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Ulysses Cosmic Ray and Solar Particle Investigation (COSPIN) High Energy Telescope (HET) Full Resolution Heavy Ion Counts and Accumulation Times for Spin-Averaged Coincidence Counting Rates, OMNI2 H10-H27, 128 s Data

ResourceID
spase://NASA/NumericalData/Ulysses/COSPIN/HET/Rates/Omni2/PT128S

Description
A Directory containing Daily FTP downloadable Files containing Readout-by-Readout Listings of the Counts accumulated in the H1-H27 Spin-Averaged Counting Rates. The Rates H10-H13 are Coincidence Counting Rates corresponding primarily to Heavy Nuclei (Z>2) with Penetrating Power equivalent to Carbon-12 Nuclei in the approximate Energy Ranges 26-36, 44-127, 127-173, and >173 MeV/n, respectively. H14-H27 are single Detector Counting Rates giving, in order, the total Number of Counts above the lowest level Discriminator Thresholds of Detectors D1-D6, K1-K6 (or D7-D12), A (or D13), and the Anti-Coincidence Scintillator S. The single Detector Counting Rates are provided simply to assess the Health of the Detectors and are of little use scientifically. The Naming Convention for the Daily Files is uly_het_full_rat_omni2_YYYDDD.txt, where YYY indicates the three digit Year since 1900 (e.g. YYY=090 for 1990, and YYY=102 for 2002) and DDD indicates the three digit Day of Year (January 1 = 1). In each File, following a detailed Description of the Format, the Data consist of a Listing of Counts accumulated in the H10-H27 Spin-Averaged Counting Rates during the Intervals between successive Readouts, organized into Columns as described below. The first four Columns give the Start Time of the Counting Rate Accumulation Period as Fractional Year (to 12 Decimal Places) and as Year since 1900, Day of Year, and Milliseconds of Day at the Start of the Accumulation, followed by one Column giving the Duration of the Accumulation Period in Milliseconds (it is the same for all Rates except H13, which is read out twice in each Accumulation Period, and is thus represented as H13a and H13b, see below and embedded Documentation in each Daily File), and 19 Columns giving the Counts accumulated in that Period for each Rate. All Fields except for the Fractional Year are in Integer Format. The Start Time for H13a is the Time given as the Start Time for the Line, but (to sufficient accuracy) its Accumulation Period is half the Period given under "Coverage". Again, to sufficient accuracy, the Start Time for H13b is the Time given plus half the Accumulation Period, and the Accumulation Period for H13b is half the Period given under "Coverage". Each Line contains Data for one single Readout of the Rates H10-H12, H13a, H13b, and H14-H27. All Readouts where at least one of the Rates has a Non-fill Value are included. Where Fill does occur it is indicated by -1. Since the Accumulation Period for each Readout is forced to include an Integral Number of Spacecraft Spins in order to produce pure Spin-Averaged Measurements, the Lengths of the Accumulation Periods vary in a Cyclic Manner as the Period of the Telemetry Cycle beats with the Spacecraft Spin Period. At the most common Science Telemetry Rate, 2048 bps, each Rate in this File is Readout on average once every 128 s, except for H13 which is Readout on average twice in every 128 s. At 2048 bps, the Cycle of Accumulation Periods is 132, 132, 120, 132, 132,, 120, 132, etc., seconds. No Noise Removal or Despiking has been done, so Caution must be used in interpreting isolated large Increases or Decreases in the Counting Rates.

