{ "HAPI": "3.2.0", "status": { "code": 1200, "message": "OK" }, "parameters": [ { "name": "time", "type": "isotime", "units": "UTC", "length": 24, "fill": null }, { "name": "accum_time", "description": "Number of one-second accumulations per sample. Not corrected for dead time.", "units": "accumulations", "fill": "65535", "type": "integer" }, { "name": "electron_counts_epam_0_0", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_epam_0_1", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_epam_1_0", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_epam_1_1", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_epam_2_0", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_epam_2_1", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_epam_3_0", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_epam_3_1", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_raw_epam_0_0", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_raw_epam_0_1", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_raw_epam_1_0", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_raw_epam_1_1", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_raw_epam_2_0", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_raw_epam_2_1", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_raw_epam_3_0", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_counts_raw_epam_3_1", "description": "Spectrally-summed counts in the pseudo-EPAM electron channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "electron_energy_edges_epam_0_0", "description": "Edges of pseudo-EPAM electron energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_energy_edges_epam_0_1", "description": "Edges of pseudo-EPAM electron energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_energy_edges_epam_1_0", "description": "Edges of pseudo-EPAM electron energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_energy_edges_epam_1_1", "description": "Edges of pseudo-EPAM electron energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_energy_edges_epam_2_0", "description": "Edges of pseudo-EPAM electron energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_energy_edges_epam_2_1", "description": "Edges of pseudo-EPAM electron energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_energy_edges_epam_3_0", "description": "Edges of pseudo-EPAM electron energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_energy_edges_epam_3_1", "description": "Edges of pseudo-EPAM electron energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_energy_epam_weighted_GdE_0", "description": "Average of midpoint energies of STIS electron channels comprising the pseudo-EPAM channel, weighted by the spectral responses (GdE) of each STIS channel. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_energy_epam_weighted_GdE_1", "description": "Average of midpoint energies of STIS electron channels comprising the pseudo-EPAM channel, weighted by the spectral responses (GdE) of each STIS channel. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_energy_epam_weighted_GdE_2", "description": "Average of midpoint energies of STIS electron channels comprising the pseudo-EPAM channel, weighted by the spectral responses (GdE) of each STIS channel. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_energy_epam_weighted_GdE_3", "description": "Average of midpoint energies of STIS electron channels comprising the pseudo-EPAM channel, weighted by the spectral responses (GdE) of each STIS channel. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_flux_epam_weighted_GdE_0", "description": "Pseudo-EPAM high-dynamic-range differential electron flux as function of energy. Averages of STIS fluxes whose midpoint energies lie within the EPAM channel energy edges, weighted by the spectral responses (GdE) of each STIS channel.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_flux_epam_weighted_GdE_1", "description": "Pseudo-EPAM high-dynamic-range differential electron flux as function of energy. Averages of STIS fluxes whose midpoint energies lie within the EPAM channel energy edges, weighted by the spectral responses (GdE) of each STIS channel.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_flux_epam_weighted_GdE_2", "description": "Pseudo-EPAM high-dynamic-range differential electron flux as function of energy. Averages of STIS fluxes whose midpoint energies lie within the EPAM channel energy edges, weighted by the spectral responses (GdE) of each STIS channel.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_flux_epam_weighted_GdE_3", "description": "Pseudo-EPAM high-dynamic-range differential electron flux as function of energy. Averages of STIS fluxes whose midpoint energies lie within the EPAM channel energy edges, weighted by the spectral responses (GdE) of each STIS channel.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_flux_epam_weighted_GdE_uncert_0", "description": "Poisson uncertainty of 'electron_flux_epam_weighted_GdE' as function of energy.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_flux_epam_weighted_GdE_uncert_1", "description": "Poisson uncertainty of 'electron_flux_epam_weighted_GdE' as function of energy.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_flux_epam_weighted_GdE_uncert_2", "description": "Poisson uncertainty of 'electron_flux_epam_weighted_GdE' as function of energy.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "electron_flux_epam_weighted_GdE_uncert_3", "description": "Poisson uncertainty of 'electron_flux_epam_weighted_GdE' as function of energy.