{
  "startDate": "2026-09-27T00:00:00Z",
  "stopDate": "2026-10-10T23:59:00Z",
  "cadence": "PT1M",
  "description": "Magnetic Field 1 minute<br/> Sampling: 1M<br/> Provider: NOAA NCEI",
  "resourceID": "spase://CNES/NumericalData/CDPP-AMDA/SOLAR-1/STIS/so1-stis-l3.1mntbc",
  "parameters": [
    {
      "name": "Time",
      "type": "isotime",
      "length": 24,
      "units": "UTC",
      "fill": null
    },
    {
      "name": "so1_stis_l3_iflux",
      "type": "double",
      "size": [
        48
      ],
      "units": "particles/cm²-s-sr-keV",
      "fill": "-1e31",
      "description": "Time-average of differential ion flux as function of energy, for each front detector - small and large. Corrected for dead time. Not corrected for contamination."
    },
    {
      "name": "so1_stis_l3_ifluxhdr",
      "type": "double",
      "size": [
        48
      ],
      "units": "particles/cm²-s-sr-keV",
      "fill": "-1e31",
      "description": "Time-average of high-dynamic-range differential ion flux as function of energy, a linear combination of fluxes from the small and large front detectors.  Corrected for dead time. Not corrected for contamination."
    },
    {
      "name": "so1_stis_l3_o1fraction",
      "type": "double",
      "units": "",
      "fill": "-1e31",
      "description": "Fraction of 'ion flux high-dynamic-range' that comes from small pixel (O1).  Value is between 0 and 1.  The small pixel flux is multiplied by this value, and the large pixel flux is multiplied by 1 minus this value, when calculating 'ion flux high-dynamic-range'."
    },
    {
      "name": "so1_stis_l3_eflux",
      "type": "double",
      "size": [
        48
      ],
      "units": "particles/cm²-s-sr-keV",
      "fill": "-1e31",
      "description": "Time-average of differential electron flux as function of energy, for each front detector - small and large. Corrected for dead time. Not corrected for contamination."
    },
    {
      "name": "so1_stis_l3_efluxhdr",
      "type": "double",
      "size": [
        48
      ],
      "units": "particles/cm²-s-sr-keV",
      "fill": "-1e31",
      "description": "Time-average of high-dynamic-range differential electron flux as function of energy, a linear combination of fluxes from the small and large front detectors.  Corrected for dead time. Not corrected for contamination."
    },
    {
      "name": "so1_stis_l3_f1fraction",
      "type": "double",
      "units": "",
      "fill": "-1e31",
      "description": "Fraction of 'e- flux high-dynamic-range' that comes from small pixel (F1).  Value is between 0 and 1.  The small pixel flux is multiplied by this value, and the large pixel flux is multiplied by 1 minus this value, when calculating 'e- flux high-dynamic-range'."
    }
  ],
  "HAPI": "2.0",
  "status": {
    "code": 1200,
    "message": "OK"
  },
  "x_LastUpdate": "2026-10-17T15:09:32Z"
}