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NumericalData

ResourceID
spase://NASA/NumericalData/Ulysses/COSPIN/HET/Rates/Omni2/PT128S
ResourceHeader
ResourceName
Ulysses Cosmic Ray and Solar Particle Investigation (COSPIN) High Energy Telescope (HET) Full Resolution Heavy Ion Counts and Accumulation Times for Spin-Averaged Coincidence Counting Rates, OMNI2 H10-H27, 128 s Data
ReleaseDate
2020-07-07 21:15:40Z
Description
A Directory containing Daily FTP downloadable Files containing Readout-by-Readout Listings of the Counts accumulated in the H1-H27 Spin-Averaged Counting Rates. The Rates H10-H13 are Coincidence Counting Rates corresponding primarily to Heavy Nuclei (Z>2) with Penetrating Power equivalent to Carbon-12 Nuclei in the approximate Energy Ranges 26-36, 44-127, 127-173, and >173 MeV/n, respectively. H14-H27 are single Detector Counting Rates giving, in order, the total Number of Counts above the lowest level Discriminator Thresholds of Detectors D1-D6, K1-K6 (or D7-D12), A (or D13), and the Anti-Coincidence Scintillator S. The single Detector Counting Rates are provided simply to assess the Health of the Detectors and are of little use scientifically. The Naming Convention for the Daily Files is uly_het_full_rat_omni2_YYYDDD.txt, where YYY indicates the three digit Year since 1900 (e.g. YYY=090 for 1990, and YYY=102 for 2002) and DDD indicates the three digit Day of Year (January 1 = 1). In each File, following a detailed Description of the Format, the Data consist of a Listing of Counts accumulated in the H10-H27 Spin-Averaged Counting Rates during the Intervals between successive Readouts, organized into Columns as described below. The first four Columns give the Start Time of the Counting Rate Accumulation Period as Fractional Year (to 12 Decimal Places) and as Year since 1900, Day of Year, and Milliseconds of Day at the Start of the Accumulation, followed by one Column giving the Duration of the Accumulation Period in Milliseconds (it is the same for all Rates except H13, which is read out twice in each Accumulation Period, and is thus represented as H13a and H13b, see below and embedded Documentation in each Daily File), and 19 Columns giving the Counts accumulated in that Period for each Rate. All Fields except for the Fractional Year are in Integer Format. The Start Time for H13a is the Time given as the Start Time for the Line, but (to sufficient accuracy) its Accumulation Period is half the Period given under "Coverage". Again, to sufficient accuracy, the Start Time for H13b is the Time given plus half the Accumulation Period, and the Accumulation Period for H13b is half the Period given under "Coverage". Each Line contains Data for one single Readout of the Rates H10-H12, H13a, H13b, and H14-H27. All Readouts where at least one of the Rates has a Non-fill Value are included. Where Fill does occur it is indicated by -1. Since the Accumulation Period for each Readout is forced to include an Integral Number of Spacecraft Spins in order to produce pure Spin-Averaged Measurements, the Lengths of the Accumulation Periods vary in a Cyclic Manner as the Period of the Telemetry Cycle beats with the Spacecraft Spin Period. At the most common Science Telemetry Rate, 2048 bps, each Rate in this File is Readout on average once every 128 s, except for H13 which is Readout on average twice in every 128 s. At 2048 bps, the Cycle of Accumulation Periods is 132, 132, 120, 132, 132,, 120, 132, etc., seconds. No Noise Removal or Despiking has been done, so Caution must be used in interpreting isolated large Increases or Decreases in the Counting Rates.
Acknowledgement
Please acknowledge the COSPIN HET Lead Investigator and COSPIN PI, R. Bruce McKibben
Contacts
Role Person StartDate StopDate Note
1. PrincipalInvestigator
TeamLeader
spase://SMWG/Person/R.Bruce.McKibben
2. DataProducer spase://SMWG/Person/Clifford.Lopate
3. CoInvestigator spase://SMWG/Person/James.Connell

InformationURL
Name
The Ulysses Cosmic Ray and Solar Particle Investigation, COSPIN
URL
Description
Published Description of the COSPIN Instrumentation, J.A. Simpson et al., Astron. Astrophys. Suppl. Ser. 92, 365-399, 1992. See especially Section 4.3 for a detailed Description of the High Energy Telescopes, HET. An electronic Copy of this Paper is available at http://adsbit.harvard.edu/cgi-bin/nph-iarticle_query?1992A%26AS...92..365S&defaultprint=YES&filetype=.pdf.
InformationURL
Name
User Notes for the COSPIN/HET Data Files
URL
Description
The User Notes File at the Ulysses Final Archive (UFA) describes the Format of the ASCII Data Files for the COSPIN High Energy Telescope, HET
InformationURL
Name
COSPIN HET Full Resolution ReadMe Document, Word Format
URL
Description
Top Level Descriptions of Formats and Contents of the six File Types that make up the COSPIN HET Full Resolution Data Set. Detailed Descriptions of the Formats and Contents are found in Header Lines at the Start of each downloaded Data File. The Data covered by this SPASE Description are described in the ReadMe under the Heading omni2. (*** Note ***: During the Build-up of this Data Set, a few Errors and Omissions have been found in the Header Lines for some of the File Types. These Errors and Omissions are listed in this ReadMe File. Upon Completion of the Data Set, all Errors and Omissions discovered will be corrected in all of the Header Lines of all of the File Types at which time this Note will be removed).
