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CDAWeb Served Heliophysics Datasets Beginning with 'R'

RBSP-A-RBSPICE_LEV-2_ESRHELT: RBSP_H0_RBSPICE_ESR_HELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-2_ESRLEHT: RBSP_H0_RBSPICE_ESR_LEHT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-2_ISRHELT: RBSP_H0_RBSPICE_ISR_HELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-2_TOFXEH: RBSP_H0_RBSPICE_TOFxE_H - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-2_TOFXEION: RBSP_H0_RBSPICE_TOFxE_Ion - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-2_TOFXENONH: RBSP_H0_RBSPICE_TOFxE_nonH - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-2_TOFXPHHHELT: RBSP_H0_RBSPICE_TOFxPH_H_HELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-2_TOFXPHHLEHT: RBSP_H0_RBSPICE_TOFxPH_H_HELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3-PAP_ESRHELT: rbsp-a-rbspice_level_3_esrhelt - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3-PAP_ESRLEHT: rbsp-a-rbspice_level_3_esrleht - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3-PAP_TOFXEH: rbsp-a-rbspice_level_3_tofxeh - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3-PAP_TOFXEHE: rbsp-a-rbspice_level_3_tofxenonh - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3-PAP_TOFXEHE-0: rbsp-a-rbspice_level_3_tofxenonh - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3-PAP_TOFXEION: rbsp-a-rbspice_level_3_tofxeion - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3-PAP_TOFXEO: rbsp-a-rbspice_level_3_tofxenonh - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3-PAP_TOFXEO-0: rbsp-a-rbspice_level_3_tofxenonh - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3-PAP_TOFXPHHHELT: rbsp-a-rbspice_level_3_tofxphhhelt - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3-PAP_TOFXPHHLEHT: rbsp-a-rbspice_level_3_tofxphhleht - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3-PAP_TOFXPHOHELT: rbsp-a-rbspice_level_3_tofxphhhelt - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3-PAP_TOFXPHOLEHT: rbsp-a-rbspice_level_3_tofxphhleht - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3_ESRHELT: rbsp-a-rbspice_level_3_ESRHELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3_ESRLEHT: rbsp-a-rbspice_level_3_ESRLEHT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3_ISRHELT: rbsp-a-rbspice_level_3_ISRHELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3_TOFXEH: rbsp-a-rbspice_level_3_TOFXEH - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3_TOFXEION: rbsp-a-rbspice_level_3_TOFXEION - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3_TOFXENONH: rbsp-a-rbspice_level_3_TOFXENONH - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3_TOFXPHHHELT: rbsp-a-rbspice_level_3_TOFXPHHHELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A-RBSPICE_LEV-3_TOFXPHHLEHT: rbsp-a-rbspice_level_3_TOFXPHHLEHT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-A_DENSITY_EMFISIS-L4: Density and other parameters inferred by digitizing the trace on the spectrograms. - Craig Kletzing (University of Iowa)
RBSP-A_HFR-SPECTRA-BURST_EMFISIS-L2: Single Axis AC Electric Field Spectra - Craig Kletzing (University of Iowa)
RBSP-A_HFR-SPECTRA-MERGED_EMFISIS-L2: Single Axis AC Electric Field Spectra - Craig Kletzing (University of Iowa)
RBSP-A_HFR-SPECTRA_EMFISIS-L2: Single Axis AC Electric Field Spectra - Craig Kletzing (University of Iowa)
RBSP-A_HFR-WAVEFORM_EMFISIS-L2: High Frequency Receiver Waveform - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_1SEC-GEI_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_1SEC-GEO_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_1SEC-GSE_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_1SEC-GSM_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_1SEC-SM_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_4SEC-GEI_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_4SEC-GEO_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_4SEC-GSE_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_4SEC-GSM_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_4SEC-SM_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_HIRES-GEI_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_HIRES-GEO_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_HIRES-GSE_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_HIRES-GSM_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_HIRES-SM_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_MAGNETOMETER_UVW_EMFISIS-L2: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-A_WFR-SPECTRAL-MATRIX-DIAGONAL-MERGED_EMFISIS-L2: WFR Spectral Matrix - Craig Kletzing (University of Iowa)
RBSP-A_WFR-SPECTRAL-MATRIX-DIAGONAL_EMFISIS-L2: WFR Spectral Matrix - Craig Kletzing (University of Iowa)
RBSP-A_WFR-SPECTRAL-MATRIX_EMFISIS-L2: WFR Spectral Matrix - Craig Kletzing (University of Iowa)
RBSP-A_WFR-WAVEFORM-CONTINUOUS-BURST_EMFISIS-L2: WFR Spectral Matrix - Craig Kletzing (University of Iowa)
RBSP-A_WFR-WAVEFORM_EMFISIS-L2: WFR Spectral Matrix - Craig Kletzing (University of Iowa)
RBSP-A_WNA-SURVEY-SHEATH-CORRECTED-E_EMFISIS-L4: Probes-A EMFISIS wave normal angle products and sheath corrected electric field level Level-4 - Craig Kletzing (University of Iowa)
RBSP-B-RBSPICE_LEV-2_ESRHELT: RBSP_H0_RBSPICE_ESR_HELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-2_ESRLEHT: RBSP_H0_RBSPICE_ESR_LEHT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-2_ISRHELT: RBSP_H0_RBSPICE_ISR_HELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-2_TOFXEH: RBSP_H0_RBSPICE_TOFxE_H - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-2_TOFXEION: RBSP_H0_RBSPICE_TOFxE_Ion - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-2_TOFXENONH: RBSP_H0_RBSPICE_TOFxE_nonH - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-2_TOFXPHHHELT: RBSP_H0_RBSPICE_TOFxPH_H_HELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-2_TOFXPHHLEHT: RBSP_H0_RBSPICE_TOFxPH_H_HELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3-PAP_ESRHELT: rbsp-b-rbspice_level_3_esrhelt - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3-PAP_ESRLEHT: rbsp-b-rbspice_level_3_esrleht - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3-PAP_TOFXEH: rbsp-b-rbspice_level_3_tofxeh - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3-PAP_TOFXEHE: rbsp-b-rbspice_level_3_tofxenonh - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3-PAP_TOFXEHE-0: rbsp-b-rbspice_level_3_tofxenonh - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3-PAP_TOFXEION: rbsp-b-rbspice_level_3_tofxeion - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3-PAP_TOFXEO: rbsp-b-rbspice_level_3_tofxenonh - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3-PAP_TOFXEO-0: rbsp-b-rbspice_level_3_tofxenonh - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3-PAP_TOFXPHHHELT: rbsp-b-rbspice_level_3_tofxphhhelt - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3-PAP_TOFXPHHLEHT: rbsp-b-rbspice_level_3_tofxphhleht - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3-PAP_TOFXPHOHELT: rbsp-b-rbspice_level_3_tofxphhhelt - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3-PAP_TOFXPHOLEHT: rbsp-b-rbspice_level_3_tofxphhleht - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3_ESRHELT: rbsp-b-rbspice_level_3_ESRHELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3_ESRLEHT: rbsp-b-rbspice_level_3_ESRLEHT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3_ISRHELT: rbsp-b-rbspice_level_3_ISRHELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3_TOFXEH: rbsp-b-rbspice_level_3_TOFXEH - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3_TOFXEION: rbsp-b-rbspice_level_3_TOFXEION - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3_TOFXENONH: rbsp-b-rbspice_level_3_TOFXENONH - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3_TOFXPHHHELT: rbsp-b-rbspice_level_3_TOFXPHHHELT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B-RBSPICE_LEV-3_TOFXPHHLEHT: rbsp-b-rbspice_level_3_TOFXPHHLEHT - Lou Lanzerotti (New Jersey Institute of Technology)
RBSP-B_DENSITY_EMFISIS-L4: Density and other parameters inferred by digitizing the trace on the spectrograms. - Craig Kletzing (University of Iowa)
RBSP-B_HFR-SPECTRA-BURST_EMFISIS-L2: Single Axis AC Electric Field Spectra - Craig Kletzing (University of Iowa)
RBSP-B_HFR-SPECTRA-MERGED_EMFISIS-L2: Single Axis AC Electric Field Spectra - Craig Kletzing (University of Iowa)
RBSP-B_HFR-SPECTRA_EMFISIS-L2: Single Axis AC Electric Field Spectra - Craig Kletzing (University of Iowa)
RBSP-B_HFR-WAVEFORM_EMFISIS-L2: High Frequency Receiver Waveform - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_1SEC-GEI_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_1SEC-GEO_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_1SEC-GSE_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_1SEC-GSM_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_1SEC-SM_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_4SEC-GEI_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_4SEC-GEO_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_4SEC-GSE_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_4SEC-GSM_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_4SEC-SM_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_HIRES-GEI_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_HIRES-GEO_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_HIRES-GSE_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_HIRES-GSM_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_HIRES-SM_EMFISIS-L3: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_MAGNETOMETER_UVW_EMFISIS-L2: Fluxgate Magnetometer data - Craig Kletzing (University of Iowa)
RBSP-B_WFR-SPECTRAL-MATRIX-DIAGONAL-MERGED_EMFISIS-L2: WFR Spectral Matrix - Craig Kletzing (University of Iowa)
RBSP-B_WFR-SPECTRAL-MATRIX-DIAGONAL_EMFISIS-L2: WFR Spectral Matrix - Craig Kletzing (University of Iowa)
RBSP-B_WFR-SPECTRAL-MATRIX_EMFISIS-L2: WFR Spectral Matrix - Craig Kletzing (University of Iowa)
RBSP-B_WFR-WAVEFORM-CONTINUOUS-BURST_EMFISIS-L2: WFR Spectral Matrix - Craig Kletzing (University of Iowa)
RBSP-B_WFR-WAVEFORM_EMFISIS-L2: WFR Spectral Matrix - Craig Kletzing (University of Iowa)
RBSP-B_WNA-SURVEY-SHEATH-CORRECTED-E_EMFISIS-L4: Probes-B EMFISIS wave normal angle products and sheath corrected electric field Level-4 - Craig Kletzing (University of Iowa)
RBSPA_EFW-L2_E-HIRES-UVW: DERIVED FROM: Reference for Spin Axis Vector in GSE - J. R. Wygant (University of Minnesota)
RBSPA_EFW-L2_E-SPINFIT-MGSE: DERIVED FROM: Spinfit DC Electric Field estimates in M-GSE coordinates - J. R. Wygant (University of Minnesota)
RBSPA_EFW-L2_ESVY_DESPUN: DERIVED FROM: Spinfit DC Electric Field estimates in M-GSE coordinates - J. R. Wygant (University of Minnesota)
RBSPA_EFW-L2_FBK: Filterbank data product from RBSP-EFW - J. R. Wygant (University of Minnesota)
RBSPA_EFW-L2_SPEC: Spectral data product from RBSP-EFW - J. R. Wygant (University of Minnesota)
RBSPA_EFW-L2_VSVY-HIRES: Single-ended potential values for boom 1-6 - J. R. Wygant (University of Minnesota)
RBSPA_EFW_BURST-WAVEFORM-UVW-L1: Burst Mode 1 (512 samples/sec) Electric and Magnetic Fields - J. R. Wygant
RBSPA_L2-1MIN_PSBR-RPS: Van Allen Probes/RPS Level 2 1-Minute Data - J. Mazur (The Aerospace Corporation)
RBSPA_L2_PSBR-RPS: Van Allen Probes/RPS Level 2 Data - J. Mazur (The Aerospace Corporation)
RBSPA_REL03_ECT-MAGEIS-L2: rbsp-a_ect-mageis-l2_pre - J. Bernard Blake (JBernard.Blake@aero.org) (The Aerospace Corporation)
RBSPA_REL03_ECT-REPT-SCI-L2: rbspa>Level 2 data for the REPT instrument - D. Baker (University of Colorado at Boulder)
RBSPA_REL03_ECT-REPT-SCI-L3: RBSP/ECT REPT Pitch Angle Resolved Electron and Proton Fluxes. Electron energies: 1.8 - 20 MeV. Proton energies: 21.25 - 4.74961e-316 MeV - D. Baker (University of Colorado at Boulder)
RBSPA_REL04_ECT-HOPE-MOM-L3: Spin resolved HOPE science data. Electrons and protons measured in alternate spin cadence. - Herbert Funsten (Los Alamos National Laboratory)
RBSPA_REL04_ECT-HOPE-PA-L3: Pitch angle resolved HOPE science data. Electrons and protons measured in alternate spin cadence. - Herbert Funsten (Los Alamos National Laboratory)
RBSPA_REL04_ECT-HOPE-SCI-L2: Spin resolved HOPE science data. Electrons and protons measured in alternate spin cadence. - Herbert Funsten (Los Alamos National Laboratory)
RBSPA_REL04_ECT-HOPE-SCI-L2SA: Spin averaged HOPE science data. Electrons and protons measured in alternate spin cadence. - Herbert Funsten (Los Alamos National Laboratory)
RBSPA_REL04_ECT-MAGEIS-L3: 14 - J. Bernard Blake (JBernard.Blake@aero.org) (The Aerospace Corporation)
RBSPB_EFW-L2_E-HIRES-UVW: DERIVED FROM: Reference for Spin Axis Vector in GSE - J. R. Wygant (University of Minnesota)
RBSPB_EFW-L2_E-SPINFIT-MGSE: DERIVED FROM: Spinfit DC Electric Field estimates in M-GSE coordinates - J. R. Wygant (University of Minnesota)
RBSPB_EFW-L2_ESVY_DESPUN: DERIVED FROM: Spinfit DC Electric Field estimates in M-GSE coordinates - J. R. Wygant (University of Minnesota)
RBSPB_EFW-L2_FBK: Filterbank data product from RBSP-EFW - J. R. Wygant (University of Minnesota)
RBSPB_EFW-L2_SPEC: Spectral data product from RBSP-EFW - J. R. Wygant (University of Minnesota)
RBSPB_EFW-L2_VSVY-HIRES: Single-ended potential values for boom 1-6 - J. R. Wygant (University of Minnesota)
RBSPB_EFW_BURST-WAVEFORM-UVW-L1: Burst Mode 1 (512 samples/sec) Electric and Magnetic Fields - J. R. Wygant
RBSPB_L2-1MIN_PSBR-RPS: Van Allen Probes/RPS Level 2 1-Minute Data - J. Mazur (The Aerospace Corporation)
RBSPB_L2_PSBR-RPS: Van Allen Probes/RPS Level 2 Data - J. Mazur (The Aerospace Corporation)
RBSPB_REL03_ECT-MAGEIS-L2: rbsp-a_ect-mageis-l2_pre - J. Bernard Blake (JBernard.Blake@aero.org) (The Aerospace Corporation)
RBSPB_REL03_ECT-REPT-SCI-L2: rbspb>Level 2 data for the REPT instrument - D. Baker (University of Colorado at Boulder)
RBSPB_REL03_ECT-REPT-SCI-L3: RBSP/ECT REPT Pitch Angle Resolved Electron and Proton Fluxes. Electron energies: 1.8 - 20 MeV. Proton energies: 21.25 - 4.94066e-324 MeV - D. Baker (University of Colorado at Boulder)
RBSPB_REL04_ECT-HOPE-MOM-L3: Spin resolved HOPE science data. Electrons and protons measured in alternate spin cadence. - Herbert Funsten (Los Alamos National Laboratory)
RBSPB_REL04_ECT-HOPE-PA-L3: Pitch angle resolved HOPE science data. Electrons and protons measured in alternate spin cadence. - Herbert Funsten (Los Alamos National Laboratory)
RBSPB_REL04_ECT-HOPE-SCI-L2: Spin resolved HOPE science data. Electrons and protons measured in alternate spin cadence. - Herbert Funsten (Los Alamos National Laboratory)
RBSPB_REL04_ECT-HOPE-SCI-L2SA: Spin averaged HOPE science data. Electrons and protons measured in alternate spin cadence. - Herbert Funsten (Los Alamos National Laboratory)
RBSPB_REL04_ECT-MAGEIS-L3: 16 - J. Bernard Blake (JBernard.Blake@aero.org) (The Aerospace Corporation)
RBSP_ECT-REPT-SCI-L3-SELESNICK-MODEL: RBSP/ECT REPT Monthly Intensities as a function of Energy, Pitch Angle and L-shell from the Selesnick model - D. Baker (University of Colorado at Boulder)
REACH-VID-101_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 101 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-102_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 102 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-105_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 105 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-108_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 108 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-113_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 113 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-114_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 114 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-115_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 115 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-116_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 116 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-133_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 133 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-134_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 134 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-135_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 135 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-136_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 136 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-137_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 137 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-138_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 138 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-139_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 139 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-140_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 140 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-148_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 148 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-149_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 149 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-162_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 162 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-163_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 163 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-164_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 164 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-165_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 165 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-166_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 166 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-169_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 169 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-170_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 170 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-171_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 171 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-172_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 172 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-173_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 173 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-175_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 175 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-176_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 176 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-180_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 180 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
REACH-VID-181_DOSIMETER-L1C: Dosimeter measurements from the Responsive Environmental Assessment Commerically Hosted satellite 181 - Joe Mazur (joseph.e.mazur@aero.org) (The Aerospace Corporation)
RENU2_H0_EFIELD: H0 - RENU2 COWBOY Electric Field. - Marc Lessard, David Hysell (University of New Hampshire, Cornell University)
RENU2_H0_EPLAS: H0 - RENU2 EPLAS Electron Flux. - Marc Lessard (University of New Hampshire)
RENU2_H0_ERPAMAIN: H0 - RENU2 ERPA Thermal Electrons. - Marc Lessard (University of New Hampshire)
RENU2_H0_ERPASUB: H0 - RENU2 ERPA Thermal Electrons. - Marc Lessard (University of New Hampshire)
RENU2_H0_FGM: H0 - RENU2 Magnetic Field. - Marc Lessard (University of New Hampshire, Cornell University)
RENU2_H0_IG2: H0 - RENU2 ionization gauge - James Clemmons (University of New Hampshire)
RENU2_H0_PMT: H0 - RENU2 PMT Rayleighs. - Jim Hecht (University of New HampshireAerospace Corporation)
RENU2_H0_UVPMT: H0 - RENU2 UV PMT Counts. - Marc Lessard (University of New Hampshire)
RENU2_H0_VLF: H0 - RENU2 COWBOY Electric Field. - Marc Lessard, David Hysell (University of New Hampshire, Cornell University)
ROSETTA_HELIO1DAY_POSITION: Position in heliocentric coordinates from SPDF Helioweb - Natalia Papitashvili (NASA/GSFC/SPDF)
RS_K0_IPEI: ROCSAT-1(FORMOSAT-1)/IPEI, Key Parameters - Shin-Yi Su (Institution of Space Science, National Central University, Taiwan, R.O.C.)

