4_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms4 spacecraft [mms4_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms4_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms4_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms4 spacecraft [mms4_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms4 spacecraft [mms4_mec_bmin_gsm]
      
      
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MMS4_MEC_BRST_L2_EPHTS04D (spase://NASA/NumericalData/MMS/4/Ephemeris/Burst/Level2/Tsyganenko_04_Dynamic/PT0.030S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms4_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms4_mec_gmst]
      
      
      Magnetic Latitude. [mms4_mec_mlat]
      
      
      Magnetic Local Time. [mms4_mec_mlt]
      
      
      Dipole L-shell value. [mms4_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms4_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms4_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms4_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms4_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms4_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms4_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms4_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms4_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms4_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms4_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms4 (km) [mms4_mec_r_eci]
      
      
      Velocity of mms4 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms4_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms4 (km) [mms4_mec_r_gsm]
      
      
      Velocity of mms4 spacecraft in GSM coordinates (km/s) [mms4_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms4 (km) [mms4_mec_r_geo]
      
      
      Velocity of mms4 spacecraft in GEO coordinates (km/s) [mms4_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms4 (km) [mms4_mec_r_sm]
      
      
      Velocity of mms4 spacecraft in SM coordinates (km/s) [mms4_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms4 (km) [mms4_mec_r_gse]
      
      
      Velocity of mms4 spacecraft in GSE coordinates (km/s) [mms4_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms4 (km) [mms4_mec_r_gse2000]
      
      
      Velocity of mms4 spacecraft in GSE2000 coordinates (km/s) [mms4_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms4 spacecraft [mms4_mec_geod_lat]
      
      
      Geodetic longitude of mms4 spacecraft [mms4_mec_geod_lon]
      
      
      Geodetic height of mms4 spacecraft. (Height above WGS84 Spheroid.) [mms4_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms4_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms4_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms4_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms4 spacecraft [mms4_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms4_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms4_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms4 spacecraft [mms4_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms4 spacecraft [mms4_mec_bmin_gsm]
      
      
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MMS4_MEC_SRVY_L2_EPHT89D (spase://NASA/NumericalData/MMS/4/Ephemeris/Survey/Level2/Tsyganenko_89_Dynamic/PT30S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms4_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms4_mec_gmst]
      
      
      Magnetic Latitude. [mms4_mec_mlat]
      
      
      Magnetic Local Time. [mms4_mec_mlt]
      
      
      Dipole L-shell value. [mms4_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms4_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms4_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms4_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms4_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms4_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms4_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms4_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms4_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms4_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms4_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms4 (km) [mms4_mec_r_eci]
      
      
      Velocity of mms4 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms4_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms4 (km) [mms4_mec_r_gsm]
      
      
      Velocity of mms4 spacecraft in GSM coordinates (km/s) [mms4_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms4 (km) [mms4_mec_r_geo]
      
      
      Velocity of mms4 spacecraft in GEO coordinates (km/s) [mms4_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms4 (km) [mms4_mec_r_sm]
      
      
      Velocity of mms4 spacecraft in SM coordinates (km/s) [mms4_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms4 (km) [mms4_mec_r_gse]
      
      
      Velocity of mms4 spacecraft in GSE coordinates (km/s) [mms4_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms4 (km) [mms4_mec_r_gse2000]
      
      
      Velocity of mms4 spacecraft in GSE2000 coordinates (km/s) [mms4_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms4 spacecraft [mms4_mec_geod_lat]
      
      
      Geodetic longitude of mms4 spacecraft [mms4_mec_geod_lon]
      
      
      Geodetic height of mms4 spacecraft. (Height above WGS84 Spheroid.) [mms4_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms4_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms4_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms4_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms4 spacecraft [mms4_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms4_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms4_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms4 spacecraft [mms4_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms4 spacecraft [mms4_mec_bmin_gsm]
      
      
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MMS4_MEC_SRVY_L2_EPHT89Q (spase://NASA/NumericalData/MMS/4/Ephemeris/Survey/Level2/Tsyganenko_89_Quiet/PT30S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms4_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms4_mec_gmst]
      
      
      Magnetic Latitude. [mms4_mec_mlat]
      
      
      Magnetic Local Time. [mms4_mec_mlt]
      
      
      Dipole L-shell value. [mms4_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms4_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms4_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms4_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms4_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms4_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms4_mec_P_phase]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms4_mec_ang_mom_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms4_mec_ang_mom_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms4_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms4_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms4_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms4_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms4 (km) [mms4_mec_r_eci]
      
      
      Velocity of mms4 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms4_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms4 (km) [mms4_mec_r_gsm]
      
      
      Velocity of mms4 spacecraft in GSM coordinates (km/s) [mms4_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms4 (km) [mms4_mec_r_geo]
      
      
      Velocity of mms4 spacecraft in GEO coordinates (km/s) [mms4_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms4 (km) [mms4_mec_r_sm]
      
      
      Velocity of mms4 spacecraft in SM coordinates (km/s) [mms4_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms4 (km) [mms4_mec_r_gse]
      
      
      Velocity of mms4 spacecraft in GSE coordinates (km/s) [mms4_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms4 (km) [mms4_mec_r_gse2000]
      
      
      Velocity of mms4 spacecraft in GSE2000 coordinates (km/s) [mms4_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms4 spacecraft [mms4_mec_geod_lat]
      
      
      Geodetic longitude of mms4 spacecraft [mms4_mec_geod_lon]
      
      
      Geodetic height of mms4 spacecraft. (Height above WGS84 Spheroid.) [mms4_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms4_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms4_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms4_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms4 spacecraft [mms4_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms4_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms4_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms4 spacecraft [mms4_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms4 spacecraft [mms4_mec_bmin_gsm]
      
      
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MMS4_MEC_SRVY_L2_EPHTS04D (spase://NASA/NumericalData/MMS/4/Ephemeris/Survey/Level2/Tsyganenko_04_Dynamic/PT30S)
Description
MMS MEC Magnetic ephemeris and coordinates, Level 2 science data. PI institution
is Los Alamos National Laboratory (LANL)
 
  • Data Variable Descriptions
      Dipole tilt angle. Rotation angle (around Y-axis) between GSM and SM coordinate systems. In units of degrees. [mms4_mec_dipole_tilt]
      
      
      Greenwich Mean Sidereal Time (GMST). [mms4_mec_gmst]
      
      
      Magnetic Latitude. [mms4_mec_mlat]
      
      
      Magnetic Local Time. [mms4_mec_mlt]
      
      
      Dipole L-shell value. [mms4_mec_l_dipole]
      
      
      Quaternion rotation from GEI/J2000 to BCS (ECI to BCS). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_bcs]
      
      
      Quaternion rotation from GEI/J2000 to DBCS (ECI to DBCS). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dbcs]
      
      
      Quaternion rotation from GEI/J2000 to DMPA (ECI to DMPA). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dmpa]
      
      
      Quaternion rotation from GEI/J2000 to SMPA (ECI to SMPA). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_smpa]
      
      
      Quaternion rotation from GEI/J2000 to DSL (ECI to DSL). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_dsl]
      
      
      Quaternion rotation from GEI/J2000 to SSL (ECI to SSL). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_ssl]
      
      
      Right ascension (deg) and declination (deg) of angular momentum (L) [mms4_mec_L_vec]
      
      
      Right ascension (deg) and declination (deg) of Body Z-axis [mms4_mec_Z_vec]
      
      
      Right ascension (deg) and declination (deg) of Major Principal Axis [mms4_mec_P_vec]
      
      
      L-phase (Sun-to-body-X dihedral angle about angular momentum vector L) (deg) [mms4_mec_L_phase]
      
      
      Z-phase (Sun-to-body-X dihedral angle about the body-Z vector) (deg) [mms4_mec_Z_phase]
      
      
      P-phase (Sun-to-body-X dihedral angle about the major principal axis, P) (deg) [mms4_mec_P_phase]
      
      
      Kp index from QinDenton files (used as input to magnetic field models) [mms4_mec_kp]
      
      
      Dst index from QinDenton files. Used as input to magnetic field models [mms4_mec_dst]
      
      
      Earth eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms4_mec_earth_eclipse_flag]
      
      
      Moon eclipse flag: 0 = no eclipse; 1 = penumbral eclipse; 2 = umbral eclipse. [mms4_mec_moon_eclipse_flag]
      
      
      Geocentric Equatorial Inertial (GEI/J2000) position vector of mms4 (km) [mms4_mec_r_eci]
      
      
      Velocity of mms4 spacecraft in GEI/J2000 (i.e. ECI) coordinates (km/s) [mms4_mec_v_eci]
      
      
      Geocentric Solar Magnetospheric (GSM) position vector of mms4 (km) [mms4_mec_r_gsm]
      
      
      Velocity of mms4 spacecraft in GSM coordinates (km/s) [mms4_mec_v_gsm]
      
      
      Quaternion rotation from GEI/J2000 to GSM (ECI to GSM). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gsm]
      
      
      Geocentric Geographic (GEO) position vector of mms4 (km) [mms4_mec_r_geo]
      
      
      Velocity of mms4 spacecraft in GEO coordinates (km/s) [mms4_mec_v_geo]
      
      
      Quaternion rotation from GEI/J2000 to GEO (ECI to GEO). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_geo]
      
      
      Geocentric Solar Magnetic (SM) position vector of mms4 (km) [mms4_mec_r_sm]
      
      
      Velocity of mms4 spacecraft in SM coordinates (km/s) [mms4_mec_v_sm]
      
      
      Quaternion rotation from GEI/J2000 to SM (ECI to SM). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_sm]
      
      
      Geocentric Solar Ecliptic (GSE) position vector of mms4 (km) [mms4_mec_r_gse]
      
      
      Velocity of mms4 spacecraft in GSE coordinates (km/s) [mms4_mec_v_gse]
      
      
      Quaternion rotation from GEI/J2000 to GSE (ECI to GSE). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gse]
      
      
      Geocentric Solar Ecliptic (J2000 Pole, GSE2000) position vector of mms4 (km) [mms4_mec_r_gse2000]
      
      
      Velocity of mms4 spacecraft in GSE2000 coordinates (km/s) [mms4_mec_v_gse2000]
      
      
      Quaternion rotation from GEI/J2000 to GSE2000 (ECI to GSE2000). ((qx,qy,qz), qw) [mms4_mec_quat_eci_to_gse2000]
      
      
      Geodetic latitude of mms4 spacecraft [mms4_mec_geod_lat]
      
      
      Geodetic longitude of mms4 spacecraft [mms4_mec_geod_lon]
      
      
      Geodetic height of mms4 spacecraft. (Height above WGS84 Spheroid.) [mms4_mec_geod_height]
      
      
      Geocentric position vector (in km) of the Sun in GEI/J2000 Coordinates. [mms4_mec_r_sun_de421_eci]
      
      
      Geocentric position vector (in km) of the Moon in GEI/J2000 Coordinates. [mms4_mec_r_moon_de421_eci]
      
      
      Fieldline Type: 0 = IMF; 1 = Closed; 2 = Open Northern Lobe; 3 = Open Southern Lobe; -1 = Inside Earth; -2 = Target Height Unreachable; -3 = Bad Trace (error). [mms4_mec_fieldline_type]
      
      
      Magnetic field (in GSM) at mms4 spacecraft [mms4_mec_bsc_gsm]
      
      
      Southern loss cone angle. Degrees. [mms4_mec_loss_cone_angle_s]
      
      
      Northern loss cone angle. Degrees. [mms4_mec_loss_cone_angle_n]
      
      
      Geodetic latitude and longitude of southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfs_geod_latlon]
      
      
      Geodetic latitude and longitude of northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfn_geod_latlon]
      
      
      GSM position southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfs_gsm]
      
      
      Magnetic field (in GSM) at southern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_bfs_gsm]
      
      
      GSM position northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_pfn_gsm]
      
      
      Magnetic field (in GSM) at northern footpoint (100km geodetic height) of field threading the mms4 spacecraft [mms4_mec_bfn_gsm]
      
      
      GSM position of min-B point of field threading the mms4 spacecraft [mms4_mec_pmin_gsm]
      
      
      Magnetic field (in GSM) at min-B point of field threading the mms4 spacecraft [mms4_mec_bmin_gsm]
      
      
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MMS4_R0_SUMMARY
Description
Pre-generated MMS Quicklook Summary Plots
File location: https://cdaweb.gsfc.nasa.gov/pub/data/mms/ql_plots/all_mms4_summ 
 
  • Data Variable Descriptions
Dataset in CDAWeb
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MMS4_SCM_BRST_L2_SCB (spase://NASA/NumericalData/MMS/4/FIELDS/SCM/Burst/Level2/PT0.0001220703125S)
Description
The tri-axial search-coil magnetometer (SCM) with its associated preamplifier
provides the three-dimensional measurement of the magnetic field fluctuations.
The analog magnetic waveforms measured by the SCM are digitized and processed
inside the digital signal processor (DSP), collected and stored by the central
instrument data processor (CIDP) via the Fields central electronics box (CEB).
Prior to launch, all SCM Flight models were calibrated by LPP at the National
Magnetic Observatory at Chambon-la-Foret (Orleans). Once per orbit, each SCM
transfer function is checked thanks to the onboard calibration signal provided
by DSP. SCM is operated for the entire MMS orbit in survey mode. Within the ROI,
burst mode data are also acquired as well as high burst mode data. 
SCM data set corresponds to the AC magnetic field waveforms in nanoTesla and in
the GSE frame.
The instrument paper for SCM can be found at
https://urldefense.proofpoint.com/v2/url?u=http-3A__link.springer.com_article_10
.1007_s11214-2D014-2D0096-2D9&d=DwIFAg&c=c6MrceVCY5m5A_KAUkrdoA&r=bjziExGTRYoZgE
2xb_dDSm9NxNIo0lG6Q-rB0Y6rHS4&m=CMzo0Vv9zPtWSdbdY1Wq9-jIkYS2cOMV9JYZsMV10y0&s=Xb
P9PiEAswHGl5lqgsDVI6zs8ivJx7yek9i2undKl10&e= 
Modification History
unpack telemetry, assign sample times
2026-07-10T20:12:44.00005370378175Z - [L1A->L1B (step 1/1)] Calibration
(TMcounts->nT). See CALIBRATION_PARAMETERS for details.
2026-07-16T12:40:49.00003373622908Z - [L1B->L2 (step 1/2)] Coordinate transform
(SCM123->GSE). See COORD_TRANS_PARAMETERS for details.
2026-07-16T12:40:57.0000305771829Z - [L1B->L2 (step 2/2)] Frequency filtering.
See FREQUENCY_FILTER for details.
 