Association
Association
Association
PriorIDs
spase://VEPO/NumericalData/Ulysses/COSPIN/HET/FullResolution/Rates/Omni2
spase://VSPO/NumericalData/Ulysses/COSPIN/HET/Rates/Omni2/PT128S
AccessInformation
RepositoryID
Availability
Online
AccessRights
Open
AccessURL
Name
Ulysses Final Archive Access to COSPIN/HET Full Resolution Heavy Ion Counts and Accumulation Times for Spin-Averaged Coincidence Counting Rates, OMNI2 H10-H27
URL
Description
Parent Directory containing FTP downloadable Daily Files with the Format described below
Format
Text
Encoding
ASCII
Acknowledgement
Please acknowledge R. Bruce McKibben, Space Science Center, University of New Hampshire
InstrumentIDs
MeasurementType
EnergeticParticles
TemporalDescription
TimeSpan
StartDate
1990-10-22 00:00:00.000
StopDate
2009-06-29 23:59:59.999
Cadence
PT128S
ObservedRegion
Heliosphere.Outer
Parameter #1
Name
Interval Start Time
Description
Nominal Start Time for the average given in decimal year, integer year, Day of Year, and Milliseconds of Day.
Cadence
PT128S
Structure
Size
4
Element
Name
Decimal Year
Index
1
ParameterKey
Column_1
ValidMin
1990
ValidMax
2009
FillValue
0.00000000000
Element
Name
Year
Index
2
ParameterKey
Column_2
ValidMin
1990
ValidMax
2009
FillValue
0
Element
Name
Day of Year
Index
3
ParameterKey
Column_3
ValidMin
1
ValidMax
366
FillValue
0
Element
Name
Milliseconds of Day
Index
4
ParameterKey
Column_4
ValidMin
0
ValidMax
86400000
FillValue
0
Support
SupportQuantity
Temporal
Parameter #2
Name
Accumulation period
ParameterKey
Column_5
Description
Length of the accumulation period in milli-seconds.
Caveats
None
Cadence
PT128S
Units
millisecond
ValidMin
100000
ValidMax
1200000
FillValue
0
Support
SupportQuantity
Temporal
Parameter #3
Name
COSPIN/HET H10
ParameterKey
Column_6
Description
Counts accumulated by counting rate H10 during the period of coverage (column 5) starting at the time defined in columns 1-4. The H10 counting rate normally responds primarily to nuclei with Z>2 with penetrating power equivalent to 26-36 MeV/n Carbon-12 nuclei. Protons, helium nuclei, and electrons are excluded by discriminators requiring an energy deposit in at least one detector greater than can be produced by a Z=2 nucleus.
Caveats
The energy range given above and below is appropriate only for Carbon-12 nuclei
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
26
High
36
Units
MeV/n
Parameter #4
Name
COSPIN/HET H11
ParameterKey
Column_7
Description
Counts accumulated by counting rate H11 during the period of coverage (column 5) starting at the time defined in columns 1-4. The H11 counting rate normally responds primarily to nuclei with Z>2 with penetrating power equivalent to 44-127 MeV/n Carbon-12 nuclei. Protons, helium nuclei, and electrons are excluded by discriminators requiring an energy deposit in at least one detector greater than can be produced by a Z=2 nucleus.
Caveats
The energy range given below is appropriate only for Carbon-12 nuclei
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
44
High
127
Units
MeV/n
Parameter #5
Name
COSPIN/HET H12
ParameterKey
Column_8
Description
Counts accumulated by counting rate H12 during the period of coverage (column 5) starting at the time defined in columns 1-4. The H12 counting rate normally responds primarily to nuclei with Z>2 with penetrating power equivalent to 127-173 MeV/n Carbon-12 nuclei. Protons, helium nuclei, and electrons are excluded by discriminators requiring an energy deposit in at least one detector greater than can be produced by a Z=2 nucleus.
Caveats
The energy range given below is appropriate only for Carbon-12 nuclei. The H12 counting rate has a bit rate dependence which is not fully understood. It is most clear during solar particle events when the H12 rate is elevated above its normally very low background rate. Also, during In-Flight-Calibrate (IFC) sequences, which over several hours (depending on telemetry bit rate) feed two ramps of pulses to the detector amplifiers, the H12 counts counts all of the IFC pulses that have sufficient amplitude to exceed the high level discriminators used to exclude protons and helium from being counted by H12. Most of the IFC pulses do exceed the levels necessary to trigger these discriminators, so that the H12 counting rate is dramatically elevated for a period of several hours when the IFC sequence is performed. A particularly clear example of both effects can be found in days 83-86 of 1991, when an IFC sequence is performed on day 86 in the tail of a solar particle event that began at the very end of day 83. As a result of these effects, the H12 counting rate should not be used to determine accurate particle flux levels.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
127
High
173
Units
MeV/n
Parameter #6
Name
COSPIN/HET H13a
ParameterKey
Column_9
Description
Counts accumulated by counting rate H13a during the first half of the period of coverage (column 5) starting at the time defined in columns 1-4. The H13a counting rate normally responds primarily to nuclei with Z>2 with penetrating power equivalent to Carbon-12 nuclei with energies greater than 173 MeV/n. Such nuclei completely penetrate the telescope. Therefore, the H13 is also sensitive, above a poorly known energy threshold, to nuclei going backward through the HET after penetrating the spacecraft structures and other instruments that lie behind the HET on the spacecraft. Protons, helium nuclei, and electrons are excluded by discriminators requiring an energy deposit in at least one detector greater than can be produced by a Z=2 nucleus.