RBSP-A-RBSPICE_LEV-2_ESRHELT doi:tbd
Proper citations should include the "Accessed on date" in the form .
Description
RBSP RBSPICE High Energy Resolution Electron Rates converted into units of
physical intensity (counts/(s*sr*cm^2*MeV) measured at high energy resolution
and low time resolution.
For more information regarding this data and the
RBSPICE science goals and mission statement see the RBSPICE team web site at:
http:// rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-2_ESRLEHT doi:tbd
Proper citations should include the "Accessed on date" in the form .
Description
RBSP RBSPICE Low Energy Resolution Electron Rates converted into units of
physical intensity (counts/(s*sr*cm^2*MeV) measured at high energy resolution
and low time resolution.
For more information regarding this data and the
RBSPICE science goals and mission statement see the RBSPICE team web site at:
http:// rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-2_ISRHELT doi:tbd
Proper citations should include the "Accessed on date" in the form .
Description
RBSP RBSPICE high energy resolution Ion Species Rates (ISRHELT) converted into
units of physical intensity (counts/(s*sr*cm^2*MeV) measured at high energy
resolution and low time resolution.
For more information regarding this data and
the RBSPICE science goals and mission statement see the RBSPICE team web site
at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-2_TOFXEH doi:tbd
Proper citations should include the "Accessed on date" in the form .
Description
RBSP RBSPICE TOF x Energy Hydrogen Rates converted into units of physical
intensity (counts/(s*sr*cm^2*MeV) measured at high energy resolution and low
time resolution.
For more information regarding this data and the RBSPICE
science goals and mission statement see the RBSPICE team web site at: http:// 
rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-2_TOFXEION doi:tbd
Proper citations should include the "Accessed on date" in the form .
Description
RBSP RBSPICE TOF x Energy Ion Rates converted into units of physical intensity
(counts/(s*sr*cm^2*MeV) measured at high energy resolution and low time
resolution.
For more information regarding this data and the RBSPICE science
goals and mission statement see the RBSPICE team web site at: http:// 
rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-2_TOFXENONH doi:tbd
Proper citations should include the "Accessed on date" in the form .
Description
RBSP RBSPICE TOF x E non Hydrogen (Helium and Oxygen) Rates converted into units
of physical intensity (counts/(s*sr*cm^2*MeV) measured at high energy resolution
and low time resolution.
For more information regarding this data and the
RBSPICE science goals and mission statement see the RBSPICE team web site at:
http:// rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-2_TOFXPHHHELT doi:tbd
Proper citations should include the "Accessed on date" in the form .
Description
RBSP RBSPICE TOF x PH Hydrogen Rates converted into units of physical intensity
(counts/(s*sr*cm^2*MeV) measured at high energy resolution and low time
resolution.
For more information regarding this data and the RBSPICE science
goals and mission statement see the RBSPICE team web site at: http:// 
rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-2_TOFXPHHLEHT doi:tbd
Proper citations should include the "Accessed on date" in the form .
Description
RBSP RBSPICE TOF x PH Hydrogen Rates converted into units of physical intensity
(counts/(s*sr*cm^2*MeV) measured at low energy resolution and high time
resolution.
For more information regarding this data and the RBSPICE science
goals and mission statement see the RBSPICE team web site at: http:// 
rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3-PAP_ESRHELT doi:10.48322/7mxy-dn25
Description
rbspa rbspice high energy res low time res electron energy intensities/pressures
sorted by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3-PAP_ESRLEHT doi:10.48322/ezsz-e525
Description
rbspa rbspice low energy res high time res electron energy intensities/pressures
sorted by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3-PAP_TOFXEH doi:10.48322/t323-cd86
Description
rbspice high energy res low time res tofxe proton intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
Version 2.0 Skeleton Produced October 1, 2015
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3-PAP_TOFXEHE doi:10.48322/knbt-qb86
Description
rbspice high energy res low time res tofxe helium intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3-PAP_TOFXEHE-0 doi:10.48322/z9kh-tp03
Description
rbspice high energy res low time res tofxe helium intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3-PAP_TOFXEION doi:10.48322/3wy7-bv28
Description
rbspice high energy res low time res tofxe ion intensities/pressures sorted by
pitch angles.
Modification History
Version 1.0 Skeleton Produced August 5, 2015
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3-PAP_TOFXEO doi:10.48322/gg52-1338
Description
rbspice high energy res low time res tofxe oxygen intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3-PAP_TOFXEO-0 doi:10.48322/nw9y-vj72
Description
rbspice high energy res low time res tofxe oxygen intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3-PAP_TOFXPHHHELT doi:10.48322/9j1k-re84
Description
rbspice high energy res low time res tofxph proton intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3-PAP_TOFXPHHLEHT doi:10.48322/1393-6m93
Description
rbspice high energy res low time res tofxph proton intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3-PAP_TOFXPHOHELT doi:10.48322/wsp2-ds36
Description
rbspice high energy res low time res tofxph oxygen intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3-PAP_TOFXPHOLEHT doi:10.48322/q87a-tn74
Description
rbspice low energy res high time res tofxph oxygen intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3_ESRHELT doi:10.48322/zcrq-hj26
Description
RBSPA RBSPICE High Energy Res Low Time Res Electron Intensities with Pitch
Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
Dataset in CDAWeb
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RBSP-A-RBSPICE_LEV-3_ESRLEHT doi:10.48322/n221-vw77
Description
RBSPA RBSPICE Low Energy Res High Time Res Electron Intensities with Pitch
Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3_ISRHELT doi:10.48322/daqq-gk90
Description
RBSPA RBSPICE High Energy Res Low Time Res Ion Energy Intensities with Pitch
Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3_TOFXEH doi:10.48322/e889-c285
Description
RBSPA RBSPICE High Energy Res Low Time Res TOFxE Proton Intensities with Pitch
Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3_TOFXEION doi:10.48322/ee6n-x567
Description
RBSPA RBSPICE High Energy Res Low Time Res TOFxE Ion Intensities with Pitch
Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3_TOFXENONH doi:10.48322/qghx-dt80
Description
RBSPA RBSPICE High Energy Res Low Time Res TOFxE non Proton Intensities with
Pitch Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3_TOFXPHHHELT doi:10.48322/nj27-cf05
Description
RBSPA RBSPICE High Energy Res Low Time Res TOFxPH Proton Intensities with Pitch
Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A-RBSPICE_LEV-3_TOFXPHHLEHT doi:10.48322/jstq-z957
Description
RBSPA RBSPICE Low Energy Res High Time Res TOFxPH Proton Rates converted into
units of physical intensity (counts/(s*sr*cm^2*MeV) measured at high energy
resolution and low time resolution which includes RBSPICE Pitch angle and
Magnetic Field derived values. \n For more information regarding this data and
the RBSPICE science goals and mission statement see the RBSPICE team web site
at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A_DENSITY_EMFISIS-L4 doi:10.48322/c4ha-xj50
Description
Density and other parameters inferred by digitizing the trace on the
spectrograms.
 