  • Data Variable Descriptions
      L2 AC magnetic field in GSE frame [mms4_scm_acb_gse_scb_brst_l2]
      These calibrated (nT) AC magnetic field waveform data are sampled at 8192S/s.
      They are high-pass filtered above 1.00Hz but not low-pass filtered. See global
      attributes for details. For more information, please have a look at the SCM Data
      Products Guide.
      
      (List/Create Only) Quality Factor (one letter per antenna, G=good) [mms4_scm_qf_scm123_scb_brst_l2]
      Each letter refers to one SCM physical antenna in the SCM123 order. 'G' stands
      for good data, 'Z' for data that are affected or set to zero by convolution
      boundary effect, 'S' for saturated data, 'X' for out of range data, 'B' for
      fillvalue/bad data.
      
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MMS4_SCM_BRST_L2_SCHB (spase://NASA/NumericalData/MMS/4/FIELDS/SCM/Burst/Level2/PT0.00006101515625S)
Description
The tri-axial search-coil magnetometer (SCM) with its associated preamplifier
provides the three-dimensional measurement of the magnetic field fluctuations.
The analog magnetic waveforms measured by the SCM are digitized and processed
inside the digital signal processor (DSP), collected and stored by the central
instrument data processor (CIDP) via the Fields central electronics box (CEB).
Prior to launch, all SCM Flight models were calibrated by LPP at the National
Magnetic Observatory at Chambon-la-Foret (Orleans). Once per orbit, each SCM
transfer function is checked thanks to the onboard calibration signal provided
by DSP. SCM is operated for the entire MMS orbit in survey mode. Within the ROI,
burst mode data are also acquired as well as high burst mode data. 
SCM data set corresponds to the AC magnetic field waveforms in nanoTesla and in
the GSE frame.
The instrument paper for SCM can be found at
http://link.springer.com/article/10.1007/s11214-014-0096-9
Modification History
unpack telemetry, assign sample times
2026-07-10T20:13:12.00006276368782Z - [L1A->L1B (step 1/1)] Calibration
(TMcounts->nT). See CALIBRATION_PARAMETERS for details.
2026-07-16T12:41:30.00005275011067Z - [L1B->L2 (step 1/2)] Coordinate transform
(SCM123->GSE). See COORD_TRANS_PARAMETERS for details.
2026-07-16T12:41:34.00003105401998Z - [L1B->L2 (step 2/2)] Frequency filtering.
See FREQUENCY_FILTER for details.
 
  • Data Variable Descriptions
      L2 AC magnetic field in GSE frame [mms4_scm_acb_gse_schb_brst_l2]
      These calibrated (nT) AC magnetic field waveform data are sampled at 16384S/s.
      They are high-pass filtered above 32.00Hz but not low-pass filtered. See global
      attributes for details. For more information, please have a look at the SCM Data
      Products Guide
      (https://lasp.colorado.edu/mms/sdc/public/datasets/fields/Science_Data_Products_ 
      Guide_vol2_SCM_v11_20160301.pdf).
      
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MMS4_SCM_SRVY_L2_SCSRVY (spase://NASA/NumericalData/MMS/4/FIELDS/SCM/Survey/Level2/PT0.03125S)
Description
The tri-axial search-coil magnetometer (SCM) with its associated preamplifier
provides the three-dimensional measurement of the magnetic field fluctuations.
The analog magnetic waveforms measured by the SCM are digitized and processed
inside the digital signal processor (DSP), collected and stored by the central
instrument data processor (CIDP) via the Fields central electronics box (CEB).
Prior to launch, all SCM Flight models were calibrated by LPP at the National
Magnetic Observatory at Chambon-la-Foret (Orleans). Once per orbit, each SCM
transfer function is checked thanks to the onboard calibration signal provided
by DSP. SCM is operated for the entire MMS orbit in survey mode. Within the ROI,
burst mode data are also acquired as well as high burst mode data. 
SCM data set corresponds to the AC magnetic field waveforms in nanoTesla and in
the GSE frame.
The instrument paper for SCM can be found at
http://link.springer.com/article/10.1007/s11214-014-0096-9
Modification History
unpack telemetry, assign sample times
2026-07-03T00:00:34.00005698204041Z - [L1A->L1B (step 1/1)] Calibration
(TMcounts->nT). See CALIBRATION_PARAMETERS for details.
2026-07-15T23:57:22.00005233287508Z - [L1B->L2 (step 1/2)] Coordinate transform
(SCM123->GSE). See COORD_TRANS_PARAMETERS for details.
2026-07-15T23:58:05.00006049871102Z - [L1B->L2 (step 2/2)] Frequency filtering.
See FREQUENCY_FILTER for details.
 
  • Data Variable Descriptions
      L2 AC magnetic field in GSE frame [mms4_scm_acb_gse_scsrvy_srvy_l2]
      These calibrated (nT) AC magnetic field waveform data are sampled at 32S/s. They
      are high-pass filtered above 0.50Hz but not low-pass filtered. See global
      attributes for details. For more information, please have a look at the SCM Data
      Products Guide
      (https://lasp.colorado.edu/mms/sdc/public/datasets/fields/Science_Data_Products_ 
      Guide_vol2_SCM_v11_20160301.pdf).
      
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MOON_HELIO1HR_POSITION
Description
No TEXT global attribute value.
 
  • Data Variable Descriptions
      Distance from Sun to object [RAD_AU]
      
      
      Latitude in Solar Ecliptic Coordinate System (SE) [SE_LAT]
      
      
      Longitude in Solar Ecliptic Coordinate System (SE) [SE_LON]
      
      
      Latitude in heliographic Rotating Coordinate System (HG) [HG_LAT]
      
      
      Longitude in Heliographic Rotating Coordinate System (HG) [HG_LON]
      
      
      Latitude in heliographic Inertial Coordinate System (HGI) [HGI_LAT]
      
      
      Longitude in heliographic Inertial Coordinate System (HGI) [HGI_LON]
      
      
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MSL_RAD_OBS-L1
Description
The Radiation Assessment Detector (RAD) and its data products are described in
detail in the literature (Hassler et al., 2012). Each RAD observation contains
the following: (1) Instrument counters, (2) Neutral particle count histograms in
detectors D and E, (3) LET count histograms, (4) Absorbed dose rate in detectors
B and E, (5) High-cadence dose rate in B and E (16 rates per observation).
 
  • Data Variable Descriptions
      Actual instrument observation time [ALIVE_TIME]
      
      
      Amount of time hardware could not accept a new trigger [DEAD_TIME]
      
      
      Total duration of the observation including dead and alive time [DURATION]
      
      
      Temperature at beginning of observation [START_TEMPERATURE]
      
      
      RAD Flight Software checksum [FSW_XSUM]
      
      
      EVIL Table checksum [EVIL_XSUM]
      
      
      Setup Table checksum [SETUP_XSUM]
      
      
      Temperature adjustment table checksum [TEMP_XSUM]
      
      
      Observation id in database as primary key [OBS_ID]
      
      
      Spacecraft Clock at beginning of observation [BEGIN_SCLK]
      
      
      Spacecraft Clock at end of observation [END_SCLK]
      
      
      UTC time at start of observation [BEGIN_UTC]
      
      
      UTC time at end of observation [END_UTC]
      
      
      Mars local time at start of observation [BEGIN_MARS]
      
      
      Mars local time at end of observation [END_MARS]
      
      
      Martian Sol [SOL]
      
      
      Precise Sol at start of observation [BEGIN_SOL]
      
      
      Precise Sol at end of observation [END_SOL]
      
      
      Rover Latitude [ROVER_LAT]
      
      
      Rover Longitude [ROVER_LONG]
      
      
      Rover Elevation [ROVER_ELEVATION]
      
      
      Rover Azmith Where to get this?? [ROVER_AZMITH]
      
      
      Rover Zenith angle [ROVER_ZENITH]
      
      
      Rover Tilt Angle [ROVER_TILT]
      
      
      Solar Zenith [SOLAR_ZENITH]
      
      
      Solar Longitude [SOLAR_LONG]
      
      
      Did RAD detect a solar event during intialization? [SOLAR_MODE]
      
      
      True if DAN was enabled during RAD observation [DAN_POWERED]
      
      
      How many fast triggers hardware detected [FAST_TRIG_COUNT]
      
      
      [Quality filtered] LET in A1 silicon detector [LET_A1_f]
      
      
      [All quality] LET in A1 silicon detector [LET_A1]
      
      
      [Quality filtered] LET in A2 silicon detector [LET_A2_f]
      
      
      [All quality] LET in A2 silicon detector [LET_A2]
      
      
      Triggers for Fast channel 0 (F2H) [CHANNEL_COUNTERS_FAST_02]
      
      
      Triggers for Slow channel 0 (F2H) [CHANNEL_COUNTERS_SLOW_02]
      
      
      Triggers for Fast channel 1 (EL) [CHANNEL_COUNTERS_FAST_03]
      
      
      Triggers for Slow channel 1 (EL) [CHANNEL_COUNTERS_SLOW_03]
      
      
      Triggers for Fast channel 2 (EN) [CHANNEL_COUNTERS_FAST_04]
      
      
      Triggers for Slow channel 2 (EN) [CHANNEL_COUNTERS_SLOW_04]
      
      
      Triggers for Fast channel 3 (EM) [CHANNEL_COUNTERS_FAST_05]
      
      
      Triggers for Slow channel 3 (EM) [CHANNEL_COUNTERS_SLOW_05]
      
      
      Triggers for Fast channel 4 (EI) [CHANNEL_COUNTERS_FAST_06]
      
      
      Triggers for Slow channel 4 (EI) [CHANNEL_COUNTERS_SLOW_06]
      
      
      Triggers for Fast channel 5 (EH) [CHANNEL_COUNTERS_FAST_07]
      
      
      Triggers for Slow channel 5 (EH) [CHANNEL_COUNTERS_SLOW_07]
      
      
      Triggers for Fast channel 6 (EU) [CHANNEL_COUNTERS_FAST_08]
      
      
      Triggers for Slow channel 6 (EU) [CHANNEL_COUNTERS_SLOW_08]
      
      
      Triggers for Fast channel 7 (DL) [CHANNEL_COUNTERS_FAST_09]
      
      
      Triggers for Slow channel 7 (DL) [CHANNEL_COUNTERS_SLOW_09]
      
      
      Triggers for Fast channel 8 (DN) [CHANNEL_COUNTERS_FAST_10]
      
      
      Triggers for Slow channel 8 (DN) [CHANNEL_COUNTERS_SLOW_10]
      
      
      Triggers for Fast channel 9 (DM) [CHANNEL_COUNTERS_FAST_11]
      
      
      Triggers for Slow channel 9 (DM) [CHANNEL_COUNTERS_SLOW_11]
      
      
      Triggers for Fast channel 10 (DI) [CHANNEL_COUNTERS_FAST_12]
      
      
      Triggers for Slow channel 10 (DI) [CHANNEL_COUNTERS_SLOW_12]
      
      
      Triggers for Fast channel 11 (DH) [CHANNEL_COUNTERS_FAST_13]
      
      
      Triggers for Slow channel 11 (DH) [CHANNEL_COUNTERS_SLOW_13]
      
      
      Triggers for Fast channel 12 (DU) [CHANNEL_COUNTERS_FAST_14]
      
      
      Triggers for Slow channel 12 (DU) [CHANNEL_COUNTERS_SLOW_14]
      
      
      Triggers for Fast channel 13 (CL) [CHANNEL_COUNTERS_FAST_15]
      
      
      Triggers for Slow channel 13 (CL) [CHANNEL_COUNTERS_SLOW_15]
      
      
      Triggers for Fast channel 14 (CM) [CHANNEL_COUNTERS_FAST_16]
      
      
      Triggers for Slow channel 14 (CM) [CHANNEL_COUNTERS_SLOW_16]
      
      
      Triggers for Fast channel 15 (CH) [CHANNEL_COUNTERS_FAST_17]
      
      
      Triggers for Slow channel 15 (CH) [CHANNEL_COUNTERS_SLOW_17]
      
      
      Triggers for Fast channel 16 (CU) [CHANNEL_COUNTERS_FAST_18]
      
      
      Triggers for Slow channel 16 (CU) [CHANNEL_COUNTERS_SLOW_18]
      
      
      Triggers for Fast channel 17 (C2L) [CHANNEL_COUNTERS_FAST_19]
      