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_0_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_0_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_1_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_1_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_2_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_2_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_3_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_3_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_4_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_4_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_5_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_5_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_6_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_6_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_7_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_epam_7_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected for dead time but not for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_0_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_0_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_1_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_1_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_2_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_2_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_3_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_3_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_4_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_4_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_5_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_5_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_6_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_6_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_7_0", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_counts_raw_epam_7_1", "description": "Spectrally-summed counts in the pseudo-EPAM ion channels, for each front detector - small and large. Corrected neither for dead time nor for contamination.", "units": "counts", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_0_0", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_0_1", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_1_0", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_1_1", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_2_0", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_2_1", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_3_0", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_3_1", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_4_0", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_4_1", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_5_0", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_5_1", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_6_0", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_6_1", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_7_0", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_edges_epam_7_1", "description": "Edges of pseudo-EPAM ion energy bins. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_epam_weighted_GdE_0", "description": "Average of midpoint energies of STIS ion channels comprising the pseudo-EPAM channel, weighted by the spectral responses (GdE) of each STIS channel. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_epam_weighted_GdE_1", "description": "Average of midpoint energies of STIS ion channels comprising the pseudo-EPAM channel, weighted by the spectral responses (GdE) of each STIS channel. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_epam_weighted_GdE_2", "description": "Average of midpoint energies of STIS ion channels comprising the pseudo-EPAM channel, weighted by the spectral responses (GdE) of each STIS channel. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_epam_weighted_GdE_3", "description": "Average of midpoint energies of STIS ion channels comprising the pseudo-EPAM channel, weighted by the spectral responses (GdE) of each STIS channel. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_epam_weighted_GdE_4", "description": "Average of midpoint energies of STIS ion channels comprising the pseudo-EPAM channel, weighted by the spectral responses (GdE) of each STIS channel. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_epam_weighted_GdE_5", "description": "Average of midpoint energies of STIS ion channels comprising the pseudo-EPAM channel, weighted by the spectral responses (GdE) of each STIS channel. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_epam_weighted_GdE_6", "description": "Average of midpoint energies of STIS ion channels comprising the pseudo-EPAM channel, weighted by the spectral responses (GdE) of each STIS channel. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_energy_epam_weighted_GdE_7", "description": "Average of midpoint energies of STIS ion channels comprising the pseudo-EPAM channel, weighted by the spectral responses (GdE) of each STIS channel. Will not change unless STIS L1b channel set changes.", "units": "keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_0", "description": "Pseudo-EPAM high-dynamic-range differential ion flux as function of energy. Averages of STIS fluxes whose midpoint energies lie within the EPAM channel energy edges, weighted by the spectral responses (GdE) of each STIS channel.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_1", "description": "Pseudo-EPAM high-dynamic-range differential ion flux as function of energy. Averages of STIS fluxes whose midpoint energies lie within the EPAM channel energy edges, weighted by the spectral responses (GdE) of each STIS channel.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_2", "description": "Pseudo-EPAM high-dynamic-range differential ion flux as function of energy. Averages of STIS fluxes whose midpoint energies lie within the EPAM channel energy edges, weighted by the spectral responses (GdE) of each STIS channel.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_3", "description": "Pseudo-EPAM high-dynamic-range differential ion flux as function of energy. Averages of STIS fluxes whose midpoint energies lie within the EPAM channel energy edges, weighted by the spectral responses (GdE) of each STIS channel.