Dataset in CDAWeb
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RBSP-A_HFR-SPECTRA-BURST_EMFISIS-L2 doi:10.48322/18b2-kt74
Description
Single Axis AC Electric Field Spectra (Selectable between the U, V and W Axis).
Frequency range: 10 kHz to 486.97kHz    (Band width:480 Hz to 23.231kHz). 82
logarithmically spaced frequency bins. Cadence: 1 spectral matrix per 6 seconds.
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A_HFR-SPECTRA-MERGED_EMFISIS-L2 doi:10.48322/j4rf-2n06
Description
1
 
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RBSP-A_HFR-SPECTRA_EMFISIS-L2 doi:10.48322/2gay-q957
Description
Single Axis AC Electric Field Spectra (Selectable between the U, V and W Axis).
Frequency range: 10 kHz to 486.97kHz    (Band width:480 Hz to 23.231kHz). 82
logarithmically spaced frequency bins. Cadence: 1 spectral matrix per 6 seconds.
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A_HFR-WAVEFORM_EMFISIS-L2 doi:10.48322/pg1z-7a92
Description
Single Axis AC Electric Field Waveform (Selectable between the U, V and W Axis).
Units: V/m. Sample Rate: 1 Msample/sec. Sample Size: 4096 samples. Cadence:
variable.
 
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Data Access Code Examples written in Python and IDL®.
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RBSP-A_MAGNETOMETER_1SEC-GEI_EMFISIS-L3 doi:10.48322/esgw-y164
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A_MAGNETOMETER_1SEC-GEO_EMFISIS-L3 doi:10.48322/2913-5d64
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A_MAGNETOMETER_1SEC-GSE_EMFISIS-L3 doi:10.48322/s5sk-bm30
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A_MAGNETOMETER_1SEC-GSM_EMFISIS-L3 doi:10.48322/w6r4-fp76
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A_MAGNETOMETER_1SEC-SM_EMFISIS-L3 doi:10.48322/4kbj-9183
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A_MAGNETOMETER_4SEC-GEI_EMFISIS-L3 doi:10.48322/hnyz-nk70
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A_MAGNETOMETER_4SEC-GEO_EMFISIS-L3 doi:10.48322/zgv3-5m40
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A_MAGNETOMETER_4SEC-GSE_EMFISIS-L3 doi:10.48322/6f9r-x856
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A_MAGNETOMETER_4SEC-GSM_EMFISIS-L3 doi:10.48322/zrvq-vt55
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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RBSP-A_MAGNETOMETER_4SEC-SM_EMFISIS-L3 doi:10.48322/d15r-3a05
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
Dataset in CDAWeb
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RBSP-A_MAGNETOMETER_HIRES-GEI_EMFISIS-L3 doi:10.48322/q8rs-hg23
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
Dataset in CDAWeb
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RBSP-A_MAGNETOMETER_HIRES-GEO_EMFISIS-L3 doi:10.48322/yhbp-n321
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-A_MAGNETOMETER_HIRES-GSE_EMFISIS-L3 doi:10.48322/hn0a-s943
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-A_MAGNETOMETER_HIRES-GSM_EMFISIS-L3 doi:10.48322/2tyy-s986
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-A_MAGNETOMETER_HIRES-SM_EMFISIS-L3 doi:10.48322/h47r-sf90
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-A_MAGNETOMETER_UVW_EMFISIS-L2 doi:10.48322/8ttw-6h90
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-A_WFR-SPECTRAL-MATRIX-DIAGONAL-MERGED_EMFISIS-L2 doi:10.48322/at6y-vy38
Description
Three Axis Electric Field (EU, EV, EW) and Three Axis Magnetic field (BU, BV,
BW)  cross spectral matrix,  6 diagonal components and 15 off-diagonal
components.Frequency range: 10 kHz to 487kHz..82 Frequency Bins.Cadence: 1
spectra per 6 seconds (survey).
 