      
      Triggers for Slow channel 17 (C2L) [CHANNEL_COUNTERS_SLOW_19]
      
      
      Triggers for Fast channel 18 (C2H) [CHANNEL_COUNTERS_FAST_20]
      
      
      Triggers for Slow channel 18 (C2H) [CHANNEL_COUNTERS_SLOW_20]
      
      
      Triggers for Fast channel 19 (BL) [CHANNEL_COUNTERS_FAST_21]
      
      
      Triggers for Slow channel 19 (BL) [CHANNEL_COUNTERS_SLOW_21]
      
      
      Triggers for Fast channel 20 (BM) [CHANNEL_COUNTERS_FAST_22]
      
      
      Triggers for Slow channel 20 (BM) [CHANNEL_COUNTERS_SLOW_22]
      
      
      Triggers for Fast channel 21 (BH) [CHANNEL_COUNTERS_FAST_23]
      
      
      Triggers for Slow channel 21 (BH) [CHANNEL_COUNTERS_SLOW_23]
      
      
      Triggers for Fast channel 22 (BU) [CHANNEL_COUNTERS_FAST_24]
      
      
      Triggers for Slow channel 22 (BU) [CHANNEL_COUNTERS_SLOW_24]
      
      
      Triggers for Fast channel 23 (A2L) [CHANNEL_COUNTERS_FAST_25]
      
      
      Triggers for Slow channel 23 (A2L) [CHANNEL_COUNTERS_SLOW_25]
      
      
      Triggers for Fast channel 24 (A2M) [CHANNEL_COUNTERS_FAST_26]
      
      
      Triggers for Slow channel 24 (A2M) [CHANNEL_COUNTERS_SLOW_26]
      
      
      Triggers for Fast channel 25 (A2H) [CHANNEL_COUNTERS_FAST_27]
      
      
      Triggers for Slow channel 25 (A2H) [CHANNEL_COUNTERS_SLOW_27]
      
      
      Triggers for Fast channel 26 (A2U) [CHANNEL_COUNTERS_FAST_28]
      
      
      Triggers for Slow channel 26 (A2U) [CHANNEL_COUNTERS_SLOW_28]
      
      
      Triggers for Fast channel 27 (A1L) [CHANNEL_COUNTERS_FAST_29]
      
      
      Triggers for Slow channel 27 (A1L) [CHANNEL_COUNTERS_SLOW_29]
      
      
      Triggers for Fast channel 28 (A1M) [CHANNEL_COUNTERS_FAST_30]
      
      
      Triggers for Slow channel 28 (A1M) [CHANNEL_COUNTERS_SLOW_30]
      
      
      Triggers for Fast channel 29 (A1H) [CHANNEL_COUNTERS_FAST_31]
      
      
      Triggers for Slow channel 29 (A1H) [CHANNEL_COUNTERS_SLOW_31]
      
      
      Triggers for Fast channel 30 (A1U) [CHANNEL_COUNTERS_FAST_32]
      
      
      Triggers for Slow channel 30 (A1U) [CHANNEL_COUNTERS_SLOW_32]
      
      
      Triggers for Fast channel 31 (F1L) [CHANNEL_COUNTERS_FAST_33]
      
      
      Triggers for Slow channel 31 (F1L) [CHANNEL_COUNTERS_SLOW_33]
      
      
      Particle events that matched for index 0 [A1U and BU and not C2L] [MATCH_COUNTER_0]
      
      
      Particle events that matched for index 1 [A2U and BU and not C2L] [MATCH_COUNTER_1]
      
      
      Particle events that matched for index 2 [A1M and BM] [MATCH_COUNTER_2]
      
      
      Particle events that matched for index 3 [A2M and BM] [MATCH_COUNTER_3]
      
      
      Particle events that matched for index 4 [BU] [MATCH_COUNTER_4]
      
      
      Particle events that matched for index 5 [EH and EI] [MATCH_COUNTER_5]
      
      
      Particle events that matched for index 6 [not F1L and not BU and not C2H and not C2L and not CU and EH and EI and EM] [MATCH_COUNTER_6]
      
      
      Particle events that matched for index 7 [not F1L and not BU and not C2H and not C2L and not CU and DH and DI] [MATCH_COUNTER_7]
      
      
      Particle events that matched for index 8 [not F1L and not BU and not C2H and not C2L and not CU and DH and DI and EH and EI] [MATCH_COUNTER_8]
      
      
      Particle events that matched for index 9 [DM and DL] [MATCH_COUNTER_9]
      
      
      Particle events that matched for index 10 [not F1L and not A1U and not A2U and BU and not BH and not C2H and not C2L and not CU and not DH and not EH] [MATCH_COUNTER_10]
      
      
      Particle events that matched for index 11 [A2U and BU and CU and DH and EH] [MATCH_COUNTER_11]
      
      
      Particle events that matched for index 12 [not A1U and not A2U and not BU and not CU and DH and EH] [MATCH_COUNTER_12]
      
      
      Particle events that matched for index 13 [A2U and BU and CU and DH and not EH] [MATCH_COUNTER_13]
      
      
      Particle events that matched for index 14 [not A1M and not A2M and BM and not CM] [MATCH_COUNTER_14]
      
      
      Particle events that matched for index 15 NA [MATCH_COUNTER_15]
      
      
      Particle events that were analyzed by hardware for index 0 [A1U and BU and not C2L] [READ_COUNTER_0]
      
      
      Particle events that were analyzed by hardware for index 1 [A2U and BU and not C2L] [READ_COUNTER_1]
      
      
      Particle events that were analyzed by hardware for index 2 [A1M and BM] [READ_COUNTER_2]
      
      
      Particle events that were analyzed by hardware for index 3 [A2M and BM] [READ_COUNTER_3]
      
      
      Particle events that were analyzed by hardware for index 4 [BU] [READ_COUNTER_4]
      
      
      Particle events that were analyzed by hardware for index 5 [EH and EI] [READ_COUNTER_5]
      
      
      Particle events that were analyzed by hardware for index 6 [not F1L and not BU and not C2H and not C2L and not CU and EH and EI and EM] [READ_COUNTER_6]
      
      
      Particle events that were analyzed by hardware for index 7 [not F1L and not BU and not C2H and not C2L and not CU and DH and DI] [READ_COUNTER_7]
      
      
      Particle events that were analyzed by hardware for index 8 [not F1L and not BU and not C2H and not C2L and not CU and DH and DI and EH and EI] [READ_COUNTER_8]
      
      
      Particle events that were analyzed by hardware for index 9 [DM and DL] [READ_COUNTER_9]
      
      
      Particle events that were analyzed by hardware for index 10 [not F1L and not A1U and not A2U and BU and not BH and not C2H and not C2L and not CU and not DH and not EH] [READ_COUNTER_10]
      
      
      Particle events that were analyzed by hardware for index 11 [A2U and BU and CU and DH and EH] [READ_COUNTER_11]
      
      
      Particle events that were analyzed by hardware for index 12 [not A1U and not A2U and not BU and not CU and DH and EH] [READ_COUNTER_12]
      
      
      Particle events that were analyzed by hardware for index 13 [A2U and BU and CU and DH and not EH] [READ_COUNTER_13]
      
      
      Particle events that were analyzed by hardware for index 14 [not A1M and not A2M and BM and not CM] [READ_COUNTER_14]
      
      
      Particle events that were analyzed by hardware for index 15 NA [READ_COUNTER_15]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MSL_RAD_OBS-L2
Description
The Radiation Assessment Detector (RAD) and its data products are described in
detail in the literature (Hassler et al., 2012). Each RAD observation contains
the following: (1) Instrument counters, (2) Neutral particle count histograms in
detectors D and E, (3) LET count histograms, (4) Absorbed dose rate in detectors
B and E, (5) High-cadence dose rate in B and E (16 rates per observation).
 
  • Data Variable Descriptions
      [Quality filtered] Actual instrument observation time [ALIVE_TIME_f]
      
      
      [Quality filtered] Radiation dose rate on Mars (recorded in Si, corrected for MMRTG contribution, and tissue-equivalent plastic) [DOSIMETRY_TOTAL_f]
      
      
      [Quality filtered] Total Dose for an observation at 1/16th timeslice of an observation [DOSIMETRY_TIMESLICE_f]
      
      
      [Quality filtered] LET spectrum on Mars in Si (geometric factor ~ 0.9 cm^2 sr) [LET_A1A2_f]
      
      
      [Quality filtered] Neutral particle (neutrons + gamma rays) counts on Mars [HISTOGRAM_NEUTRAL_DE_f]
      
      
      [Quality filtered] Neutral particle counts in CsI [HISTOGRAM_NEUTRAL_D_f]
      
      
      [Quality filtered] Neutral particle counts in tissue-equivalent plastic [HISTOGRAM_NEUTRAL_E_f]
      
      
      [All quality] Actual instrument observation time [ALIVE_TIME]
      
      
      [All quality] Radiation dose rate on Mars (recorded in Si, corrected for MMRTG contribution, and tissue-equivalent plastic) [DOSIMETRY_TOTAL]
      
      
      [All quality] Total Dose for an observation at 1/16th timeslice of an observation [DOSIMETRY_TIMESLICE]
      
      
      [All quality] LET spectrum on Mars in Si (geometric factor ~ 0.9 cm^2 sr) [LET_A1A2]
      
      
      [All quality] Neutral particle (neutrons + gamma rays) counts on Mars [HISTOGRAM_NEUTRAL_DE]
      
      
      [All quality] Neutral particle counts in CsI [HISTOGRAM_NEUTRAL_D]
      
      
      [All quality] Neutral particle counts in tissue-equivalent plastic [HISTOGRAM_NEUTRAL_E]
      
      
      [NO PLOT] Quality indicator - flagged data has quality issues from various sources, Commanding, DAN activity, Other; no value=good [FLAGGED_DATA]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MUNIN_M1_MDSE (spase://ESA/NumericalData/Munin/MEDUSA/Electron/PT0.25S)
Description
References:                                             
1. The Instrument Data File Set. URL http://www.idfs.org 
Modification History
Initial Release
 
  • Data Variable Descriptions
      Science data in units of Telemetry (Dimensionless) [MEDUSA_Electron_1_Telemetry_Dimensionless]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of Telemetry (Dimensionless) [MEDUSA_Electron_1_Telemetry_D_atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of Telemetry (Dimensionless) [MEDUSA_Electron_1_Telemetry_D_atSensor]
      
      
      Science data in units of >c/acc [MEDUSA_Electron_2_gt_c_acc_gt_c_per_acc]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of >c/acc [MEDUSA_Electron_2_gt_c_acc_gt_c_per_acc-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of >c/acc [MEDUSA_Electron_2_gt_c_acc_gt_c_per_acc-atSensor]
      
      
      Science data in units of c/acc [MEDUSA_Electron_3_c_acc_c_per_acc]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of c/acc [MEDUSA_Electron_3_c_acc_c_per_acc-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of c/acc [MEDUSA_Electron_3_c_acc_c_per_acc-atSensor]
      
      
      Science data in units of #/sec (cnts/sec) [MEDUSA_Electron_4_num_sec_cnts_per_sec]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of #/sec(cnts/sec) [MEDUSA_Electron_4_num_sec_cnts_per_sec-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of #/sec(cnts/sec) [MEDUSA_Electron_4_num_sec_cnts_per_sec-atSensor]
      
      
      Science data in units of #/sec (cor cnts/sec) [MEDUSA_Electron_5_num_sec_cor_cnts_per_sec]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of #/sec(cor cnts/sec) [MEDUSA_Electron_5_num_sec_cor_cnts_per_sec-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of #/sec(cor cnts/sec) [MEDUSA_Electron_5_num_sec_cor_cnts_per_sec-atSensor]
      
      
      Science data in units of NFLUX (cnts/(cm**2 sr s)) [MEDUSA_Electron_6_NFLUX_cnts_per_cm_2_sr_s]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of NFLUX (cnts/(cm**2 sr s)) [MEDUSA_Electron_6_NFLUX_cnts_per_cm_2_sr_s-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of NFLUX (cnts/(cm**2 sr s)) [MEDUSA_Electron_6_NFLUX_cnts_per_cm_2_sr_s-atSensor]
      
      
      Science data in units of dNFLUX (cnts/(cm**2 sr s eV)) [MEDUSA_Electron_7_dNFLUX_cnts_per_cm_2_sr_s_eV]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of dNFLUX (cnts/(cm**2 sr s eV)) [MEDUSA_Electron_7_dNFLUX_cnts_per_cm_2_sr_s_eV-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of dNFLUX (cnts/(cm**2 sr s eV)) [MEDUSA_Electron_7_dNFLUX_cnts_per_cm_2_sr_s_eV-atSensor]
      
      
      Science data in units of dEFLUX (ergs/(cm**2 str s eV) [MEDUSA_Electron_8_dEFLUX_ergs_per_cm_2_str_s_eV]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of dEFLUX (ergs/(cm**2 str s eV) [MEDUSA_Electron_8_dEFLUX_ergs_per_cm_2_str_s_eV-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of dEFLUX (ergs/(cm**2 str s eV) [MEDUSA_Electron_8_dEFLUX_ergs_per_cm_2_str_s_eV-atSensor]
      
      
      Science data in units of DF (sec**3/km**6) [MEDUSA_Electron_9_DF_sec_3_per_km_6]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of DF (sec**3/km**6) [MEDUSA_Electron_9_DF_sec_3_per_km_6-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of DF (sec**3/km**6) [MEDUSA_Electron_9_DF_sec_3_per_km_6-atSensor]
      