Caveats
The energy range given below is appropriate only for Carbon-12 nuclei
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
173
High
1.0E+14
Units
MeV/n
Parameter #7
Name
COSPIN/HET H13b
ParameterKey
Column_10
Description
H13b is identical to H13a except that it accumulates counts during the second half of the period of coverage (column 5) starting at the time defined in columns 1-4. Thus the start time for the H13b accumulation is the time in columns 1-4 plus half coverage interval listed in column 5. All other considerations described for H13a apply equally to H13b.
Caveats
The energy range given below is appropriate only for Carbon-12 nuclei
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
173
High
1.0E+14
Units
MeV/n
Parameter #8
Name
COSPIN/HET H14
ParameterKey
Column_11
Description
H14 registers the total number of counts above the lowest level threshold in detector D1 of the HET during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV
Parameter #9
Name
COSPIN/HET H15
ParameterKey
Column_12
Description
H15 registers the total number of counts above the lowest level threshold in detector D2 of the HET during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV
Parameter #10
Name
COSPIN/HET H16
ParameterKey
Column_13
Description
H16 registers the total number of counts above the lowest level threshold in detector D3 of the HET during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV
Parameter #11
Name
COSPIN/HET H17
ParameterKey
Column_14
Description
H17 registers the total number of counts above the lowest level threshold in detector D4 of the HET during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV
Parameter #12
Name
COSPIN/HET H18
ParameterKey
Column_15
Description
H18 registers the total number of counts above the lowest level threshold in detector D5 of the HET during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV
Parameter #13
Name
COSPIN/HET H19
ParameterKey
Column_16
Description
H19 registers the total number of counts above the lowest level threshold in detector D6 of the HET during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV
Parameter #14
Name
COSPIN/HET H20
ParameterKey
Column_17
Description
H20 registers the total number of counts above the lowest level threshold in detector K1 (D7) of the HET during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV
Parameter #15
Name
COSPIN/HET H21
ParameterKey
Column_18
Description
H21 registers the total number of counts above the lowest level threshold in detector K2 (D8) of the HET during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV
Parameter #16
Name
COSPIN/HET H22
ParameterKey
Column_19
Description
H22 registers the total number of counts above the lowest level threshold in detector K3 (D9) of the HET during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV
Parameter #17
Name
COSPIN/HET H23
ParameterKey
Column_20
Description
H23 registers the total number of counts above the lowest level threshold in detector K4 (D10) of the HET during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV
Parameter #18
Name
COSPIN/HET H24
ParameterKey
Column_21
Description
H24 registers the total number of counts above the lowest level threshold in detector K5 (D11) of the HET during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV
Parameter #19
Name
COSPIN/HET H25
ParameterKey
Column_22
Description
H25 registers the total number of counts above the lowest level threshold in detector K6 (D12) of the HET during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV
Parameter #20
Name
COSPIN/HET H26
ParameterKey
Column_23
Description
H26 registers the total number of counts above threshold in detector A (D13) of the HET during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV
Parameter #21
Name
COSPIN/HET H27
ParameterKey
Column_24
Description
H27 registers the total number of counts above threshold in the Anti-Coincidence plastic scintillator, S, that surrounds the HET detector stack during the accumulation period (column 5) starting at the time defined in columns 1-4. No coincidence conditions are applied, so no particle identification can be made, nor can any energy range be defined other than that the particle (or gamma ray) must be able to reach the detector either through the telescope aperture and overlying detector stack, or through the side of the telescope and any spacecraft or instrument structure in its path. Consequently, the counting rate is most often dominated by high energy cosmic rays and by electrons produced by Gamma Rays in the telescope.
Caveats
The minimum energy given below is accurate only to order of magnitude.
Cadence
PT128S
ValidMin
0.0
ValidMax
1000000
FillValue
-1
Particle
ParticleType
Ion
ParticleQuantity
Counts
EnergyRange
Low
1
High
1.0E+14
Units
MeV