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RBSP-A_WFR-SPECTRAL-MATRIX-DIAGONAL_EMFISIS-L2 doi:10.48322/3v2f-af86
Description
Three Axis Electric Field (EU, EV, EW) and Three Axis Magnetic field (BU, BV,
BW)  cross spectral matrix,  6 diagonal components and 15 off-diagonal
components.Frequency range: 10 kHz to 487kHz..82 Frequency Bins.Cadence: 1
spectra per 6 seconds (survey).
 
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RBSP-A_WFR-SPECTRAL-MATRIX_EMFISIS-L2
Description
Three Axis Electric Field (EU, EV, EW) and Three Axis Magnetic field (BU, BV,
BW)  cross spectral matrix,  6 diagonal components and 15 off-diagonal
components.Frequency range: 10 kHz to 487kHz..82 Frequency Bins.Cadence: 1
spectra per 6 seconds (survey).
 
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RBSP-A_WFR-WAVEFORM-CONTINUOUS-BURST_EMFISIS-L2 doi:10.48322/czxv-qx38
Description
Three Axis Electric Field (EU, EV, EW) and Three Axis Magnetic field (BU, BV,
BW)  continuous burst waveforms208896 samples @ 35 kS/sec.
 
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RBSP-A_WFR-WAVEFORM_EMFISIS-L2 doi:10.48322/13vc-c837
Description
Three Axis Electric Field (EU, EV, EW) and Three Axis Magnetic field (BU, BV,
BW)  waveforms16384 samples @ 35 kS/sec...Calibration Notes:.Warning: All L2
Waveform products are calibrated in amplitude at 1kHz only.  There is no phase
calibration applied at this stage...Before using these waveforms to process wave
parameters, please follow the calibration process described below or the results
will be wrong...Level-2 (L2) Waveform data is amplitude-calibrated at 1 kHz. 
But there are amplitude deviations at other frequencies, and there are phase
shifts which are not reflected in the L2 data at all. The phase shift is a
frequency-dependent shift in the phase of the observed wave relative to the
input wave, tantamount to a time delay at that frequency. . .The L2 data can be
adjusted over frequency by applying dimensionless complex factors over frequency
immediately after Fourier transforming the L2 data. The Variables
BCalibrationCoef and ECalibration Coef in the cdf consists of a table for the B
sensors and a table for the E sensors. Each table has 5600 X 2 entries. The 
first column is the real component and the second is the imaginary component of
the calibration, extending from 2.13623 to 11962.89 Hz, in steps of 2.13623 Hz 
(Variable: CalFrequencies contains the associated frequencies of the calibration
coeficients). Above the highest frequency the WFR filters roll off; no
calibration measurements exist, but one could apply the last value to any
frequencies above that.. .The table is constructed assuming 16384 data points
are to be FFT'ed. If fewer than that are to be transformed, then the table can
be decimated to accommodate a shorter data set. The procedure is;  FFT the L2
data at the desired resolution and then perform a complex multiplication of the
FFT'ed dataset  and the E or B adjustment table.. .If comparing results of the
frequency-adjusted L2 data with the onboard survey spectra, note that the L2
data has units of volts/meter and nanoTesla for E and B respectively, whereas
the onboard survey spectra have units of RMS volts/meter and RMS nanoTesla.. 
 
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RBSP-A_WNA-SURVEY-SHEATH-CORRECTED-E_EMFISIS-L4
Description
Wave Normal Analysis products, based on L1 spectral matrix survey E and B data,
and produced via PRASSADCO (Santolik, et al., Radio Sci., 38(1), 1010, 2003). A
correction for antenna sheath effects has been applied to the electric field
data, before being input to PRASSADCO. The correction is density-dependent, so
fill values are inserted for E-dependent data where a density estimate is not
available.
 Be aware that the spin-plane E antennas began deployment at 2012-09-13T19:44,
and were not fully deployed until 2012-09-22T19:48. The spin-axis deployment
began on 2012-09-24T17:59 and did not fully complete until 2012-12-07T04:41.
Noise levels in the E data are increased by incomplete antenna deployment.
 There was a significant upgrade to the onboard calibration tables, for both E
and B in Feb 2013. Prior to this, the highest survey frequency bin (11.24 kHz)
used a flawed cal value that resulted in both amplitude and phase errors. The
effect is stronger for the B data. New, corrected, tables took effect at
2013-02-12T04:30:00.
 In Mar 2013, there was a ~2-day interval where a software issue resulted in the
wrong calibration tables being used for both E and B data. These data should be
used with extreme caution. The interval is 2013-03-21T06:53:00 to
2013-03-23T05:46:00.
 
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RBSP-B-RBSPICE_LEV-2_ESRHELT doi:10.48322/2zcv-0b61
Description
RBSP RBSPICE High Energy Resolution Electron Rates converted into units of
physical intensity (counts/(s*sr*cm^2*MeV) measured at high energy resolution
and low time resolution.
For more information regarding this data and the
RBSPICE science goals and mission statement see the RBSPICE team web site at:
http:// rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
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RBSP-B-RBSPICE_LEV-2_ESRLEHT doi:10.48322/btrq-0a49
Description
RBSP RBSPICE Low Energy Resolution Electron Rates converted into units of
physical intensity (counts/(s*sr*cm^2*MeV) measured at high energy resolution
and low time resolution.
For more information regarding this data and the
RBSPICE science goals and mission statement see the RBSPICE team web site at:
http:// rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
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RBSP-B-RBSPICE_LEV-2_ISRHELT doi:10.48322/gd0d-6e49
Description
RBSP RBSPICE high energy resolution Ion Species Rates (ISRHELT) converted into
units of physical intensity (counts/(s*sr*cm^2*MeV) measured at high energy
resolution and low time resolution.
For more information regarding this data and
the RBSPICE science goals and mission statement see the RBSPICE team web site
at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
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RBSP-B-RBSPICE_LEV-2_TOFXEH doi:10.48322/49dp-jw39
Description
RBSP RBSPICE TOF x Energy Hydrogen Rates converted into units of physical
intensity (counts/(s*sr*cm^2*MeV) measured at high energy resolution and low
time resolution.
For more information regarding this data and the RBSPICE
science goals and mission statement see the RBSPICE team web site at: http:// 
rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
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RBSP-B-RBSPICE_LEV-2_TOFXEION doi:10.48322/jt55-m188
Description
RBSP RBSPICE TOF x Energy Ion Rates converted into units of physical intensity
(counts/(s*sr*cm^2*MeV) measured at high energy resolution and low time
resolution.
For more information regarding this data and the RBSPICE science
goals and mission statement see the RBSPICE team web site at: http:// 
rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
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RBSP-B-RBSPICE_LEV-2_TOFXENONH doi:10.48322/v4tx-ej55
Description
RBSP RBSPICE TOF x E non Hydrogen (Helium and Oxygen) Rates converted into units
of physical intensity (counts/(s*sr*cm^2*MeV) measured at high energy resolution
and low time resolution.
For more information regarding this data and the
RBSPICE science goals and mission statement see the RBSPICE team web site at:
http:// rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
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RBSP-B-RBSPICE_LEV-2_TOFXPHHHELT doi:10.48322/4qe2-5145
Description
RBSP RBSPICE TOF x PH Hydrogen Rates converted into units of physical intensity
(counts/(s*sr*cm^2*MeV) measured at high energy resolution and low time
resolution.
For more information regarding this data and the RBSPICE science
goals and mission statement see the RBSPICE team web site at: http:// 
rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
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RBSP-B-RBSPICE_LEV-2_TOFXPHHLEHT doi:10.48322/2jc4-tb70
Description
RBSP RBSPICE TOF x PH Hydrogen Rates converted into units of physical intensity
(counts/(s*sr*cm^2*MeV) measured at low energy resolution and high time
resolution.
For more information regarding this data and the RBSPICE science
goals and mission statement see the RBSPICE team web site at: http:// 
rbspice.ftecs.com.
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
 
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RBSP-B-RBSPICE_LEV-3-PAP_ESRHELT doi:10.48322/yean-0a44
Description
rbspb rbspice high energy res low time res electron energy intensities/pressures
sorted by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
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RBSP-B-RBSPICE_LEV-3-PAP_ESRLEHT doi:10.48322/yq1a-4q76
Description
rbspb rbspice low energy res high time res electron energy intensities/pressures
sorted by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
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RBSP-B-RBSPICE_LEV-3-PAP_TOFXEH doi:10.48322/6n22-6807
Description
rbspice high energy res low time res tofxe proton intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
Version 2.0 Skeleton Produced October 1, 2015
 
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RBSP-B-RBSPICE_LEV-3-PAP_TOFXEHE doi:10.48322/0nfn-gt73
Description
rbspice high energy res low time res tofxe helium intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
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RBSP-B-RBSPICE_LEV-3-PAP_TOFXEHE-0 doi:10.48322/dkyf-gz14
Description
rbspice high energy res low time res tofxe helium intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
Dataset in CDAWeb
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RBSP-B-RBSPICE_LEV-3-PAP_TOFXEION doi:10.48322/ke3e-5s15
Description
rbspice high energy res low time res tofxeion ion intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced August 5, 2015
 
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RBSP-B-RBSPICE_LEV-3-PAP_TOFXEO doi:10.48322/7bnw-z839
Description
rbspice high energy res low time res tofxe oxygen intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
Dataset in CDAWeb
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RBSP-B-RBSPICE_LEV-3-PAP_TOFXEO-0 doi:10.48322/2c4e-dk29
Description
rbspice high energy res low time res tofxe oxygen intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
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RBSP-B-RBSPICE_LEV-3-PAP_TOFXPHHHELT doi:10.48322/7dg0-7h47
Description
rbspice high energy res low time res tofxph proton intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
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RBSP-B-RBSPICE_LEV-3-PAP_TOFXPHHLEHT doi:10.48322/njhg-7j22
Description
rbspice high energy res low time res tofxph proton intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
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RBSP-B-RBSPICE_LEV-3-PAP_TOFXPHOHELT doi:10.48322/hrv9-ec37
Description
rbspice high energy res low time res tofxph oxygen intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
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RBSP-B-RBSPICE_LEV-3-PAP_TOFXPHOLEHT doi:10.48322/bwm7-5m36
Description
rbspice low energy res high time res tofxph oxygen intensities/pressures sorted
by pitch angles.
Modification History
Version 1.0 Skeleton Produced July 29, 2014
 