      
      Science data in units of DF (sec**3/m**6) [MEDUSA_Electron_10_DF_sec_3_per_m_6]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of DF (sec**3/m**6) [MEDUSA_Electron_10_DF_sec_3_per_m_6-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of DF (sec**3/m**6) [MEDUSA_Electron_10_DF_sec_3_per_m_6-atSensor]
      
      
      Science data in units of DF (sec**3/cm**6) [MEDUSA_Electron_11_DF_sec_3_per_cm_6]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of DF (sec**3/cm**6) [MEDUSA_Electron_11_DF_sec_3_per_cm_6-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of DF (sec**3/cm**6) [MEDUSA_Electron_11_DF_sec_3_per_cm_6-atSensor]
      
      
      Data quality Electron Sensor 4 (11.25 deg) [Data_Quality_Munin_MEDUSA_Electron_4_11_25_deg]
      
      
      Data quality Electron Sensor 6 (33.75 deg) [Data_Quality_Munin_MEDUSA_Electron_6_33_75_deg]
      
      
      Data quality Electron Sensor 8 (56.25 deg) [Data_Quality_Munin_MEDUSA_Electron_8_56_25_deg]
      
      
      Data quality Electron Sensor 10 (78.75 deg) [Data_Quality_Munin_MEDUSA_Electron_10_78_75_deg]
      
      
      Data quality Electron Sensor 12 (101.25 deg) [Data_Quality_Munin_MEDUSA_Electron_12_101_25_deg]
      
      
      Data quality Electron Sensor 14 (123.75 deg) [Data_Quality_Munin_MEDUSA_Electron_14_123_75_deg]
      
      
      Data quality Electron Sensor 15 (146.25 deg) [Data_Quality_Munin_MEDUSA_Electron_15_146_25_deg]
      
      
      Data quality Electron Sensor 13 (168.75 deg) [Data_Quality_Munin_MEDUSA_Electron_13_168_75_deg]
      
      
      Data quality Electron Sensor 2 (-11.25 deg) [Data_Quality_Munin_MEDUSA_Electron_2_Neg_11_25_deg]
      
      
      Data quality Electron Sensor 0 (-33.75 deg) [Data_Quality_Munin_MEDUSA_Electron_0_Neg_33_75_deg]
      
      
      Data quality Electron Sensor 1 (-56.25 deg) [Data_Quality_Munin_MEDUSA_Electron_1_Neg_56_25_deg]
      
      
      Data quality Electron Sensor 3 (-78.75 deg) [Data_Quality_Munin_MEDUSA_Electron_3_Neg_78_75_deg]
      
      
      Data quality Electron Sensor 5 (-101.25 deg) [Data_Quality_Munin_MEDUSA_Electron_5_Neg_101_25_deg]
      
      
      Data quality Electron Sensor 7 (-123.75 deg) [Data_Quality_Munin_MEDUSA_Electron_7_Neg_123_75_deg]
      
      
      Data quality Electron Sensor 9 (-146.25 deg) [Data_Quality_Munin_MEDUSA_Electron_9_Neg_146_25_deg]
      
      
      Data quality Electron Sensor 11 (-168.75 deg) [Data_Quality_Munin_MEDUSA_Electron_11_Neg_168_75]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MUNIN_M1_MDSI (spase://ESA/NumericalData/Munin/MEDUSA/Ion/PT0.25S)
Description
References:                                             
1. The Instrument Data File Set. URL http://www.idfs.org 
Modification History
Initial Release
 
  • Data Variable Descriptions
      Science data in units of Telemetry (Dimensionless) [MEDUSA_Ion_1_Telemetry_Dimensionless]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of Telemetry (Dimensionless) [MEDUSA_Ion_1_Telemetry_D_atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of Telemetry (Dimensionless) [MEDUSA_Ion_1_Telemetry_D_atSensor]
      
      
      Science data in units of >c/acc [MEDUSA_Ion_2_gt_c_acc_gt_c_per_acc]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of >c/acc [MEDUSA_Ion_2_gt_c_acc_gt_c_per_acc-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of >c/acc [MEDUSA_Ion_2_gt_c_acc_gt_c_per_acc-atSensor]
      
      
      Science data in units of c/acc [MEDUSA_Ion_3_c_acc_c_per_acc]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of c/acc [MEDUSA_Ion_3_c_acc_c_per_acc-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of c/acc [MEDUSA_Ion_3_c_acc_c_per_acc-atSensor]
      
      
      Science data in units of #/sec (cnts/sec) [MEDUSA_Ion_4_num_sec_cnts_per_sec]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of #/sec (cnts/sec) [MEDUSA_Ion_4_num_sec_cnts_per_sec-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of #/sec (cnts/sec) [MEDUSA_Ion_4_num_sec_cnts_per_sec-atSensor]
      
      
      Science data in units of #/sec (cor cnts/sec) [MEDUSA_Ion_5_num_sec_cor_cnts_per_sec]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of #/sec (cor cnts/sec) [MEDUSA_Ion_5_num_sec_cor_cnts_per_sec-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of #/sec (cor cnts/sec) [MEDUSA_Ion_5_num_sec_cor_cnts_per_sec-atSensor]
      
      
      Science data in units of NFLUX (cnts/(cm**2 sr s)) [MEDUSA_Ion_6_NFLUX_cnts_per_cm_2_sr_s]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of NFLUX (cnts/(cm**2 sr s)) [MEDUSA_Ion_6_NFLUX_cnts_per_cm_2_sr_s-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of NFLUX (cnts/(cm**2 sr s)) [MEDUSA_Ion_6_NFLUX_cnts_per_cm_2_sr_s-atSensor]
      
      
      Science data in units of dNFLUX (cnts/(cm**2 sr s eV)) [MEDUSA_Ion_7_dNFLUX_cnts_per_cm_2_sr_s_eV]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of dNFLUX (cnts/(cm**2 sr s eV)) [MEDUSA_Ion_7_dNFLUX_cnts_per_cm_2_sr_s_eV-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of dNFLUX (cnts/(cm**2 sr s eV)) [MEDUSA_Ion_7_dNFLUX_cnts_per_cm_2_sr_s_eV-atSensor]
      
      
      Science data in units of dEFLUX (ergs/(cm**2 str s eV) [MEDUSA_Ion_8_dEFLUX_ergs_per_cm_2_str_s_eV]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of dEFLUX (ergs/(cm**2 str s eV) [MEDUSA_Ion_8_dEFLUX_ergs_per_cm_2_str_s_eV-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of dEFLUX (ergs/(cm**2 str s eV) [MEDUSA_Ion_8_dEFLUX_ergs_per_cm_2_str_s_eV-atSensor]
      
      
      Science data in units of DF (sec**3/km**6) [MEDUSA_Ion_9_DF_sec_3_per_km_6]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of DF (sec**3/km**6) [MEDUSA_Ion_9_DF_sec_3_per_km_6-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of DF (sec**3/km**6) [MEDUSA_Ion_9_DF_sec_3_per_km_6-atSensor]
      
      
      Science data in units of DF (sec**3/m**6) [MEDUSA_Ion_10_DF_sec_3_per_m_6]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of DF (sec**3/m**6) [MEDUSA_Ion_10_DF_sec_3_per_m_6-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of DF (sec**3/m**6) [MEDUSA_Ion_10_DF_sec_3_per_m_6-atSensor]
      
      
      Science data in units of DF (sec**3/cm**6) [MEDUSA_Ion_11_DF_sec_3_per_cm_6]
      
      
      ---> Spectrograms by Scan at sample Sensors - Science data in units of DF (sec**3/cm**6) [MEDUSA_Ion_11_DF_sec_3_per_cm_6-atScan]
      
      
      ---> Spectrograms by Sensor at sample Scans - Science data in units of DF (sec**3/cm**6) [MEDUSA_Ion_11_DF_sec_3_per_cm_6-atSensor]
      
      
      Data quality Ion Sensor 3 (11.25 deg) [Data_Quality_Munin_MEDUSA_Ion_3_11_25_deg]
      
      
      Data quality Ion Sensor 1 (33.75 deg) [Data_Quality_Munin_MEDUSA_Ion_1_33_75_deg]
      
      
      Data quality Ion Sensor 0 (56.25 deg) [Data_Quality_Munin_MEDUSA_Ion_0_56_25_deg]
      
      
      Data quality Ion Sensor 2 (78.75 deg) [Data_Quality_Munin_MEDUSA_Ion_2_78_75_deg]
      
      
      Data quality Ion Sensor 4 (101.25 deg) [Data_Quality_Munin_MEDUSA_Ion_4_101_25_deg]
      
      
      Data quality Ion Sensor 6 (123.75 deg) [Data_Quality_Munin_MEDUSA_Ion_6_123_75_deg]
      
      
      Data quality Ion Sensor 8 (146.25 deg) [Data_Quality_Munin_MEDUSA_Ion_8_146_25_deg]
      
      
      Data quality Ion Sensor 10 (168.75 deg) [Data_Quality_Munin_MEDUSA_Ion_10_168_75_deg]
      
      
      Data quality Ion Sensor 5 (-11.25 deg) [Data_Quality_Munin_MEDUSA_Ion_5_Neg_11_25_deg]
      
      
      Data quality Ion Sensor 7 (-33.75 deg) [Data_Quality_Munin_MEDUSA_Ion_7_Neg_33_75_deg]
      
      
      Data quality Ion Sensor 9 (-56.25 deg) [Data_Quality_Munin_MEDUSA_Ion_9_Neg_56_25_deg]
      
      
      Data quality Ion Sensor 11 (78.75 deg) [Data_Quality_Munin_MEDUSA_Ion_11_Neg_78_75_deg]
      
      
      Data quality Ion Sensor 13 (-101.25 deg) [Data_Quality_Munin_MEDUSA_Ion_13_Neg_101_25_deg]
      
      
      Data quality Ion Sensor 15 (-123.75 deg) [Data_Quality_Munin_MEDUSA_Ion_15_Neg_123_75_deg]
      
      
      Data quality Ion Sensor 14 (-146.25 deg) [Data_Quality_Munin_MEDUSA_Ion_14_Neg_146_25_deg]
      
      
      Data quality Ion Sensor 12 (168.75 deg) [Data_Quality_Munin_MEDUSA_Ion_12_Neg_168_75_deg]
      
      
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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MUNIN_M1_OA (spase://ESA/NumericalData/Munin/Ephemeris/PT0.25S)
Description
References:                                             
1. The Instrument Data File Set. URL http://www.idfs.org 
Modification History
Initial Release
 
  • Data Variable Descriptions
      Altitude [Altitude]
      
      
      CGLat [CGLat]
      
      
      ---> CGLong [CGLong]
      
      
      Latitude [Latitude]
      
      
      ---> Longitude [Longitude]
      
      
      MLT [MLT]
      
      
      L-shell [L_shell]
      
      
      Eclipse Status [Eclipse_status]
      
      
      GEI X [GEI_X]
      
      
      ---> GEI Y [GEI_Y]
      
      
      ---> GEI Z [GEI_Z]
      
      
      GEI Vx [GEI_Vx]
      
      
      ---> GEI Vy [GEI_Vy]
      
      
      ---> GEI Vz [GEI_Vz]
      
      
      GEI Sun-X [GEI_Sun_X]
      
      
      ---> GEI Sun-Y [GEI_Sun_Y]
      
      
      ---> GEI Sun-Z [GEI_Sun_Z]
      
      
      GEO X [GEO_X]
      
      
      ---> GEO Y [GEO_Y]
      
      
      ---> GEO Z [GEO_Z]
      
      
      RA [RA]
      
      
      ---> Declination [Declination]
      
      
      Sun angle [Sun_Angle]
      
      
      B-field angle [B_field_Angle]
      
      
      Spin period [Spin_period]
      
      
Dataset in CDAWeb
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MVN_INSITU_KP-4SEC doi:10.48322/p7yg-g215
Proper citations should include the "Accessed on date" in the form .
Description
Multi-Instrument
 
  • Data Variable Descriptions
      Electron density (LPW) [LPW_Electron_density]
      Derived from the LP sweep and when available from the plasma line
      
      ---> Electron density min (LPW) [LPW_Electron_density_min]
      
      
      ---> Electron density max (LPW) [LPW_Electron_density_max]
      
      
      Electron temperature (LPW) [LPW_Electron_temperature]
      Derived from the LP sweep
      
      ---> Electron temperature min (LPW) [LPW_Electron_temperature_min]
      
      
      ---> Electron temperature max (LPW) [LPW_Electron_temperature_max]
      
      
      Spacecraft potential (LPW) [LPW_Spacecraft_potential]
      Measured from the probe potentials
      
      ---> Spacecraft potential min (LPW) [LPW_Spacecraft_potential_min]
      
      
      ---> Spacecraft potential max (LPW) [LPW_Spacecraft_potential_max]
      
      
      E-field wave power 2-100 Hz (LPW) [LPW_E_field_wave_power_2_100]
      Integrated wave power from the onboard calculated FFT, frequencies important for
      wave heating
      
      ---> E-field wave power 2-100 Hz data quality (LPW) [LPW_E_field_wave_power_2_100_data_quality]
      Range: 0-100, where 100 is the highest confidence level, use data with quality
      flag of 50 or above
      
      E-field wave power 100-800 Hz (LPW) [LPW_E_field_wave_power_100_800]
      Integrated wave power from the onboard calculated FFT
      
      ---> E-field wave power 100-800 Hz data quality (LPW) [LPW_E_field_wave_power_100_800_data_quality]
      Range: 0-100, where 100 is the highest confidence level, use data with quality
      flag of 50 or above
      