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_4", "description": "Pseudo-EPAM high-dynamic-range differential ion flux as function of energy. Averages of STIS fluxes whose midpoint energies lie within the EPAM channel energy edges, weighted by the spectral responses (GdE) of each STIS channel.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_5", "description": "Pseudo-EPAM high-dynamic-range differential ion flux as function of energy. Averages of STIS fluxes whose midpoint energies lie within the EPAM channel energy edges, weighted by the spectral responses (GdE) of each STIS channel.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_6", "description": "Pseudo-EPAM high-dynamic-range differential ion flux as function of energy. Averages of STIS fluxes whose midpoint energies lie within the EPAM channel energy edges, weighted by the spectral responses (GdE) of each STIS channel.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_7", "description": "Pseudo-EPAM high-dynamic-range differential ion flux as function of energy. Averages of STIS fluxes whose midpoint energies lie within the EPAM channel energy edges, weighted by the spectral responses (GdE) of each STIS channel.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_uncert_0", "description": "Poisson uncertainty of 'ion_flux_epam_weighted_GdE' as function of energy.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_uncert_1", "description": "Poisson uncertainty of 'ion_flux_epam_weighted_GdE' as function of energy.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_uncert_2", "description": "Poisson uncertainty of 'ion_flux_epam_weighted_GdE' as function of energy.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_uncert_3", "description": "Poisson uncertainty of 'ion_flux_epam_weighted_GdE' as function of energy.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_uncert_4", "description": "Poisson uncertainty of 'ion_flux_epam_weighted_GdE' as function of energy.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_uncert_5", "description": "Poisson uncertainty of 'ion_flux_epam_weighted_GdE' as function of energy.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_uncert_6", "description": "Poisson uncertainty of 'ion_flux_epam_weighted_GdE' as function of energy.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "ion_flux_epam_weighted_GdE_uncert_7", "description": "Poisson uncertainty of 'ion_flux_epam_weighted_GdE' as function of energy.", "units": "particles/cm^2-s-sr-keV", "fill": "-1e+31", "type": "double" }, { "name": "quality_flags", "description": "Quality flag (bit-wise, 64 bits). The first bit indicates whether the data are real-time or replayed. The next 31 bits are data quality flags originating in the instrument. The next 31 bits are data quality flags originating in the spacecraft. The case of all bits = 1 is reserved for the fill value. L0b flag: Bit 0: 0 = real-time data, 1 = data extracted from playback. L1a flags: Bits 1-6: Pulser 1-6 enabled; 7-12: Chan 1-6 noise sigma exceed criteria; 13: Any detector disabled, 14-17: Decimation active in Chan 2, 3, 5, 6; 18-23: Chan 1-6 count rates exceed criteria; 24: One or more instrument temperatures exceed criteria; 25: Non-standard configuration; 32-35: Reaction wheel (RW) speeds exceed criteria; 38: Any inertial reference unit (IRU) is invalid; 39: spacecraft off-pointing, 40: Sun in STIS FOV. L1b flags - 26-27: Ion pixel merging is suspect, likely due to excessive noise in small or large pixel; 28-29: Electron pixel merging is suspect, likely due to excessive noise in small or large pixel; 30: Electron contamination of ion fluxes is significant", "units": "unitless", "fill": "18446744073709551615", "type": "integer" }, { "name": "time_met", "description": "Mission elapsed time since 1958-01-01/00:00. Corrected periodically on-board for spacecraft clock drift.", "units": "microseconds since 1958-01-01T00:00:00.00Z", "fill": "-1e+31", "type": "double" }, { "name": "time_unix", "description": "Unix time (elapsed seconds since 1970-01-01/00:00) for this data record", "units": "seconds since 1970-01-01T00:00:00.00Z", "fill": "-1e+31", "type": "double" } ], "additionalMetadata": [ { "name": "Parameter Extended Metadata", "content": { "accum_time": { "long_name": "accumulations_per_sample", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_epam_0_0": { "long_name": "counts_electron_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_epam_0_1": { "long_name": "counts_electron_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_epam_1_0": { "long_name": "counts_electron_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_epam_1_1": { "long_name": "counts_electron_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_epam_2_0": { "long_name": "counts_electron_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_epam_2_1": { "long_name": "counts_electron_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_epam_3_0": { "long_name": "counts_electron_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_epam_3_1": { "long_name": "counts_electron_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_raw_epam_0_0": { "long_name": "counts_electron_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_raw_epam_0_1": { "long_name": "counts_electron_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_raw_epam_1_0": { "long_name": "counts_electron_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_raw_epam_1_1": { "long_name": "counts_electron_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_raw_epam_2_0": { "long_name": "counts_electron_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_raw_epam_2_1": { "long_name": "counts_electron_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_raw_epam_3_0": { "long_name": "counts_electron_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_counts_raw_epam_3_1": { "long