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RBSP-B-RBSPICE_LEV-3_ESRHELT doi:10.48322/vn20-5g44
Description
RBSPB RBSPICE High Energy Res Low Time Res Electron Intensities with Pitch
Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Level 1.3 version produced December 20, 2012
L
 
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RBSP-B-RBSPICE_LEV-3_ESRLEHT doi:10.48322/nxsw-2k50
Description
RBSPB RBSPICE Low Energy Res High Time Res Electron Intensities with Pitch
Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
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RBSP-B-RBSPICE_LEV-3_ISRHELT doi:10.48322/1t5a-gm85
Description
RBSPB RBSPICE High Energy Res Low Time Res Ion Energy Intensities with Pitch
Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
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RBSP-B-RBSPICE_LEV-3_TOFXEH doi:10.48322/6crc-aj02
Description
RBSPB RBSPICE High Energy Res Low Time Res TOFxE Proton Intensities with Pitch
Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
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RBSP-B-RBSPICE_LEV-3_TOFXEION doi:10.48322/1qnv-8c11
Description
RBSPB RBSPICE High Energy Res Low Time Res TOFxE Ion Intensities with Pitch
Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
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RBSP-B-RBSPICE_LEV-3_TOFXENONH doi:10.48322/w7nq-kz93
Description
RBSPB RBSPICE High Energy Res Low Time Res TOFxE non Proton Intensities with
Pitch Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
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RBSP-B-RBSPICE_LEV-3_TOFXPHHHELT doi:10.48322/6wj8-zz20
Description
RBSPB RBSPICE High Energy Res Low Time Res TOFxPH Proton Intensities with Pitch
Angles converted into units of physical intensity (counts/(s*sr*cm^2*MeV)
measured at high energy resolution and low time resolution which includes
RBSPICE Pitch angle and Magnetic Field derived values. \n For more information
regarding this data and the RBSPICE science goals and mission statement see the
RBSPICE team web site at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
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RBSP-B-RBSPICE_LEV-3_TOFXPHHLEHT doi:10.48322/9f4c-2b63
Description
RBSPB RBSPICE Low Energy Res High Time Res TOFxPH Proton Rates converted into
units of physical intensity (counts/(s*sr*cm^2*MeV) measured at high energy
resolution and low time resolution which includes RBSPICE Pitch angle and
Magnetic Field derived values. \n For more information regarding this data and
the RBSPICE science goals and mission statement see the RBSPICE team web site
at: http:// rbspice.ftecs.com. 
Modification History
Skeleton Produced June 6, 2012
Version 1.3 produced December 20, 2012
L
 
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RBSP-B_DENSITY_EMFISIS-L4 doi:10.48322/c6s1-wg66
Description
Density and other parameters inferred by digitizing the trace on the
spectrograms.
 
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RBSP-B_HFR-SPECTRA-BURST_EMFISIS-L2 doi:10.48322/prbv-3b62
Description
Single Axis AC Electric Field Spectra (Selectable between the U, V and W Axis).
Frequency range: 10 kHz to 486.97kHz    (Band width:480 Hz to 23.231kHz). 82
logarithmically spaced frequency bins. Cadence: 1 spectral matrix per 6 seconds.
 
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RBSP-B_HFR-SPECTRA-MERGED_EMFISIS-L2 doi:10.48322/g03f-pz86
Description
1
 
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RBSP-B_HFR-SPECTRA_EMFISIS-L2 doi:10.48322/zpmq-qm18
Description
Single Axis AC Electric Field Spectra (Selectable between the U, V and W Axis).
Frequency range: 10 kHz to 486.97kHz    (Band width:480 Hz to 23.231kHz). 82
logarithmically spaced frequency bins. Cadence: 1 spectral matrix per 6 seconds.
 
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RBSP-B_HFR-WAVEFORM_EMFISIS-L2 doi:10.48322/dz64-x875
Description
Single Axis AC Electric Field Waveform (Selectable between the U, V and W Axis).
Units: V/m. Sample Rate: 1 Msample/sec. Sample Size: 4096 samples. Cadence:
variable.
 
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RBSP-B_MAGNETOMETER_1SEC-GEI_EMFISIS-L3 doi:10.48322/8zvn-5753
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_1SEC-GEO_EMFISIS-L3 doi:10.48322/9fmv-3p17
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_1SEC-GSE_EMFISIS-L3 doi:10.48322/xhkc-6v40
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_1SEC-GSM_EMFISIS-L3 doi:10.48322/x429-5310
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_1SEC-SM_EMFISIS-L3 doi:10.48322/fg6n-yr78
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_4SEC-GEI_EMFISIS-L3 doi:10.48322/7gy4-qd32
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_4SEC-GEO_EMFISIS-L3 doi:10.48322/5zd2-dk98
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_4SEC-GSE_EMFISIS-L3 doi:10.48322/e698-nb28
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_4SEC-GSM_EMFISIS-L3 doi:10.48322/kh8k-hc54
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_4SEC-SM_EMFISIS-L3 doi:10.48322/knn2-mp16
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_HIRES-GEI_EMFISIS-L3 doi:10.48322/b30v-s029
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_HIRES-GEO_EMFISIS-L3 doi:10.48322/y09z-a990
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_HIRES-GSE_EMFISIS-L3 doi:10.48322/mdts-0y61
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_HIRES-GSM_EMFISIS-L3 doi:10.48322/4dx1-s250
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_HIRES-SM_EMFISIS-L3 doi:10.48322/k10e-1w74
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_MAGNETOMETER_UVW_EMFISIS-L2 doi:10.48322/66f8-6c92
Description
3 axis Fluxgate Magnetometer data.  Sampled onboard at 64 vectors per second.  3
range states available,  Range 0 (+/- 256 nT),  Range 1 (+/- 4096 nT), Range 3
(+/- 65536 nT).
 
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RBSP-B_WFR-SPECTRAL-MATRIX-DIAGONAL-MERGED_EMFISIS-L2 doi:10.48322/0ch5-t113
Description
Three Axis Electric Field (EU, EV, EW) and Three Axis Magnetic field (BU, BV,
BW)  cross spectral matrix,  6 diagonal components and 15 off-diagonal
components.Frequency range: 10 kHz to 487kHz..82 Frequency Bins.Cadence: 1
spectra per 6 seconds (survey).
 
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RBSP-B_WFR-SPECTRAL-MATRIX-DIAGONAL_EMFISIS-L2 doi:10.48322/dafd-6p95
Description
Three Axis Electric Field (EU, EV, EW) and Three Axis Magnetic field (BU, BV,
BW)  cross spectral matrix,  6 diagonal components and 15 off-diagonal
components.Frequency range: 10 kHz to 487kHz..82 Frequency Bins.Cadence: 1
spectra per 6 seconds (survey).
 
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RBSP-B_WFR-SPECTRAL-MATRIX_EMFISIS-L2 doi:10.48322/abqk-a365
Description
Three Axis Electric Field (EU, EV, EW) and Three Axis Magnetic field (BU, BV,
BW)  cross spectral matrix,  6 diagonal components and 15 off-diagonal
components.Frequency range: 10 kHz to 487kHz..82 Frequency Bins.Cadence: 1
spectra per 6 seconds (survey).
 
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RBSP-B_WFR-WAVEFORM-CONTINUOUS-BURST_EMFISIS-L2 doi:10.48322/gm07-2739
Description
Three Axis Electric Field (EU, EV, EW) and Three Axis Magnetic field (BU, BV,
BW)  continuous burst waveforms208896 samples @ 35 kS/sec.
 
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RBSP-B_WFR-WAVEFORM_EMFISIS-L2 doi:10.48322/mf9b-6r41
Description
Three Axis Electric Field (EU, EV, EW) and Three Axis Magnetic field (BU, BV,
BW)  waveforms16384 samples @ 35 kS/sec...Calibration Notes:.Warning: All L2
Waveform products are calibrated in amplitude at 1kHz only.  There is no phase
calibration applied at this stage...Before using these waveforms to process wave
parameters, please follow the calibration process described below or the results
will be wrong...Level-2 (L2) Waveform data is amplitude-calibrated at 1 kHz. 
But there are amplitude deviations at other frequencies, and there are phase
shifts which are not reflected in the L2 data at all. The phase shift is a
frequency-dependent shift in the phase of the observed wave relative to the
input wave, tantamount to a time delay at that frequency. . .The L2 data can be
adjusted over frequency by applying dimensionless complex factors over frequency
immediately after Fourier transforming the L2 data. The Variables
BCalibrationCoef and ECalibration Coef in the cdf consists of a table for the B
sensors and a table for the E sensors. Each table has 5600 X 2 entries. The 
first column is the real component and the second is the imaginary component of
the calibration, extending from 2.13623 to 11962.89 Hz, in steps of 2.13623 Hz 
(Variable: CalFrequencies contains the associated frequencies of the calibration
coeficients). Above the highest frequency the WFR filters roll off; no
calibration measurements exist, but one could apply the last value to any
frequencies above that.. .The table is constructed assuming 16384 data points
are to be FFT'ed. If fewer than that are to be transformed, then the table can
be decimated to accommodate a shorter data set. The procedure is;  FFT the L2
data at the desired resolution and then perform a complex multiplication of the
FFT'ed dataset  and the E or B adjustment table.. .If comparing results of the
frequency-adjusted L2 data with the onboard survey spectra, note that the L2
data has units of volts/meter and nanoTesla for E and B respectively, whereas
the onboard survey spectra have units of RMS volts/meter and RMS nanoTesla.. 
 