      E-field wave power 800-1000 Hz (LPW) [LPW_E_field_wave_power_800_1000]
      Integrated wave power from the onboard calculated FFT
      
      ---> E-field wave power 800-1000 Hz data quality (LPW) [LPW_E_field_wave_power_800_1000_data_quality]
      Range: 0-100, where 100 is the highest confidence level, use data with quality
      flag of 50 or above
      
      EUV irradiance wave power 0.1-7.0 nm bandpass (LPW-EUV) [LPW_EUV_irradiance_pt1_7]
      
      
      ---> EUV irradiance wave power 0.1-7.0 nm data quality (LPW-EUV) [LPW_EUV_irradiance_pt1_7_data_quality]
      0 = good solar, 1 = occultation, 2 = no pointing info, 3 = Sun NOT fully in FOV,
      4 = Sun NOT in FOV, 5 = windowed, 6 = eclipse, 7 = spare
      
      EUV irradiance wave power 17-22 nm bandpass (LPW-EUV) [LPW_EUV_irradiance_17_22]
      
      
      ---> EUV irradiance wave power 17-22 nm data quality (LPW-EUV) [LPW_EUV_irradiance_17_22_data_quality]
      0 = good solar, 1 = occultation, 2 = no pointing info, 3 = Sun NOT fully in FOV,
      4 = Sun NOT in FOV, 5 = windowed, 6 = eclipse, 7 = spare
      
      EUV irradiance wave power Lyman-alpha bandpass (LPW-EUV) [LPW_EUV_irradiance_lyman_alpha]
      
      
      ---> EUV irradiance wave power Lyman-alpha data quality (LPW-EUV) [LPW_EUV_irradiance_lyman_alpha_data_quality]
      0 = good solar, 1 = occultation, 2 = no pointing info, 3 = Sun NOT fully in FOV,
      4 = Sun NOT in FOV, 5 = windowed, 6 = eclipse, 7 = spare
      
      Solar wind electron density (SWEA) [SWEA_Electron_density]
      Density of solar wind or magnetosheath electrons based on moments of the
      electron distribution after correcting for the spacecraft potential
      
      ---> Solar wind electron density data quality (SWEA) [SWEA_Electron_density_quality]
      Statistical uncertainty,  (1 sigma),  not including systematic error
      
      Solar wind electron temperature (SWEA) [SWEA_Electron_temperature]
      Temperature of solar wind or magnetosheath electrons based on moments of the
      electron distribution after correcting for the spacecraft potential
      
      ---> Solar wind electron temperature data quality (SWEA) [SWEA_Electron_temperature_quality]
      Statistical uncertainty,  (1 sigma),  not including systematic error
      
      Electron energy flux parallel 5-100 eV (SWEA) [SWEA_Electron_parallel_flux_5_100]
      Electron energy flux parallel to the magnetic field vector (0-90 degrees pitch
      angle)
      
      ---> Electron energy flux parallel 5-100 eV data quality (SWEA) [SWEA_Electron_parallel_flux_5_100_data_quality]
      
      
      Electron energy flux parallel 100-500 eV (SWEA) [SWEA_Electron_parallel_flux_100_500]
      Electron energy flux parallel to the magnetic field vector (0-90 degrees pitch
      angle)
      
      ---> Electron energy flux parallel 100-500 eV data quality (SWEA) [SWEA_Electron_parallel_flux_100_500_data_quality]
      
      
      Electron energy flux parallel 500-1000 eV (SWEA) [SWEA_Electron_parallel_flux_500_1000]
      Electron energy flux parallel to the magnetic field vector (0-90 degrees pitch
      angle)
      
      ---> Electron energy flux parallel 500-1000 eV data quality (SWEA) [SWEA_Electron_parallel_flux_500_1000_data_quality]
      
      
      Electron energy flux anti-parallel 5-100 eV (SWEA) [SWEA_Electron_anti_parallel_flux_5_100]
      Electron energy flux anti-parallel to the magnetic field vector (90-180 degrees
      pitch angle)
      
      ---> Electron energy flux anti-parallel 5-100 eV data quality (SWEA) [SWEA_Electron_anti_parallel_flux_5_100_data_quality]
      
      
      Electron energy flux anti-parallel 100-500 eV (SWEA) [SWEA_Electron_anti_parallel_flux_100_500]
      Electron energy flux anti-parallel to the magnetic field vector (90-180 degrees
      pitch angle)
      
      ---> Electron energy flux anti-parallel 100-500 eV data quality (SWEA) [SWEA_Electron_anti_parallel_flux_100_500_data_quality]
      
      
      Electron energy flux anti-parallel 500-1000 eV (SWEA) [SWEA_Electron_anti_parallel_flux_500_1000]
      Electron energy flux anti-parallel to the magnetic field vector (90-180 degrees
      pitch angle)
      
      ---> Electron energy flux anti-parallel 500-1000 eV data quality (SWEA) [SWEA_Electron_anti_parallel_flux_500_1000_data_quality]
      
      
      Electron spectrum shape parameter (SWEA) [SWEA_Electron_spectrum_shape]
      Energy spectrum shape parameter used to distingush between ionospheric
      photoelectrons  and solar wind electrons
      
      ---> Electron spectrum shape parameter data quality (SWEA) [SWEA_Electron_spectrum_shape_data_quality]
      
      
      Total ion density from onboard moment calculation, assuming 100% protons (SWIA) [SWIA_Hplus_density]
      
      
      ---> Total ion density data quality (SWIA) [SWIA_Hplus_density_data_quality]
      Quality flag (0 = bad, 1 = good) indicating whether the distribution is
      well-measured and decommutation parameters are definite
      
      Bulk ion flow velocity XYZ component from onboard moment calculation, assuming 100% protons (SWIA) [SWIA_Hplus_flow_velocity_MSO]
      
      
      ---> Bulk ion flow velocity XYZ data quality (SWIA) [SWIA_Hplus_flow_velocity_MSO_data_quality]
      Quality flag (0 = bad, 1 = good) indicating whether the distribution is
      well-measured and decommutation parameters are definite
      
      Scalar ion temperature from onboard moment calculation, assuming 100% protons (SWIA) [SWIA_Hplus_temperature]
      
      
      ---> Scalar ion temperature data quality (SWIA) [SWIA_Hplus_temperature_data_quality]
      Quality flag (0 = bad, 1 = good) indicating whether the distribution is
      well-measured and decommutation parameters are definite
      
      Ion dynamic pressure computed on ground from density and velocity moments, assuming 100% protons (SWIA) [SWIA_dynamic_pressure]
      
      
      ---> Ion dynamic pressure data quality (SWIA) [SWIA_dynamic_pressure_data_quality]
      Quality flag (0 = bad, 1 = good) indicating whether the distribution is
      well-measured and decommutation parameters are definite
      
      STATIC Data quality [STATIC_Quality]
      Integer flag bits, Valid=0, Flag=1, See KP SIS for bit descriptions (formatted
      as a float in order to include NaN values for data gaps) 
      
      H+ density (STATIC) [STATIC_Hplus_density]
      H+ number density below TBD altitude determined from APID c6 (32 energy x 64
      mass) while in Ram or Conic modes
      
      ---> H+ density data quality (STATIC) [STATIC_Hplus_density_data_quality]
      Number of counts in the measurement
      
      O+ density (STATIC) [STATIC_Oplus_density]
      O+ number density below TBD altitude determined from APID c6 (32 energy x 64
      mass) while in Ram or Conic modes
      
      ---> O+ density data quality (STATIC) [STATIC_Oplus_density_data_quality]
      Number of counts in the measurement
      
      O2+ density (STATIC) [STATIC_O2plus_density]
      O2+ number density below TBD altitude determined from APID c6 (32 energy x 64
      mass) while in Ram or Conic modes
      
      ---> O2+ density data quality (STATIC) [STATIC_O2plus_density_data_quality]
      Number of counts in the measurement
      
      H+ temperature (STATIC) [STATIC_Hplus_temperature]
      H+ RAM temperature below TBD altitude determined from APID c6 (32 energy x 64
      mass) while in Ram or Conic modes
      
      ---> H+ temperature data quality (STATIC) [STATIC_Hplus_temperature_data_quality]
      Number of counts in the measurement
      
      O+ temperature (STATIC) [STATIC_Oplus_temperature]
      O+ RAM temperature below TBD altitude determined from APID c6 (32 energy x 64
      mass) while in Ram or Conic modes
      
      ---> O+ temperature data quality (STATIC) [STATIC_Oplus_temperature_data_quality]
      Number of counts in the measurement
      
      O2+ temperature (STATIC) [STATIC_O2plus_temperature]
      O2+ RAM temperature below TBD altitude determined from APID c6 (32 energy x 64
      mass) while in Ram or Conic modes
      
      ---> O2+ temperature data quality (STATIC) [STATIC_O2plus_temperature_data_quality]
      Number of counts in the measurement
      
      O2+ MAVEN_APP XYZ component of velocity below TBD altitude determined from APID c6 while in Ram or Conic mode (STATIC) [STATIC_O2plus_flow_velocity_MAVEN_APP]
      
      
      ---> O2+ MAVEN_APP XYZ component of velocity data quality (STATIC) [STATIC_O2plus_flow_velocity_MAVEN_APP_data_quality]
      Number of counts in the measurement
      
      O2+ MSO XYZ component of velocity below TBD altitude while in Ram or Conic mode (STATIC) [STATIC_O2plus_flow_velocity_MSO]
      
      
      ---> O2+ MSO XYZ component of velocity data quality (STATIC) [STATIC_O2plus_flow_velocity_MSO_data_quality]
      Number of counts in the measurement
      
      H+ omni-directional flux (STATIC) [STATIC_Hplus_omni_directional_flux]
      H+ omni-directional flux above TBD altitude determined from APID c6 while in
      Pickup, Eclipse and Protect mode
      
      H+ characteristic energy (STATIC) [STATIC_Hplus_characteristic_energy]
      H+ omni-directional characteristic energy above TBD altitude determined from
      APID c6 while in Pickup, Eclipse and Protect mode
      
      ---> H+ characteristic energy data quality (STATIC) [STATIC_Hplus_characteristic_energy_DQ]
      Number of counts in the measurement
      
      He+ omni-directional flux (STATIC) [STATIC_HEplus_omni_directional_flux]
      HE+ omni-directional flux above TBD altitude determined from APID c6 while in
      Pickup, Eclipse and Protect mode
      
      He+ characteristic energy (STATIC) [STATIC_HEplus_characteristic_energy]
      HE+ omni-directional characteristic energy above TBD altitude determined from
      APID c6 while in Pickup, Eclipse and Protect mode
      
      ---> He+ characteristic energy data quality (STATIC) [STATIC_HEplus_characteristic_energy_DQ]
      Number of counts in the measurement
      
      O+ omni-directional flux (STATIC) [STATIC_Oplus_omni_directional_flux]
      O+ omni-directional flux above TBD altitude determined from APID c6 while in
      Pickup, Eclipse and Protect mode
      
      O+ characteristic energy (STATIC) [STATIC_Oplus_characteristic_energy]
      O+ omni-directional characteristic energy above TBD altitude determined from
      APID c6 while in Pickup, Eclipse and Protect mode
      
      ---> O+ characteristic energy data quality (STATIC) [STATIC_Oplus_characteristic_energy_DQ]
      Number of counts in the measurement
      
      O2+ omni-directional flux (STATIC) [STATIC_O2plus_omni_directional_flux]
      O2+ omni-directional flux above TBD altitude determined from APID c6 while in
      Pickup, Eclipse and Protect mode
      
      O2+ characteristic energy (STATIC) [STATIC_O2plus_characteristic_energy]
      O2+ omni-directional characteristic energy above TBD altitude determined from
      APID c6 while in Pickup, Eclipse and Protect mode
      
      ---> O2+ characteristic energy data quality (STATIC) [STATIC_O2plus_characteristic_energy_DQ]
      Number of counts in the measurement
      
      H+ MSO X-direction of flux above TBD altitude determined from TBD APID while in Pickup and Scan mode (STATIC) [STATIC_Hplus_characteristic_direction_MSO]
      
      
      H+ characteristic width (STATIC) [STATIC_Hplus_characteristic_angular_width]
      H+ flux angular width above TBD altitude determined from TBD APID while in
      Pickup and Scan mode
      
      ---> H+ characteristic width data quality (STATIC) [STATIC_Hplus_characteristic_angular_width_DQ]
      Number of counts in the measurement
      
      Dominant pickup ion MSO XYZ direction of flux above TBD altitude determined from APID D0 and CE while in Pickup, Eclipse and Protect mode [STATIC_dominant_pickup_ion_characteristic_direction_MSO]
      
      
      Dominant pickup ion characteristic angular width (STATIC) [STATIC_dominant_pickup_ion_characteristic_angular_width]
      Dominant pickup ion flux angular width above TBD altitude determined from APID
      D0 and CE while in Pickup, Eclipse and Protect mode
      
      ---> Dominant pickup ion characteristic angular width DQ (STATIC) [STATIC_dominant_pickup_ion_characteristic_angular_width_DQ]
      Number of counts in the measurement
      
      Ion energy flux (30-1000 keV), FOV 1-F (SEP) [SEP_Ion_Energy_Flux_30_1000_FOV_1F]
      Number flux of ions, integrated over the energy range 0.03-1.0 MeV
      
      ---> Ion energy flux (30-1000 keV), FOV 1-F data quality (SEP) [SEP_Ion_Energy_Flux_30_1000_FOV_1F_data_quality]
      Standard uncertainty in total ion flux, based on Poisson statistics
      