_name": "counts_electron_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_energy_edges_epam_0_0": { "long_name": "electron_epam_band_energy_width", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_energy_edges_epam_0_1": { "long_name": "electron_epam_band_energy_width", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_energy_edges_epam_1_0": { "long_name": "electron_epam_band_energy_width", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_energy_edges_epam_1_1": { "long_name": "electron_epam_band_energy_width", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_energy_edges_epam_2_0": { "long_name": "electron_epam_band_energy_width", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_energy_edges_epam_2_1": { "long_name": "electron_epam_band_energy_width", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_energy_edges_epam_3_0": { "long_name": "electron_epam_band_energy_width", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_energy_edges_epam_3_1": { "long_name": "electron_epam_band_energy_width", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_energy_epam_weighted_GdE_0": { "long_name": "electron_epam_band_averaged_energy_weighted_by_spectral_response", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_energy_epam_weighted_GdE_1": { "long_name": "electron_epam_band_averaged_energy_weighted_by_spectral_response", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_energy_epam_weighted_GdE_2": { "long_name": "electron_epam_band_averaged_energy_weighted_by_spectral_response", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_energy_epam_weighted_GdE_3": { "long_name": "electron_epam_band_averaged_energy_weighted_by_spectral_response", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_flux_epam_weighted_GdE_0": { "long_name": "flux_electron_differential_unidirectional_weighted_by_spectral_response", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_flux_epam_weighted_GdE_1": { "long_name": "flux_electron_differential_unidirectional_weighted_by_spectral_response", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_flux_epam_weighted_GdE_2": { "long_name": "flux_electron_differential_unidirectional_weighted_by_spectral_response", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_flux_epam_weighted_GdE_3": { "long_name": "flux_electron_differential_unidirectional_weighted_by_spectral_response", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_flux_epam_weighted_GdE_uncert_0": { "long_name": "poisson_uncertainty_flux_electron_differential_unidirectional_weighted_by_spectral_response", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_flux_epam_weighted_GdE_uncert_1": { "long_name": "poisson_uncertainty_flux_electron_differential_unidirectional_weighted_by_spectral_response", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_flux_epam_weighted_GdE_uncert_2": { "long_name": "poisson_uncertainty_flux_electron_differential_unidirectional_weighted_by_spectral_response", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "electron_flux_epam_weighted_GdE_uncert_3": { "long_name": "poisson_uncertainty_flux_electron_differential_unidirectional_weighted_by_spectral_response", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_0_0": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_0_1": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_1_0": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_1_1": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_2_0": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_2_1": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_3_0": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_3_1": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_4_0": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_4_1": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_5_0": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_5_1": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_6_0": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_6_1": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_7_0": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_epam_7_1": { "long_name": "counts_ion_epam_dead_time_corrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_0_0": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_0_1": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_1_0": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_1_1": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_2_0": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_2_1": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_3_0": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_3_1": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_4_0": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_4_1": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_5_0": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_5_1": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_6_0": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_6_1": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_7_0": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_counts_raw_epam_7_1": { "long_name": "counts_ion_epam_uncorrected", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_energy_edges_epam_0_0": { "long_name": "ion_epam_band_edge_energies", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_energy_edges_epam_0_1": { "long_name": "ion_epam_band_edge_energies", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_energy_edges_epam_1_0": { "long_name": "ion_epam_band_edge_energies", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_energy_edges_epam_1_1": { "long_name": "ion_epam_band_edge_energies", "product": "sci_stis-l2_solar1", "instrument": "STIS", "satellite": "SOLAR-1" }, "ion_energy_edges_epam_2_0": { "long_name": "ion_epam_band_edge_energies", "product": "sci_stis-l2_solar1", 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