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RBSP-B_WNA-SURVEY-SHEATH-CORRECTED-E_EMFISIS-L4
Description
Wave Normal Analysis products, based on L1 spectral matrix survey E and B data,
and produced via PRASSADCO (Santolik, et al., Radio Sci., 38(1), 1010, 2003). A
correction for antenna sheath effects has been applied to the electric field
data, before being input to PRASSADCO. The correction is density-dependent, so
fill values are inserted for E-dependent data where a density estimate is not
available.
 Be aware that the spin-plane E antennas began deployment at 2012-09-13T23:06,
and were not fully deployed until 2012-09-22T22:32. The spin-axis deployment
began on 2012-09-24T20:33 and did not fully complete until 2012-12-07T17:25.
Noise levels in the E data are increased by incomplete antenna deployment.
 There was a significant upgrade to the onboard calibration tables, for both E
and B in Feb 2013. Prior to this, the highest survey frequency bin (11.24 kHz)
used a flawed cal value that resulted in both amplitude and phase errors. The
effect is stronger for the B data. New, corrected, tables took effect at
2013-02-13T01:48:00.
 In Mar 2013, there was a ~2-day interval where a software issue resulted in the
wrong calibration tables being used for both E and B data. These data should be
used with extreme caution. The interval is 2013-03-21T09:35:00 to
2013-03-23T02:07:00.
 
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RBSPA_EFW-L2_E-HIRES-UVW doi:10.48322/qtvb-dd97
Description
High Resolution DC Electric Field in UVW Coordinates.
Modification History
v01:  initial version.
 
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RBSPA_EFW-L2_E-SPINFIT-MGSE doi:10.48322/rhve-mz23
Description
CDAWeb interface derived data on Fri Jun 14 15:33:16 EDT 2013. Contacts: 
Tami.J.Kovalick@nasa.gov, Rita.C.Johnson@nasa.gov. Spinfit DC electric field
estimates in the M-GSE coordinate system - see the EFW-FAQ
(http://rbsp.space.umn.edu/efw_faq.html) for a description of the spin fit 
algorithm and the M-GSE coordinate system.
One 2D vector estimate of the E-field is computed at a cadence of once per spin
period (typ. 10.7 to 11.1 s) using the survey E-field data product - the
potential difference between EFW sensors V1 and V2 (E12) or V3 and V4 (E34)
sampled at a nominal rate of 32 samp/s with a resolution of 16 bits.
The X-component of the E-field estimate, corresponding to the axial component in
the spacecraft coordinate system, is set to zero in this data product.  See the
EFW-FAQ (http://rbsp.space.umn.edu/efw_faq.html) for a discussion of this 
convention for this data product.
The VxB electric field in the spacecraft frame due to orbital motion of the
spacecraft around the Earth as computed from the spacecraft orbital velocity and
measured B-field in the spacraft frame has been subtracted from the measured
electric field, and so the data product is in the quasi-inertial frame
equivalent to GSE (i.e. it is NOT in the corotation frame of the Earth!).
Each spin fit is time-tagged with the time corresponding to the middle of the
spin of data that went into the spin fit algorithm; in other words, if a given
spin covers the interval [t1, t2), then the spin fit E-field estimate associated
with that spin is given the time tag 0.5*(t1 + t2).
The root mean square residual between the data included in the fit and the
resulting best-fit model, sigma, and the final number of points included in the
spin fit, npts, are also provided at spin-period cadence.
The nominal dynamic range of the E-field estimate is +/- 1 V/m in any component.
Modification History
v01:  initial version.
 
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RBSPA_EFW-L2_ESVY_DESPUN doi:10.48322/t40m-em97
Description
CDAWeb interface derived data on Fri Jun 14 15:33:16 EDT 2013. Contacts: 
Tami.J.Kovalick@nasa.gov, Rita.C.Johnson@nasa.gov. Spinfit DC electric field
estimates in the M-GSE coordinate system - see the EFW-FAQ
(http://rbsp.space.umn.edu/efw_faq.html) for a description of the spin fit 
algorithm and the M-GSE coordinate system.
One 2D vector estimate of the E-field is computed at a cadence of once per spin
period (typ. 10.7 to 11.1 s) using the survey E-field data product - the
potential difference between EFW sensors V1 and V2 (E12) or V3 and V4 (E34)
sampled at a nominal rate of 32 samp/s with a resolution of 16 bits.
The X-component of the E-field estimate, corresponding to the axial component in
the spacecraft coordinate system, is set to zero in this data product.  See the
EFW-FAQ (http://rbsp.space.umn.edu/efw_faq.html) for a discussion of this 
convention for this data product.
The VxB electric field in the spacecraft frame due to orbital motion of the
spacecraft around the Earth as computed from the spacecraft orbital velocity and
measured B-field in the spacraft frame has been subtracted from the measured
electric field, and so the data product is in the quasi-inertial frame
equivalent to GSE (i.e. it is NOT in the corotation frame of the Earth!).
Each spin fit is time-tagged with the time corresponding to the middle of the
spin of data that went into the spin fit algorithm; in other words, if a given
spin covers the interval [t1, t2), then the spin fit E-field estimate associated
with that spin is given the time tag 0.5*(t1 + t2).
The root mean square residual between the data included in the fit and the
resulting best-fit model, sigma, and the final number of points included in the
spin fit, npts, are also provided at spin-period cadence.
The nominal dynamic range of the E-field estimate is +/- 1 V/m in any component.
Modification History
v01:  initial version.
 
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RBSPA_EFW-L2_FBK doi:10.48322/6a7j-p736
Description
Up to two sources are returned. The possible sources are:
E12DC, E34DC,E56DC,
E12AC,E34AC,E56AC,
SCMU,SCMV,SCMW
(V1DC+V2DC+V3DC+V4DC)/4
 
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RBSPA_EFW-L2_SPEC doi:10.48322/78pf-4k59
Description
Six spectral products are returned. The possible sources
are:.E12dc,E34dc,E56dc.E12ac,E34ac,E56ac.Edcpar,Edcprp.Eacpar,Eacprp.V1ac,V2ac,V
3ac,V4ac,V5ac,V6ac.SCMU,SCMV,SCMW.SCMpar,SCMprp,.(V1ac+V2ac+V3ac+V4ac)/4,.Edcprp
2, Eacprp2, SCMprp2.
Caveats
See THEMIS website for caveats
 
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RBSPA_EFW-L2_VSVY-HIRES doi:10.48322/7mwt-de58
Description
CDAWeb interface derived data on Fri Jun 14 15:33:16 EDT 2013. Contacts: 
Tami.J.Kovalick@nasa.gov, Rita.C.Johnson@nasa.gov. Spinfit DC electric field
estimates in the M-GSE coordinate system - see the EFW-FAQ
(http://rbsp.space.umn.edu/efw_faq.html) for a description of the spin fit 
algorithm and the M-GSE coordinate system.
One 2D vector estimate of the E-field is computed at a cadence of once per spin
period (typ. 10.7 to 11.1 s) using the survey E-field data product - the
potential difference between EFW sensors V1 and V2 (E12) or V3 and V4 (E34)
sampled at a nominal rate of 32 samp/s with a resolution of 16 bits.
The X-component of the E-field estimate, corresponding to the axial component in
the spacecraft coordinate system, is set to zero in this data product.  See the
EFW-FAQ (http://rbsp.space.umn.edu/efw_faq.html) for a discussion of this 
convention for this data product.
The VxB electric field in the spacecraft frame due to orbital motion of the
spacecraft around the Earth as computed from the spacecraft orbital velocity and
measured B-field in the spacraft frame has been subtracted from the measured
electric field, and so the data product is in the quasi-inertial frame
equivalent to GSE (i.e. it is NOT in the corotation frame of the Earth!).
Each spin fit is time-tagged with the time corresponding to the middle of the
spin of data that went into the spin fit algorithm; in other words, if a given
spin covers the interval [t1, t2), then the spin fit E-field estimate associated
with that spin is given the time tag 0.5*(t1 + t2).
The root mean square residual between the data included in the fit and the
resulting best-fit model, sigma, and the final number of points included in the
spin fit, npts, are also provided at spin-period cadence.
The nominal dynamic range of the E-field estimate is +/- 1 V/m in any component.
 
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RBSPA_EFW_BURST-WAVEFORM-UVW-L1 doi:10.48322/jcd5-kf50
Description
No TEXT global attribute value.
 
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RBSPA_L2-1MIN_PSBR-RPS doi:10.48322/h4my-4k78
Description
The RPS instrument is a solid state detector telescope combined with a Cherenkov
radiator. It measures protons with energies from about 60 MeV to about 2 GeV.
For more information, see .http://rbsp.aerospace.org/. For a complete description 
of the instrument, see Mazur et al., 2012, The Relativistic Proton Spectrometer
(RPS) for the Van Allen Probes Mission (formerly known as Radiation Belt Storm
Probes, RBSP), Space Science Reviews. DOI 10.1007/s11214-012-9926-9, 
http://www.springerlink.com/content/p84680786570g7qp/. The instrument PI, Dr.
Joe Mazur, can be reached at Joseph.E.Mazur@aero.org.
Modification History
TBD
 
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RBSPA_L2_PSBR-RPS doi:10.48322/a587-0r70
Description
The RPS instrument is a solid state detector telescope combined with a Cherenkov
radiator. It measures protons with energies from about 60 MeV to about 2 GeV.
For more information, see .http://rbsp.aerospace.org/. For a complete description 
of the instrument, see Mazur et al., 2012, The Relativistic Proton Spectrometer
(RPS) for the Van Allen Probes Mission (formerly known as Radiation Belt Storm
Probes, RBSP), Space Science Reviews. DOI 10.1007/s11214-012-9926-9, 
http://www.springerlink.com/content/p84680786570g7qp/. The instrument PI, Dr.
Joe Mazur, can be reached at Joseph.E.Mazur@aero.org.
Modification History
TBD
 
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RBSPA_REL03_ECT-MAGEIS-L2 doi:10.48322/dhj8-f337
Description
MagEIS consists of 4 energetic particle sensors per RBSP spacecraft: low unit,
medium35 unit, medium75 unit and the high unit.  The low and 2 medium units are
magnetic spectrometers that measure electrons across roughly the 20 keV - 1 MeV
energy range. The high unit contains a magnetic spectrometer that measures
electrons from roughly the 700 keV to 4 MeV range. The high unit also has a
proton telescope that measures protons from roughly 50 keV to 20 MeV, Helium
ions from roughly 300 keV - 1.5 MeV and Oxygen ions from roughly 1-5 MeV. 
MagEIS is one of three instrument packages on the ECT instrument suite (HOPE and
REPT are the others).
 