      Ion energy flux (30-1000 keV), FOV 1-R (SEP) [SEP_Ion_Energy_Flux_30_1000_FOV_1R]
      Number flux of ions, integrated over the energy range 0.03-1.0 MeV
      
      ---> Ion energy flux (30-1000 keV), FOV 1-R data quality (SEP) [SEP_Ion_Energy_Flux_30_1000_FOV_1R_data_quality]
      Standard uncertainty in total ion flux, based on Poisson statistics
      
      Ion energy flux (30-1000 keV), FOV 2-F (SEP) [SEP_Ion_Energy_Flux_30_1000_FOV_2F]
      Number flux of ions, integrated over the energy range 0.03-1.0 MeV
      
      ---> Ion energy flux (30-1000 keV), FOV 2-F data quality (SEP) [SEP_Ion_Energy_Flux_30_1000_FOV_2F_data_quality]
      Standard uncertainty in total ion flux, based on Poisson statistics
      
      Ion energy flux (30-1000 keV), FOV 2-R (SEP) [SEP_Ion_Energy_Flux_30_1000_FOV_2R]
      Number flux of ions, integrated over the energy range 0.03-1.0 MeV
      
      ---> Ion energy flux (30-1000 keV), FOV 2-R data quality (SEP) [SEP_Ion_Energy_Flux_30_1000_FOV_2R_data_quality]
      Standard uncertainty in total ion flux, based on Poisson statistics
      
      Electron energy flux (30-300 keV), FOV 1-F (SEP) [SEP_Electron_Energy_Flux_30_300_FOV_1F]
      Number flux of electrons, integrated over the energy range 30-300 keV
      
      ---> Electron energy flux (30-300 keV), FOV 1-F data quality (SEP) [SEP_Electron_Energy_Flux_30_300_FOV_1F_data_quality]
      Standard uncertainty in total electron flux, based on Poisson statistics
      
      Electron energy flux (30-300 keV), FOV 1-R (SEP) [SEP_Electron_Energy_Flux_30_300_FOV_1R]
      Number flux of electrons, integrated over the energy range 30-300 keV
      
      ---> Electron energy flux (30-300 keV), FOV 1-R data quality (SEP) [SEP_Electron_Energy_Flux_30_300_FOV_1R_data_quality]
      Standard uncertainty in total electron flux, based on Poisson statistics
      
      Electron energy flux (30-300 keV), FOV 2-F (SEP) [SEP_Electron_Energy_Flux_30_300_FOV_2F]
      Number flux of electrons, integrated over the energy range 30-300 keV
      
      ---> Electron energy flux (30-300 keV), FOV 2-F data quality (SEP) [SEP_Electron_Energy_Flux_30_300_FOV_2F_data_quality]
      Standard uncertainty in total electron flux, based on Poisson statistics
      
      Electron energy flux (30-300 keV), FOV 2-R (SEP) [SEP_Electron_Energy_Flux_30_300_FOV_2R]
      Number flux of electrons, integrated over the energy range 30-300 keV
      
      ---> Electron energy flux (30-300 keV), FOV 2-R data quality (SEP) [SEP_Electron_Energy_Flux_30_300_FOV_2R_data_quality]
      Standard uncertainty in total electron flux, based on Poisson statistics
      
      SEP look direction 1-F MSO XYZ [SEP_Look_direction_1F_MSO]
      
      
      SEP look direction 1-R MSO XYZ [SEP_Look_direction_1R_MSO]
      
      
      SEP look direction 2-F MSO XYZ [SEP_Look_direction_2F_MSO]
      
      
      SEP look direction 2-R MSO XYZ [SEP_Look_direction_2R_MSO]
      
      
      Magnetic field vector component in the XYZ direction in MSO coordinates (MAG) [MAG_field_MSO]
      
      
      ---> Magnetic field vector component in MSO coordinates data quality (MAG) [MAG_field_MSO_data_quality]
      Unused column
      
      Magnetic field vector component in the XYZ direction in GEO coordinates (MAG) [MAG_field_GEO]
      
      
      ---> Magnetic field vector component in GEO coordinates data quality (MAG) [MAG_field_GEO_data_quality]
      Unused column
      
      Deviations from the mean magnetic field magnitude (MAG) [MAG_field_RMS_deviation]
      
      
      ---> Deviations from the mean magnetic field magnitude data quality (MAG) [MAG_field_RMS_deviation_data_quality]
      Unused column
      
      He density (NGIMS) [NGIMS_He_density]
      Abundance or upper limit
      
      ---> He density precision (NGIMS) [NGIMS_He_density_precision]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] He density data quality (NGIMS) [NGIMS_He_density_data_quality]
      NIV - Neutral Inbound Verified, NIU - Neutral Inbound Unverified, NOV - Neutral
      Outbound Verified, NOU - Neutral Outbound Unverified
      
      O density (NGIMS) [NGIMS_O_density]
      Abundance or upper limit
      
      ---> O density precision (NGIMS) [NGIMS_O_density_precision]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] O density data quality (NGIMS) [NGIMS_O_density_data_quality]
      NIV - Neutral Inbound Verified, NIU - Neutral Inbound Unverified, NOV - Neutral
      Outbound Verified, NOU - Neutral Outbound Unverified
      
      CO density (NGIMS) [NGIMS_CO_density]
      Abundance or upper limit
      
      ---> CO density precision (NGIMS) [NGIMS_CO_density_precision]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] CO density data quality (NGIMS) [NGIMS_CO_density_data_quality]
      NIV - Neutral Inbound Verified, NIU - Neutral Inbound Unverified, NOV - Neutral
      Outbound Verified, NOU - Neutral Outbound Unverified
      
      N2 density (NGIMS) [NGIMS_N2_density]
      Abundance or upper limit
      
      ---> N2 density precision (NGIMS) [NGIMS_N2_density_precision]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] N2 density data quality (NGIMS) [NGIMS_N2_density_data_quality]
      NIV - Neutral Inbound Verified, NIU - Neutral Inbound Unverified, NOV - Neutral
      Outbound Verified, NOU - Neutral Outbound Unverified
      
      NO density (NGIMS) [NGIMS_NO_density]
      Abundance or upper limit
      
      ---> NO density precision (NGIMS) [NGIMS_NO_density_precision]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] NO density data quality (NGIMS) [NGIMS_NO_density_data_quality]
      NIV - Neutral Inbound Verified, NIU - Neutral Inbound Unverified, NOV - Neutral
      Outbound Verified, NOU - Neutral Outbound Unverified
      
      Ar density (NGIMS) [NGIMS_Ar_density]
      Abundance or upper limit
      
      ---> Ar density precision (NGIMS) [NGIMS_Ar_density_precision]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] Ar density data quality (NGIMS) [NGIMS_Ar_density_data_quality]
      NIV - Neutral Inbound Verified, NIU - Neutral Inbound Unverified, NOV - Neutral
      Outbound Verified, NOU - Neutral Outbound Unverified
      
      CO2 density (NGIMS) [NGIMS_CO2_density]
      Abundance or upper limit
      
      ---> CO2 density precision (NGIMS) [NGIMS_CO2_density_precision]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] CO2 density data quality (NGIMS) [NGIMS_CO2_density_data_quality]
      NIV - Neutral Inbound Verified, NIU - Neutral Inbound Unverified, NOV - Neutral
      Outbound Verified, NOU - Neutral Outbound Unverified
      
      Ion density - amu 32+ (NGIMS) [NGIMS_Ion_density_32plus]
      Abundance or upper limit
      
      ---> Ion density precision - amu 32+ (NGIMS) [NGIMS_Ion_density_precision_32plus]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] Ion density data quality - amu 32+ (NGIMS) [NGIMS_Ion_density_data_quality_32plus]
      SCP - SpaceCraft Potential available and used as computed by STATIC, SC0 -
      SpaceCraft potential not available
      
      Ion density - amu 44+ (NGIMS) [NGIMS_Ion_density_44plus]
      Abundance or upper limit
      
      ---> Ion density precision - amu 44+ (NGIMS) [NGIMS_Ion_density_precision_44plus]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] Ion density data quality - amu 44+ (NGIMS) [NGIMS_Ion_density_data_quality_44plus]
      SCP - SpaceCraft Potential available and used as computed by STATIC, SC0 -
      SpaceCraft potential not available
      
      Ion density - amu 30+ (NGIMS) [NGIMS_Ion_density_30plus]
      Abundance or upper limit
      
      ---> Ion density precision - amu 30+ (NGIMS) [NGIMS_Ion_density_precision_30plus]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] Ion density data quality - amu 30+ (NGIMS) [NGIMS_Ion_density_data_quality_30plus]
      SCP - SpaceCraft Potential available and used as computed by STATIC, SC0 -
      SpaceCraft potential not available
      
      Ion density - amu 16+ (NGIMS) [NGIMS_Ion_density_16plus]
      Abundance or upper limit
      
      ---> Ion density precision - amu 16+ (NGIMS) [NGIMS_Ion_density_precision_16plus]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] Ion density data quality - amu 16+ (NGIMS) [NGIMS_Ion_density_data_quality_16plus]
      SCP - SpaceCraft Potential available and used as computed by STATIC, SC0 -
      SpaceCraft potential not available
      
      Ion density - amu 28+ (NGIMS) [NGIMS_Ion_density_28plus]
      Abundance or upper limit
      
      ---> Ion density precision - amu 28+ (NGIMS) [NGIMS_Ion_density_precision_28plus]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] Ion density data quality - amu 28+ (NGIMS) [NGIMS_Ion_density_data_quality_28plus]
      SCP - SpaceCraft Potential available and used as computed by STATIC, SC0 -
      SpaceCraft potential not available
      
      Ion density - amu 12+ (NGIMS) [NGIMS_Ion_density_12plus]
      Abundance or upper limit
      
      ---> Ion density precision - amu 12+ (NGIMS) [NGIMS_Ion_density_precision_12plus]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] Ion density data quality - amu 12+ (NGIMS) [NGIMS_Ion_density_data_quality_12plus]
      SCP - SpaceCraft Potential available and used as computed by STATIC, SC0 -
      SpaceCraft potential not available
      
      Ion density - amu 17+ (NGIMS) [NGIMS_Ion_density_17plus]
      Abundance or upper limit
      
      ---> Ion density precision - amu 17+ (NGIMS) [NGIMS_Ion_density_precision_17plus]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] Ion density data quality - amu 17+ (NGIMS) [NGIMS_Ion_density_data_quality_17plus]
      SCP - SpaceCraft Potential available and used as computed by STATIC, SC0 -
      SpaceCraft potential not available
      
      Ion density - amu 14+ (NGIMS) [NGIMS_Ion_density_14plus]
      Abundance or upper limit
      
      ---> Ion density precision - amu 14+ (NGIMS) [NGIMS_Ion_density_precision_14plus]
      % Error (1 sigma), if -1, the value is an upper limit
      
      ---> [DOES NOT PLOT] Ion density data quality - amu 14+ (NGIMS) [NGIMS_Ion_density_data_quality_14plus]
      SCP - SpaceCraft Potential available and used as computed by STATIC, SC0 -
      SpaceCraft potential not available
      
      XYZ-component of spacecraft position in Mars planetocentric (geographic) GEO coordinates [SPICE_spacecraft_GEO]
      same as IAU_MARS in SPICE
      
      XYZ-component of spacecraft position in MSO coordinates [SPICE_spacecraft_MSO]
      same as IAU_MARS in SPICE
      
      Spacecraft longitude GEO (SPICE) [SPICE_spacecraft_longitude_GEO]
      Longitudinal component of MAVEN's location with respect to Mars
      
      Spacecraft latitude GEO (SPICE) [SPICE_spacecraft_latitude_GEO]
      Latitudinal (areodetic) component of MAVEN's location with respect to IAU Mars
      ellipsoid, equatorial radius of 3396.2 km, polar radius of
      
      Spacecraft solar zenith angle (SPICE) [SPICE_spacecraft_sza]
      Angle measured from MAVEN to the geometric center of the Sun's disc, as
      described using a horizontal coordinate system
      
      Spacecraft local time (SPICE) [SPICE_spacecraft_local_time]
      Angle measured from MAVEN to the geometric center of the Sun's disc, as
      described using a horizontal coordinate system
      
      Spacecraft altitude w.r.t. aeroid (SPICE) [SPICE_spacecraft_altitude]
      Altitude (areodetic) with respect to IAU Mars ellipsoid, equatorial radius of
      3396.2 km, 
      
      XYZ-component of spacecraft attitude in GEO coordinates [SPICE_spacecraft_attitude_GEO]
      same as IAU_MARS in SPICE
      
      XYZ-component of spacecraft attitude in MSO coordinates [SPICE_spacecraft_attitude_MSO]
      same as IAU_MARS in SPICE
      
      XYZ-component of articulated payload platform (app) attitude in GEO coordinates [SPICE_app_attitude_GEO]
      XYZ-component of pointing direction of Articulated Payload Platform (z-axis of
      MAVEN_APP_BP frame) in GEO coordinates
      
      XYZ-component of articulated payload platform (app) attitude in MSO coordinates [SPICE_app_attitude_MSO]
      same as IAU_MARS in SPICE
      
      Orbit number (SPICE) [SPICE_Orbit_Number]
      Orbit number increments each time MAVEN reaches geometric periapsis
      
      ---> [DOES NOT PLOT] Inbound/Outbound Flag (SPICE) [Inbound_Outbound_Flag]
      Inbound (\'I\') is from geometric apoapsis to next geometric periapsis in time,
      outbound (\'O\') is the reverse
      
      Mars Season (Ls) (SPICE) [SPICE_Mars_season]
      Martian solar longitude. Ls = 0 (northern spring equinox), Ls = 90 (northern
      summer solstice), etc.
      