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RBSPA_REL03_ECT-REPT-SCI-L2 doi:10.48322/hpp2-yy26
Description
RBSP Relativistic Electron Proton Telescope, Level 2 science data
Modification History
CDF skeleton version of rbsp_rept_science_l2_data.template.cdf written by R.
Reukauf
 
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RBSPA_REL03_ECT-REPT-SCI-L3 doi:10.48322/4x5t-th95
Description
Van Allen Probes, RBSPECT/REPT (Radiation Belt Storm Probes Energetic particle,
Composition and Thermal plasma suite/Relativistic Electron Proton Telescope,
Level 3 Pitch Angle Sorted Data.
 
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RBSPA_REL04_ECT-HOPE-MOM-L3 doi:10.48322/egeg-7005
Description
none
Modification History
CDF skeleton version of 20120705.Written by B. Larsen.20140304
 
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RBSPA_REL04_ECT-HOPE-PA-L3 doi:10.48322/17p9-rf75
Description
Pitch angle binned data from the HOPE plasma spectrometer.  Note that there are
no correections performed on the data (e.g. background subtraction, velocity
corrections, etc.)
Modification History
CDF skeleton version of 20120705. Written by R. Friedel.
20120706 version written by R. Skoug. 
20130715 revisions by J. T. Niehof.
20130808 revisions by J. T. Niehof/BA Larsen.
20130927 revision (remove per-mode variables)by J. T. Niehof.
 
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RBSPA_REL04_ECT-HOPE-SCI-L2 doi:10.48322/34q8-8q26
Description
none
Modification History
CDF skeleton version of 20120705.Written by R. Friedel..20120706 version,
written by R. Skoug.20130715 revisions by J. T. Niehof.20120706 version, written
by R. Skoug.20130715 revisions by J. T. Niehof.20120706 version, written by R.
Skoug.20130715 revisions by J. T. Niehof
20120706 version, written by R. Skoug
20130715 revisions by J. T. Niehof
 
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RBSPA_REL04_ECT-HOPE-SCI-L2SA doi:10.48322/rcxw-mm23
Description
none
Modification History
CDF skeleton version of 20120705.Written by R. Friedel..20120706 version,
written by R. Skoug.20130715 revisions by J. T. Niehof.20120706 version, written
by R. Skoug.20130715 revisions by J. T. Niehof.20120706 version, written by R.
Skoug.20130715 revisions by J. T. Niehof
20120706 version, written by R. Skoug
20130715 revisions by J. T. Niehof
 
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RBSPA_REL04_ECT-MAGEIS-L3 doi:10.48322/09qz-tf17
Description
Van Allen Probes, RBSPECT/MagEIS (Radiation Belt Storm Probes Energetic
particle, Composition and Thermal plasma suite/Magnetic Electron Ion
Spectrometer, Level 3 Pitch Angle Sorted Data.
 
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RBSPB_EFW-L2_E-HIRES-UVW doi:10.48322/64bn-y776
Description
High Resolution DC Electric Field in UVW Coordinates.
Modification History
v01:  initial version.
 
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RBSPB_EFW-L2_E-SPINFIT-MGSE doi:10.48322/s0hb-rp21
Description
CDAWeb interface derived data on Fri Jun 14 15:33:16 EDT 2013. Contacts: 
Tami.J.Kovalick@nasa.gov, Rita.C.Johnson@nasa.gov. Spinfit DC electric field
estimates in the M-GSE coordinate system - see the EFW-FAQ
(http://rbsp.space.umn.edu/efw_faq.html) for a description of the spin fit 
algorithm and the M-GSE coordinate system.
One 2D vector estimate of the E-field is computed at a cadence of once per spin
period (typ. 10.7 to 11.1 s) using the survey E-field data product - the
potential difference between EFW sensors V1 and V2 (E12) or V3 and V4 (E34)
sampled at a nominal rate of 32 samp/s with a resolution of 16 bits.
The X-component of the E-field estimate, corresponding to the axial component in
the spacecraft coordinate system, is set to zero in this data product.  See the
EFW-FAQ (http://rbsp.space.umn.edu/efw_faq.html) for a discussion of this 
convention for this data product.
The VxB electric field in the spacecraft frame due to orbital motion of the
spacecraft around the Earth as computed from the spacecraft orbital velocity and
measured B-field in the spaceraft frame has been subtracted from the measured
electric field, and so the data product is in the quasi-inertial frame
equivalent to GSE (i.e. it is NOT in the corotation frame of the Earth!).
Each spin fit is time-tagged with the time corresponding to the middle of the
spin of data that went into the spin fit algorithm; in other words, if a given
spin covers the interval [t1, t2), then the spin fit E-field estimate associated
with that spin is given the time tag 0.5*(t1 + t2).
The root mean square residual between the data included in the fit and the
resulting best-fit model, sigma, and the final number of points included in the
spin fit, npts, are also provided at spin-period cadence.
The nominal dynamic range of the E-field estimate is +/- 1 V/m in any component.
 
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RBSPB_EFW-L2_ESVY_DESPUN doi:10.48322/036a-q517
Description
CDAWeb interface derived data on Fri Jun 14 15:33:16 EDT 2013. Contacts: 
Tami.J.Kovalick@nasa.gov, Rita.C.Johnson@nasa.gov. Spinfit DC electric field
estimates in the M-GSE coordinate system - see the EFW-FAQ
(http://rbsp.space.umn.edu/efw_faq.html) for a description of the spin fit 
algorithm and the M-GSE coordinate system.
One 2D vector estimate of the E-field is computed at a cadence of once per spin
period (typ. 10.7 to 11.1 s) using the survey E-field data product - the
potential difference between EFW sensors V1 and V2 (E12) or V3 and V4 (E34)
sampled at a nominal rate of 32 samp/s with a resolution of 16 bits.
The X-component of the E-field estimate, corresponding to the axial component in
the spacecraft coordinate system, is set to zero in this data product.  See the
EFW-FAQ (http://rbsp.space.umn.edu/efw_faq.html) for a discussion of this 
convention for this data product.
The VxB electric field in the spacecraft frame due to orbital motion of the
spacecraft around the Earth as computed from the spacecraft orbital velocity and
measured B-field in the spaceraft frame has been subtracted from the measured
electric field, and so the data product is in the quasi-inertial frame
equivalent to GSE (i.e. it is NOT in the corotation frame of the Earth!).
Each spin fit is time-tagged with the time corresponding to the middle of the
spin of data that went into the spin fit algorithm; in other words, if a given
spin covers the interval [t1, t2), then the spin fit E-field estimate associated
with that spin is given the time tag 0.5*(t1 + t2).
The root mean square residual between the data included in the fit and the
resulting best-fit model, sigma, and the final number of points included in the
spin fit, npts, are also provided at spin-period cadence.
The nominal dynamic range of the E-field estimate is +/- 1 V/m in any component.
 
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RBSPB_EFW-L2_FBK doi:10.48322/m9dn-c472
Description
Up to two sources are returned. The possible sources are:
E12DC, E34DC,E56DC,
E12AC,E34AC,E56AC,
SCMU,SCMV,SCMW
(V1DC+V2DC+V3DC+V4DC)/4
 
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RBSPB_EFW-L2_SPEC doi:10.48322/hdnm-mh60
Description
Six spectral products are returned. The possible sources
are:.E12dc,E34dc,E56dc.E12ac,E34ac,E56ac.Edcpar,Edcprp.Eacpar,Eacprp.V1ac,V2ac,V
3ac,V4ac,V5ac,V6ac.SCMU,SCMV,SCMW.SCMpar,SCMprp,.(V1ac+V2ac+V3ac+V4ac)/4,.Edcprp
2, Eacprp2, SCMprp2.
Caveats
See THEMIS website for caveats
 
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RBSPB_EFW-L2_VSVY-HIRES doi:10.48322/e9bt-8x09
Description
CDAWeb interface derived data on Fri Jun 14 15:33:16 EDT 2013. Contacts: 
Tami.J.Kovalick@nasa.gov, Rita.C.Johnson@nasa.gov. Spinfit DC electric field
estimates in the M-GSE coordinate system - see the EFW-FAQ
(http://rbsp.space.umn.edu/efw_faq.html) for a description of the spin fit 
algorithm and the M-GSE coordinate system.
One 2D vector estimate of the E-field is computed at a cadence of once per spin
period (typ. 10.7 to 11.1 s) using the survey E-field data product - the
potential difference between EFW sensors V1 and V2 (E12) or V3 and V4 (E34)
sampled at a nominal rate of 32 samp/s with a resolution of 16 bits.
The X-component of the E-field estimate, corresponding to the axial component in
the spacecraft coordinate system, is set to zero in this data product.  See the
EFW-FAQ (http://rbsp.space.umn.edu/efw_faq.html) for a discussion of this 
convention for this data product.
The VxB electric field in the spacecraft frame due to orbital motion of the
spacecraft around the Earth as computed from the spacecraft orbital velocity and
measured B-field in the spaceraft frame has been subtracted from the measured
electric field, and so the data product is in the quasi-inertial frame
equivalent to GSE (i.e. it is NOT in the corotation frame of the Earth!).
Each spin fit is time-tagged with the time corresponding to the middle of the
spin of data that went into the spin fit algorithm; in other words, if a given
spin covers the interval [t1, t2), then the spin fit E-field estimate associated
with that spin is given the time tag 0.5*(t1 + t2).
The root mean square residual between the data included in the fit and the
resulting best-fit model, sigma, and the final number of points included in the
spin fit, npts, are also provided at spin-period cadence.
The nominal dynamic range of the E-field estimate is +/- 1 V/m in any component.
 