      Mars-Sun distance (SPICE) [SPICE_Mars_Sun_distance]
      
      
      Subsolar Point longitude GEO (SPICE) [SPICE_Subsolar_Point_longitude_GEO]
      GEO longitude of the sub-solar point
      
      Subsolar Point latitude GEO (SPICE) [SPICE_Subsolar_Point_latitude_GEO]
      GEO latitude of the sub-solar point
      
      Sub-Mars Point on the Sun, Longitude (SPICE) [SPICE_Sub_Mars_Point_longitude]
      Solar longitude of the center of the Sun as seen from Mars
      
      Sub-Mars Point on the Sun, Latitude (SPICE) [SPICE_Sub_Mars_Point_latitude]
      Solar latitude of the center of the Sun as seen from Mars
      
      Rotation matrix (IAU_MARS -> MAVEN_MSO) (SPICE) [Rotation_matrix_IAU_MARS_MAVEN_MSO]
      From IAU_MARS frame to MAVEN_MSO frame
      
      ---> Rotation matrix (MAVEN_SPACECRAFT -> MAVEN_MSO) (SPICE) [Rotation_matrix_SPACECRAFT_MAVEN_MSO]
      From MAVEN_SPACECRAFT frame to MAVEN_MSO frame
      
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MVN_MAG_L2-SUNSTATE-1SEC doi:10.48322/b9da-ph25
Proper citations should include the "Accessed on date" in the form .
Description
MAG>Mag
 
  • Data Variable Descriptions
      OUTBOARD B J2000 [OB_B]
      
      
      ---> OUTBOARD B J2000 range [OB_B_range]
      
      
      SC position [POSN]
      
      
      OUTBOARD BD PAYLOAD [OB_BDPL]
      
      
      ---> OUTBOARD BD PAYLOAD range [OB_BDPL_range]
      
      
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MVN_SEP_L2_S1-CAL-SVY-FULL (spase://NASA/NumericalData/MAVEN/SEP/Level2/Sensor1/Survey/PT8S)
Description
MAVEN SEP electron and ion Flux
Modification History
Revision 0
 
  • Data Variable Descriptions
      Attenuator state, 0=error, 1=open, 2=closed, 3=mixed [attenuator_state]
      
      
      Differential ion flux in forward look direction (#/cm^2/sec/ster/keV) [f_ion_flux]
      
      
      Total (integrated) ion flux in forward look direction (#/cm^2/sec/ster) [f_ion_flux_tot]
      
      
      Differential electron flux in forward look direction (#/cm^2/sec/ster/keV) [f_elec_flux]
      
      
      Total (integrated) electron flux in forward look direction (#/cm^2/sec/ster) [f_elec_flux_tot]
      
      
      Differential ion flux in reverse look direction (#/cm^2/sec/ster/keV) [r_ion_flux]
      
      
      Total (integrated) ion flux in reverse look direction (#/cm^2/sec/ster) [r_ion_flux_tot]
      
      
      Differential electron flux in reverse look direction (#/cm^2/sec/ster/keV) [r_elec_flux]
      
      
      Total (integrated) electron flux in reverse look direction (#/cm^2/sec/ster) [r_elec_flux_tot]
      
      
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MVN_SEP_L2_S2-CAL-SVY-FULL (spase://NASA/NumericalData/MAVEN/SEP/Level2/Sensor2/Survey/PT8S)
Description
MAVEN SEP electron and ion flux
Modification History
Revision 0
 
  • Data Variable Descriptions
      Attenuator state, 0=error, 1=open, 2=closed, 3=mixed [attenuator_state]
      
      
      Differential ion flux in forward look direction (#/cm^2/sec/ster/keV) [f_ion_flux]
      
      
      Total (integrated) ion flux in forward look direction (#/cm^2/sec/ster) [f_ion_flux_tot]
      
      
      Differential electron flux in forward look direction (#/cm^2/sec/ster/keV) [f_elec_flux]
      
      
      Total (integrated) electron flux in forward look direction (#/cm^2/sec/ster) [f_elec_flux_tot]
      
      
      Differential ion flux in reverse look direction (#/cm^2/sec/ster/keV) [r_ion_flux]
      
      
      Total (integrated) ion flux in reverse look direction (#/cm^2/sec/ster) [r_ion_flux_tot]
      
      
      Differential electron flux in reverse look direction (#/cm^2/sec/ster/keV) [r_elec_flux]
      
      
      Total (integrated) electron flux in reverse look direction (#/cm^2/sec/ster) [r_elec_flux_tot]
      
      
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MVN_STA_L2_D8-12R1E (spase://NASA/NumericalData/MAVEN/STATIC/Level2/Distributions/APIDd8/PT4S)
Description
STATIC>Supra-Thermal And Thermal Ion Composition Particle Distributions
Modification History
Rev-1 2014-04-28
 
  • Data Variable Descriptions
      Rate data for the rate channels sorted by energy step [rates]
      Rate data for the rate channels sorted by energy step with dimension (NUM_DISTS,
      NRATE, NENERGY) units=counts/s
      
      Quality flag [quality_flag]
      Quality flag (NUM_DISTS elements)
      
      ---> Validity flag codes valid data (bit 0), test pulser on (bit 1), diag mode (bit 2), data comp type (bit 3-4), packet compn (bit 5) [valid]
      ---> Validity flag codes valid data (bit 0), test pulser on (bit 1), diagnostic
      mode (bit 2), data compression type (bit 3-4), packet compression (bit 5)
      (NUM_DISTS elements)
      
      ---> Decoded mode number [mode]
      ---> Decoded mode number. (NUM_DISTS elements)
      
      ---> Index that identifies the energy and deflector sweep look up tables (LUT) for the sensor [swp_ind]
      ---> Index that identifies the energy and deflector sweep look up tables (LUT)
      for the sensor. SWP_IND is an index that selects the following support data
      arrays: ENERGY, DENERGY, THETA, DTHETA, PHI, DPHI, DOMEGA, GF and MASS_ARR.
      (NUM_DISTS elements), EN_IND Le NSWP
      
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MVN_STA_L2_D9-12R64E (spase://NASA/NumericalData/MAVEN/STATIC/Level2/Distributions/APIDd9/PT128S)
Description
STATIC> Supra-Thermal And Thermal Ion Composition Particle Distributions
Modification History
Rev-1 2014-04-28
 
  • Data Variable Descriptions
      Rate data for the rate channels sorted by energy step [rates]
      Rate data for the rate channels sorted by energy step with dimension (NUM_DISTS,
      NRATE, NENERGY) units=counts/s
      
      Quality flag [quality_flag]
      Quality flag (NUM_DISTS elements)
      
      ---> Validity flag codes valid data (bit 0), test pulser on (bit 1), diag mode (bit 2), data comp type (bit 3-4), packet compn (bit 5) [valid]
      ---> Validity flag codes valid data (bit 0), test pulser on (bit 1), diagnostic
      mode (bit 2), data compression type (bit 3-4), packet compression (bit 5)
      (NUM_DISTS elements)
      
      ---> Decoded mode number [mode]
      ---> Decoded mode number. (NUM_DISTS elements)
      
      Decoded telemetry rate number [rate]
      Decoded telemetry rate number. (NUM_DISTS elements)
      
      ---> Index that identifies the energy and deflector sweep look up tables (LUT) for the sensor [swp_ind]
      ---> Index that identifies the energy and deflector sweep look up tables (LUT)
      for the sensor. SWP_IND is an index that selects the following support data
      arrays: ENERGY, DENERGY, THETA, DTHETA, PHI, DPHI, DOMEGA, GF and MASS_ARR.
      (NUM_DISTS elements), EN_IND Le NSWP
      
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MVN_STA_L2_DA-1R64E (spase://NASA/NumericalData/MAVEN/STATIC/Level2/Distributions/APIDda/PT4S)
Description
STATIC>Supra-Thermal And Thermal Ion Composition Particle Distributions
Modification History
Rev-1 2014-04-28
 
  • Data Variable Descriptions
      Data for selected rate channel by energy step [rates]
      Rate data for the rate channels sorted by energy step with dimension (NUM_DISTS,
      NRATE, NENERGY) units=counts/s
      
      Rate Channel selected (0-11) [rate_channel]
      
      
      Quality flag [quality_flag]
      Quality flag (NUM_DISTS elements)
      
      ---> Validity flag codes valid data (bit 0), test pulser on (bit 1), diag mode (bit 2), data comp type (bit 3-4), packet compn (bit 5) [valid]
      ---> Validity flag codes valid data (bit 0), test pulser on (bit 1), diagnostic
      mode (bit 2), data compression type (bit 3-4), packet compression (bit 5)
      (NUM_DISTS elements)
      
      ---> Decoded mode number [mode]
      ---> Decoded mode number. (NUM_DISTS elements)
      
      Decoded telemetry rate number [rate]
      Decoded telemetry rate number. (NUM_DISTS elements)
      
      ---> Index that identifies the energy and deflector sweep look up tables (LUT) for the sensor [swp_ind]
      ---> Index that identifies the energy and deflector sweep look up tables (LUT)
      for the sensor. SWP_IND is an index that selects the following support data
      arrays: ENERGY, DENERGY, THETA, DTHETA, PHI, DPHI, DOMEGA, GF and MASS_ARR.
      (NUM_DISTS elements), EN_IND Le NSWP
      
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MVN_SWE_L2_ARC3D (spase://NASA/NumericalData/MAVEN/SWEA/Level2/Distributions3D/Archive/PT8S)
Description
MAVEN SWEA 3D Distributions
Modification History
Revision 0
 
  • Data Variable Descriptions
      Energy binning factor: 1 = 64 energies, 2 = 32 energies, 4 = 16 energies [binning]
      
      
      [no-plot for now]Raw instrument counts [counts]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and azimuth angle] at 1st Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes]
      
      
      Variance of differential energy flux (unavailable before 2014/11/15) [variance]
      
      
      Secondary electron contamination (unavailable before 2014/11/15) [secondary]
      
      
      ---> Movie of above [flux vs. energy and azimuth angle] [diff_en_fluxes_mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec1]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and azimuth angle] at 2nd Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_2]
      
      
      ---> Movie of above [flux vs. energy and azimuth angle] [diff_en_fluxes_2mv]
      
      
      ---> Spectrogram at Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec2]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and azimuth angle] at 3rd Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_3]
      
      
      ---> Movie of above [flux vs. energy and azimuth angle] [diff_en_fluxes_3mv]
      
      
      ---> Spectrogram at Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec3]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and azimuth angle] at 4th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_4]
      
      
      ---> Movie of above [flux vs. energy and azimuth angle] [diff_en_fluxes_4mv]
      
      
      ---> Spectrogram at Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec4]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and azimuth angle] at 5th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_5]
      
      
      ---> Movie of above [flux vs. energy and azimuth angle] [diff_en_fluxes_5mv]
      
      
      ---> Spectrogram at Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec5]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and azimuth angle] at 6th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_6]
      
      
      ---> Movie of above [flux vs. energy and azimuth angle] [diff_en_fluxes_6mv]
      
      
      ---> Spectrogram at Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec6]
      
      
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MVN_SWE_L2_ARCPAD (spase://NASA/NumericalData/MAVEN/SWEA/Level2/PitchAngleDistributions/Archive/PT2S)
Description
MAVEN SWEA Pitch Angle Distributions
Modification History
Revision 0
 
  • Data Variable Descriptions
      Raw Instrument Counts (energy vs pitch angle index) [counts]
      
      
      ---> Counts (movie: energy vs pitch angle index) [counts_movie]
      
      
      Calibrated differential energy flux (energy vs pitch angles for 158eV) [diff_en_fluxes]
      
      
      Variance of differential energy flux (unavailable before 2014/11/16) [variance]
      
      
      Secondary electron contamination (unavailable before 2014/11/16) [secondary]
      
      
      ---> Flux (movie: energy vs pitch angles for 158eV) [diff_en_fluxes_movie]
      
      
      ---> Flux (spectrogram in PA at 4630 eV) [diff_en_fluxes_byPA_atE01]
      
      
      ---> Flux (spectrogram in PA at 1620 eV) [diff_en_fluxes_byPA_atE11]
      
      
      ---> Flux (spectrogram in PA at 506 eV) [diff_en_fluxes_byPA_atE21]
      
      
      ---> Flux (spectrogram in PA at 158 eV) [diff_en_fluxes_byPA_atE31]
      
      
      ---> Flux (spectrogram in PA at 49 eV) [diff_en_fluxes_byPA_atE41]
      
      
      ---> Flux (spectrogram in PA at 15 eV) [diff_en_fluxes_byPA_atE51]
      
      
      ---> Flux (spectrogram in PA at 5 eV) [diff_en_fluxes_byPA_atE61]
      
      
      Pitch Angles (energy vs angle index) [pa]
      
      
      ---> Pitch Angles (movie: energy vs angle index) [pa_movie]
      
      
      ---> Median Pitch Angles (values at 158 eV) [pa_E31]
      
      
      Magnetic field azimuth in instrument coordiantes [b_azim]
      
      
      Magnetic field elevation in instrument coordiantes [b_elev]
      
      
      Energy binning factor: 1 = 64 energies, 2 = 32 energies, 4 = 16 energies [binning]
      
      
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MVN_SWE_L2_SVY3D (spase://NASA/NumericalData/MAVEN/SWEA/Level2/Distributions3D/Survey/PT16S)
Description
MAVEN SWEA 3D Distributions
Modification History
Revision 0
 
  • Data Variable Descriptions
      Time, center of sample, in raw mission elapsed time [time_met]
      