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RBSPB_EFW_BURST-WAVEFORM-UVW-L1 doi:10.48322/zbw6-0626
Description
No TEXT global attribute value.
 
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RBSPB_L2-1MIN_PSBR-RPS doi:10.48322/r0b5-m046
Description
The RPS instrument is a solid state detector telescope combined with a Cherenkov
radiator. It measures protons with energies from about 60 MeV to about 2 GeV.
For more information, see .http://rbsp.aerospace.org/. For a complete description 
of the instrument, see Mazur et al., 2012, The Relativistic Proton Spectrometer
(RPS) for the Van Allen Probes Mission (formerly known as Radiation Belt Storm
Probes, RBSP), Space Science Reviews. DOI 10.1007/s11214-012-9926-9, 
http://www.springerlink.com/content/p84680786570g7qp/. The instrument PI, Dr.
Joe Mazur, can be reached at Joseph.E.Mazur@aero.org.
Modification History
TBD
 
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RBSPB_L2_PSBR-RPS doi:10.48322/b5me-tj22
Description
The RPS instrument is a solid state detector telescope combined with a Cherenkov
radiator. It measures protons with energies from about 60 MeV to about 2 GeV.
For more information, see .http://rbsp.aerospace.org/. For a complete description 
of the instrument, see Mazur et al., 2012, The Relativistic Proton Spectrometer
(RPS) for the Van Allen Probes Mission (formerly known as Radiation Belt Storm
Probes, RBSP), Space Science Reviews. DOI 10.1007/s11214-012-9926-9, 
http://www.springerlink.com/content/p84680786570g7qp/. The instrument PI, Dr.
Joe Mazur, can be reached at Joseph.E.Mazur@aero.org.
Modification History
TBD
 
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RBSPB_REL03_ECT-MAGEIS-L2 doi:10.48322/mfa4-z841
Description
MagEIS consists of 4 energetic particle sensors per RBSP spacecraft: low unit,
medium35 unit, medium75 unit and the high unit.  The low and 2 medium units are
magnetic spectrometers that measure electrons across roughly the 20 keV - 1 MeV
energy range. The high unit contains a magnetic spectrometer that measures
electrons from roughly the 700 keV to 4 MeV range. The high unit also has a
proton telescope that measures protons from roughly 50 keV to 20 MeV, Helium
ions from roughly 300 keV - 1.5 MeV and Oxygen ions from roughly 1-5 MeV. 
MagEIS is one of three instrument packages on the ECT instrument suite (HOPE and
REPT are the others).
 
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RBSPB_REL03_ECT-REPT-SCI-L2 doi:10.48322/nzhx-1t77
Description
RBSP Relativistic Electron Proton Telescope, Level 2 science data
Modification History
CDF skeleton version of rbsp_rept_science_l2_data.template.cdf written by R.
Reukauf
 
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RBSPB_REL03_ECT-REPT-SCI-L3 doi:10.48322/5t1q-9z75
Description
Van Allen Probes, RBSPECT/REPT (Radiation Belt Storm Probes Energetic particle,
Composition and Thermal plasma suite/Relativistic Electron Proton Telescope,
Level 3 Pitch Angle Sorted Data.
 
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RBSPB_REL04_ECT-HOPE-MOM-L3 doi:10.48322/ndtr-v928
Description
none
Modification History
CDF skeleton version of 20120705.Written by B. Larsen.20140304
 
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RBSPB_REL04_ECT-HOPE-PA-L3 doi:10.48322/4671-8e02
Description
Pitch angle binned data from the HOPE plasma spectrometer.  Note that there are
no correections performed on the data (e.g. background subtraction, velocity
corrections, etc.)
Modification History
CDF skeleton version of 20120705. Written by R. Friedel.
20120706 version written by R. Skoug. 
20130715 revisions by J. T. Niehof.
20130808 revisions by J. T. Niehof/BA Larsen.
20130927 revision (remove per-mode variables)by J. T. Niehof.
 
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RBSPB_REL04_ECT-HOPE-SCI-L2 doi:10.48322/1xw2-1868
Description
none
Modification History
CDF skeleton version of 20120705.Written by R. Friedel..20120706 version,
written by R. Skoug.20130715 revisions by J. T. Niehof.20120706 version, written
by R. Skoug.20130715 revisions by J. T. Niehof.20120706 version, written by R.
Skoug.20130715 revisions by J. T. Niehof
20120706 version, written by R. Skoug
20130715 revisions by J. T. Niehof
 
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RBSPB_REL04_ECT-HOPE-SCI-L2SA doi:10.48322/68w5-kh78
Description
none
Modification History
CDF skeleton version of 20120705.Written by R. Friedel..20120706 version,
written by R. Skoug.20130715 revisions by J. T. Niehof.20120706 version, written
by R. Skoug.20130715 revisions by J. T. Niehof.20120706 version, written by R.
Skoug.20130715 revisions by J. T. Niehof
20120706 version, written by R. Skoug
20130715 revisions by J. T. Niehof
 
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RBSPB_REL04_ECT-MAGEIS-L3 doi:10.48322/6qrc-aq80
Description
Van Allen Probes, RBSPECT/MagEIS (Radiation Belt Storm Probes Energetic
particle, Composition and Thermal plasma suite/Magnetic Electron Ion
Spectrometer, Level 3 Pitch Angle Sorted Data.
 
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RBSP_ECT-REPT-SCI-L3-SELESNICK-MODEL doi:10.48322/0qyz-h276
Description
The files contain model radiation belt proton intensity derived from data taken
by the Van Allen Probes REPT instruments using the method described by:
Selesnick, R. S., Baker, D. N., Kanekal, S. G., Hoxie, V. C., & Li, X. (2018). 
Modeling the proton radiation belt with Van Allen Probes Relativistic
Electron-Proton Telescope data. Journal of Geophysical Research: Space Physics,
123. https://doi.org/10.1002/2017JA024661 Each file contains average intensity, 
as a function of kinetic energy, equatorial pitch angle, and L-shell, derived
from 1 month of data. 
 
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REACH-VID-101_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-102_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-105_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-108_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-113_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-114_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-115_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-116_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-133_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-134_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-135_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-136_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-137_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-138_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-139_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-140_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-148_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-149_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-162_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-163_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-164_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-165_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-166_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-169_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-170_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-171_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-172_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-173_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-175_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-176_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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REACH-VID-180_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
Dataset in CDAWeb
Data Access Code Examples written in Python and IDL®.
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REACH-VID-181_DOSIMETER-L1C
Description
The Responsive Environmental Assessment Commercially Hosted (REACH)
constellation is collection of 32 small sensors hosted on six orbital planes of
the Iridium-Next space vehicles in low earth orbit. Each sensor contains two
micro-dosimeters sensitive to the passage of charged particles from the Earth's
radiation belts. There are six distinct dosimeter types spread among the 64
individual sensors, which are unique in shielding and electronic threshold. When
taken together, this effectively enables a high time-cadence measurement of
protons and electrons in six integral energy channels over the entire globe.
 
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RENU2_H0_EFIELD doi:10.48322/35v3-c331
Description
RENU2 COrnell Wire BOom Yo-yo (COWBOY)
 
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RENU2_H0_EPLAS doi:10.48322/5zvf-1q82
Description
RENU2 EPLAS
 
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RENU2_H0_ERPAMAIN doi:10.48322/7hy6-k889
Description
RENU2 ERPA
 
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RENU2_H0_ERPASUB doi:10.48322/cy19-2944
Description
RENU2 ERPA
 
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RENU2_H0_FGM doi:10.48322/ndrv-ds51
Description
RENU2 magnetometer
 
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RENU2_H0_IG2 doi:10.48322/k3hd-7y51
Description
RENU2 ionization gauge
 
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RENU2_H0_PMT doi:10.48322/hwz5-q486
Description
RENU2 PMT counts converted to Rayleighs and background subtracted
 
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RENU2_H0_UVPMT doi:10.48322/f1c4-b375
Description
RENU2 UV PMT
 
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RENU2_H0_VLF doi:10.48322/7pss-6w70
Description
RENU2 COrnell Wire BOom Yo-yo (COWBOY)
 
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ROSETTA_HELIO1DAY_POSITION (spase://NASA/NumericalData/Rosetta/HelioWeb/Ephemeris/P1D)
Description
No TEXT global attribute value.
 
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RS_K0_IPEI (spase://NASA/NumericalData/ROCSAT-1/IPEI/PT1s)
Description
1-second averaged data
***Important Notes*** on Accuracy of VperpM_MF (meridional),VperpZ_MF (zonal),
and VparaMF (parallel) components.
Geophysical flow components VperpM_MF, VperpZ_MF, and VparaMF are converted from
flow velocities, Vx, Vy, and Vz 
measured in the S/C coordinate system. Vx points along the S/C trajectory
vector, Vz is in the nadir direction, 
and Vy points to the right of the S/C trajectory vector (in the anti-angular
momentum direction).
1) Vx, Vy, and Vz are measured flow velocities at S/C coordinate in the
Earth-centered Inertia Coordinate System (non-rotating) (ECI coordinate).
2) VperZ_MF, VperM_MF, and VparaMF are geophysical flows in the Earth-centered
Fixed Coordinated System (rotate with the Earth) (ECF coordinate).
3) Uncertainty of +-(37.8-75.45) m/s in Vx based on 0.5% - 1% error in fitting
could be introduced to all geophysical flow components.
4) VperpM_MF at low latitude is almost identical to (-Vz). No Vx is included so
that it is very reliable.
5) Uncertainties from Vx could exist in VperpZ_MF and VparaMF.
6) VperpZ_MF and VparaMF can be used to study the relative changes in flow
velocity due to  geophysical effects.
But can not be used to study the long-term variations because the result could
be biased by the uncertainty in Vx.
Modification History
Version 1.0 Jan. 28, 2008
 
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