      
      Energy binning factor: 1 = 64 energies, 2 = 32 energies, 4 = 16 energies [binning]
      
      
      [no-plot]Raw Instrument Counts [counts]
      
      
      Calibrated differential energy flux [vary with time, energy, deflection index and azimuth angle] at 1st Deflection Index [Thumbnails, select a few hours] [diff_en_fluxes]
      
      
      Variance of differential energy flux (unavailable before 2014/11/15) [variance]
      
      
      Secondary electron contamination (unavailable before 2014/11/15) [secondary]
      
      
      ---> Movie of above [flux vs. energy and azimuth angle] [diff_en_fluxes_mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec1]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and azimuth angle] at 2nd Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_2]
      
      
      ---> Movie of above [flux vs. energy and azimuth angle] [diff_en_fluxes_2mv]
      
      
      ---> Spectrogram at Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec2]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and azimuth angle] at 3rd Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_3]
      
      
      ---> Movie of above [flux vs. energy and azimuth angle] [diff_en_fluxes_3mv]
      
      
      ---> Spectrogram at Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec3]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and azimuth angle] at 4th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_4]
      
      
      ---> Movie of above [flux vs. energy and azimuth angle] [diff_en_fluxes_4mv]
      
      
      ---> Spectrogram at Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec4]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and azimuth angle] at 5th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_5]
      
      
      ---> Movie of above [flux vs. energy and azimuth angle] [diff_en_fluxes_5mv]
      
      
      ---> Spectrogram at Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec5]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and azimuth angle] at 6th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_6]
      
      
      ---> Movie of above [flux vs. energy and azimuth angle] [diff_en_fluxes_6mv]
      
      
      ---> Spectrogram at Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec6]
      
      
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MVN_SWE_L2_SVYPAD (spase://NASA/NumericalData/MAVEN/SWEA/Level2/PitchAngleDistributions/Survey/PT2S)
Description
MAVEN SWEA Pitch Angle Distributions
Modification History
Revision 0
 
  • Data Variable Descriptions
      Raw instrument counts (energy vs pitch angle index) [counts]
      
      
      ---> Counts (movie: energy vs pitch angle index) [counts_movie]
      
      
      Calibrated differential energy flux (energy vs pitch angles for 158eV) [diff_en_fluxes]
      
      
      Variance of differential energy flux (unavailable before 2014/11/15) [variance]
      
      
      Secondary electron contamination (unavailable before 2014/11/15) [secondary]
      
      
      ---> Flux (movie: energy vs pitch angles for 158eV) [diff_en_fluxes_movie]
      
      
      Flux (spectrogram in PA at 4630 eV) [diff_en_fluxes_byPA_atE01]
      
      
      ---> Flux (spectrogram in PA at 1620 eV) [diff_en_fluxes_byPA_atE11]
      
      
      ---> Flux (spectrogram in PA at 506 eV) [diff_en_fluxes_byPA_atE21]
      
      
      ---> Flux (spectrogram in PA at 158 eV) [diff_en_fluxes_byPA_atE31]
      
      
      ---> Flux (spectrogram in PA at 49 eV) [diff_en_fluxes_byPA_atE41]
      
      
      ---> Flux (spectrogram in PA at 15 eV) [diff_en_fluxes_byPA_atE51]
      
      
      ---> Flux (spectrogram in PA at 5 eV) [diff_en_fluxes_byPA_atE61]
      
      
      Pitch angles (energy vs angle index) [pa]
      
      
      ---> Pitch angles (movie: energy vs angle index) [pa_movie]
      
      
      Median pitch angles (values at 158 eV) [pa_E31]
      
      
      Magnetic field azimuth in instrument coordiantes [b_azim]
      
      
      Magnetic field elevation in instrument coordiantes [b_elev]
      
      
      Energy binning factor: 1 = 64 energies, 2 = 32 energies, 4 = 16 energies [binning]
      
      
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MVN_SWE_L2_SVYSPEC (spase://NASA/NumericalData/MAVEN/SWEA/Level2/EnergySpectra/Survey/PT2S)
Description
MAVEN SWEA Energy Spectra
Modification History
Revision 0
 
  • Data Variable Descriptions
      Raw instrument counts [counts]
      
      
      ---> Raw instrument counts (as separate time series) [counts_time]
      
      
      Calibrated differential energy flux (as spectrogram) [diff_en_fluxes]
      
      
      Variance of differential energy flux (unavailable before 2014/11/15) [variance]
      
      
      Secondary electron contamination (unavailable before 2014/11/15) [secondary]
      
      
      ---> Calibrated differential energy flux (as overlaid time series) [diff_en_fluxes_stack]
      
      
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MVN_SWI_L2_COARSEARC3D (spase://NASA/NumericalData/MAVEN/SWIA/Level2/Distributions3D/Coarse/Archive/PT8S)
Description
MAVEN SWIA Coarse 3d Distributions
Modification History
Revision 0
 
  • Data Variable Descriptions
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 1st deflection index [Thumnails, select a few hours] [diff_en_fluxes]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_mv]
      
      
      ---> Spectrogram at selected anode angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec1]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection and anode angles] at 2nd deflection index[Thumbnails, select a few hours] [diff_en_fluxes_2]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_2mv]
      
      
      ---> Spectrogram at selected anode angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec2]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection and anode angles] at 3rd deflection index[Thumbnails, select a few hours] [diff_en_fluxes_3]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_3mv]
      
      
      ---> Spectrogram at selected anode angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec3]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection and anode angles] at 4th deflection index[Thumbnails, select a few hours] [diff_en_fluxes_4]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_4mv]
      
      
      ---> Spectrogram at selected anode angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec4]
      
      
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MVN_SWI_L2_COARSESVY3D (spase://NASA/NumericalData/MAVEN/SWIA/Level2/Distributions3D/Coarse/Survey/PT8S)
Description
MAVEN SWIA Coarse 3d Distributions
Modification History
Revision 0
 
  • Data Variable Descriptions
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 1st deflection index[Thumbnails, select a few hours] [diff_en_fluxes]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec1]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 2nd deflection index[Thumbnails, select a few hours] [diff_en_fluxes_2]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_2mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec2]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 3rd deflection index[Thumbnails, select a few hours] [diff_en_fluxes_3]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_3mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec3]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 4th deflection index[Thumbnails, select a few hours] [diff_en_fluxes_4]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_4mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec4]
      
      
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MVN_SWI_L2_FINEARC3D (spase://NASA/NumericalData/MAVEN/SWIA/Level2/Distributions3D/Fine/Archive/PT8S)
Description
MAVEN SWIA Fine 3d Distributions
Modification History
Revision 0
 
  • Data Variable Descriptions
      Attenuator state, 1 = open, 2 = closed, 3 = cover closed [atten_state]
      
      
      Starting Energy Step [estep_first]
      
      
      Starting Deflection Step [dstep_first]
      
      
      [no-plot for now]Raw Instrument counts [counts]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 1st Deflection Index [Thumbnails, select a few hours] [diff_en_fluxes]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_mv]
      
      
      ---> Spectrogram at selected Anode Angle bins 1,4,7,10 [diff_en_fluxes_spec1]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 2nd Deflection Index [Thumbnails, select a few hours] [diff_en_fluxes_2]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_2mv]
      
      
      ---> Spectrogram at selected Anode Angle bins 1,4,7,10 [diff_en_fluxes_spec2]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 3rd Deflection Index [Thumbnails, select a few hours] [diff_en_fluxes_3]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_3mv]
      
      
      ---> Spectrogram at selected Anode Angle bins 1,4,7,10 [diff_en_fluxes_spec3]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 4th Deflection Index [Thumbnails, select a few hours] [diff_en_fluxes_4]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_4mv]
      
      
      ---> Spectrogram at selected Anode Angle bins 1,4,7,10 [diff_en_fluxes_spec4]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 5th Deflection Index [Thumbnails, select a few hours] [diff_en_fluxes_5]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_5mv]
      
      
      ---> Spectrogram at selected Anode Angle bins 1,4,7,10 [diff_en_fluxes_spec5]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 6th Deflection Index [Thumbnails, select a few hours] [diff_en_fluxes_6]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_6mv]
      
      
      ---> Spectrogram at selected Anode Angle bins 1,4,7,10,13,16 [diff_en_fluxes_spec6]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 2nd Deflection Index [Thumbnails, select a few hours] [diff_en_fluxes_7]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_7mv]
      
      
      ---> Spectrogram at selected Anode Angle bins 1,4,7,10 [diff_en_fluxes_spec7]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 8th Deflection Index [Thumbnails, select a few hours] [diff_en_fluxes_8]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_8mv]
      
      
      ---> Spectrogram at selected Anode Angle bins 1,4,7,10 [diff_en_fluxes_spec8]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 9th Deflection Index [Thumbnails, select a few hours] [diff_en_fluxes_9]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_9mv]
      
      
      ---> Spectrogram at selected Anode Angle bins 1,4,7,10 [diff_en_fluxes_spec9]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 10th Deflection Index [Thumbnails, select a few hours] [diff_en_fluxes_10]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_10mv]
      
      
      ---> Spectrogram at selected Anode Angle bins 1,4,7,10 [diff_en_fluxes_spec10]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 11th Deflection Index [Thumbnails, select a few hours] [diff_en_fluxes_11]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_11mv]
      
      
      ---> Spectrogram at selected Anode Angle bins 1,4,7,10 [diff_en_fluxes_spec11]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 12th Deflection Index [Thumbnails, select a few hours] [diff_en_fluxes_12]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_12mv]
      
      
      ---> Spectrogram at selected Anode Angle bins 1,4,7,10 [diff_en_fluxes_spec12]
      
      
      Fine Anode Angle (Phi) Table [phi_fine]
      
      
      Energy Index for CDF compatibility [eindex]
      
      
      Deflection Index for CDF compatibility [dindex]
      
      
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MVN_SWI_L2_FINESVY3D (spase://NASA/NumericalData/MAVEN/SWIA/Level2/Distributions3D/Fine/Survey/PT8S)
Description
MAVEN SWIA Fine 3d Distributions
Modification History
Revision 0
 
  • Data Variable Descriptions
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 1st Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10 [diff_en_fluxes_spec1]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 2nd Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_2]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_2mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10 [diff_en_fluxes_spec2]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 3rd Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_3]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_3mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10 [diff_en_fluxes_spec3]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 4th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_4]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_4mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10 [diff_en_fluxes_spec4]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 5th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_5]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_5mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10 [diff_en_fluxes_spec5]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 6th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_6]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_6mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10 [diff_en_fluxes_spec6]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 7th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_7]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_7mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10 [diff_en_fluxes_spec7]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 8th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_8]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_8mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10 [diff_en_fluxes_spec8]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 9th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_9]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_9mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10 [diff_en_fluxes_spec9]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 10th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_10]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_10mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10 [diff_en_fluxes_spec10]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 11th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_11]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_11mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10 [diff_en_fluxes_spec11]
      
      
      Calibrated Differential Energy Flux [vary with time, energy, deflection index and anode angle] at 12th Deflection Index[Thumbnails, select a few hours] [diff_en_fluxes_12]
      
      
      ---> Movie of above [flux vs. energy and anode angle] [diff_en_fluxes_12mv]
      
      
      ---> Spectrogram at selected Azimuth Angle bins 1,4,7,10 [diff_en_fluxes_spec12]
      
      
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MVN_SWI_L2_ONBOARDSVYMOM (spase://NASA/NumericalData/MAVEN/SWIA/Level2/OnboardMoments/Survey/PT4S)
Description
MAVEN SWIA Onboard Moments
Modification History
Revision 0
 
  • Data Variable Descriptions
      Onboard density moment, assuming 100% protons [density]
      
      
      Onboard pressure moment (Inst. Coords), assuming 100% protons [pressure]
      
      
      Onboard velocity moment (Inst. Coords), assuming 100% protons [velocity]
      
      
      Onboard velocity moment (MSO [Mars-Sun Orbit] Coords), assuming 100% protons [velocity_mso]
      
      
      Onboard temperature moment (Inst. Coords), assuming 100% protons [temperature]
      
      
      Onboard temperature moment (MSO [Mars-Sun Orbit] Coords), assuming 100% protons [temperature_mso]
      
      
      Attenuator state, 1 = open, 2 = closed, 3 = cover closed [atten_state]
      
      
      Telemetry Mode: 1 = Sheath, 0 = Solar Wind [telem_mode]
      
      
      Quality Flag: 0 = bad, 1 = good [quality_flag]
      
      
      Decommutation Flag: 0 = uncertain mode/attenuator flags, 1 = known mode/attenuator flags [decom_flag]
      
      
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MVN_SWI_L2_ONBOARDSVYSPEC (spase://NASA/NumericalData/MAVEN/SWIA/Level2/EnergySpectra/Survey/PT4S)
Description
MAVEN SWIA Onboard Energy Spectra
Modification History
Revision 0
 
  • Data Variable Descriptions
      Raw Instrument Counts (as spectrogram) [spectra_counts]
      
      
      ---> Raw Instrument Counts (as time series). [spectra_counts_time]
      
      
      Calibrated differential energy flux (as spectrogram) [spectra_diff_en_fluxes]
      
      
      ---> Calibrated differential energy flux (as overlaid time series) [spectra_diff_en_fluxes_stack]
      
      
      Attenuator state, 1 = open, 2 = closed, 3 = cover closed [atten_state]
      
      
      Number of Accumulations Summed [num_accum]
      
      
      Decommutation Flag: 0 = uncertain mode/attenuator flags, 1 = known mode/attenuator flags [decom_flag]
      
      
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