Nominal Start Time for the average given in year, day of year, hour, min, second.

Size

5

Elements

Index	Name	Valid min	Valid max	Fill value
1	Year	1990	2009	Null
2	Day of year	1	366	Null
3	Hour of day	0	23	Null
4	Minute of hour	0	59	Null
5	Seconds of minute	0	59	Null

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(0) responding primarily to 0.7-0.9 MeV protons. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.28 MeV proton will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.28

High energy

7.0

Units

MeV

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(1) responding primarily to 0.50-2.27 MeV protons. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.50 MeV proton will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.50

High energy

2.27

Units

MeV

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(2) responding primarily to 0.76-1.37 MeV protons. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.76 MeV proton will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.76

High energy

1.37

Units

MeV

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(3) responding primarily to 0.31-5.4 MeV/n Helium nuclei. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.31 MeV/n Helium nucleus (alpha particle) will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.31

High energy

5.4

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(4) responding primarily to 0.38-3.9 MeV/n Helium nuclei. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.38 MeV/n Helium nucleus (alpha particle) will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.38

High energy

3.9

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(5) responding primarily to 0.45-2.9 MeV/n Helium nuclei. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.45 MeV/n Helium nucleus (alpha particle) will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.45

High energy

2.9

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(6) responding primarily to 0.51-2.26 MeV/n Helium nuclei. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.51 MeV/n Helium nucleus (alpha particle) will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.51

High energy

2.26

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(7) responding primarily to 0.58-1.91 MeV/n Helium nuclei. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.58 MeV/n Helium nucleus (alpha particle) will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.58

High energy

1.91

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(8) responding primarily to 0.64-1.66 MeV/n Helium nuclei. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.64 MeV/n Helium nucleus (alpha particle) will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.64

High energy

1.66

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(9) responding primarily to 0.71-1.50 MeV/n Helium nuclei. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.71 MeV/n Helium nucleus (alpha particle) will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.71

High energy

1.50

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(10) responding primarily to 0.78-1.35 MeV/n Helium nuclei. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.78 MeV/n Helium nucleus (alpha particle) will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.78

High energy

1.35

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(11) responding primarily to 0.85-1.25 MeV/n Helium nuclei. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.85 MeV/n Helium nucleus (alpha particle) will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.85

High energy

1.25

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(12) responding primarily to 0.91-1.17 MeV/n Helium nuclei. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.85 MeV/n Helium nucleus (alpha particle) will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.91

High energy

1.17

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(13) responding primarily to 0.98-1.12 MeV/n Helium nuclei. This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.98 MeV/n Helium nucleus (alpha particle) will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.98

High energy

1.12

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(14) responding primarily to heavy nuclei (0.34-29.6 MeV/n for Oxygen) . This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.34 MeV/n Oxygen nucleus will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.34

High energy

29.6

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F1J(15) responding primarily to heavy nuclei (0.36-27.4 MeV/n for Oxygen) . This flux represents one step in a 16 step sequence of discriminator levels. The step is identified in the rate name, where J(x) implies step x. In the most common operational mode the discriminator level advances one step with each readout of F1 (16 seconds at 1024 bps). Each complete cycle thus takes 256 seconds (at 1024 bps).

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.36 MeV/n Oxygen nucleus will also contribute to this flux. The total accumulation interval for this rate is much less than the 10 minute nominal interval since it represents one step in a 16-step sequence of discriminator levels.

Low energy

0.36

High energy

27.4

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F2L responding primarily to 0.20-6.7 MeV protons. This discriminator level corresponding to this flux is set to L or H by command. If the level is set to H, this field will be fill.

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.20 MeV proton will also contribute to this flux.

Low energy

0.20

High energy

6.7

Units

MeV

Nominal 10-minute average HFT spin-averaged flux based on counting rate F2H responding primarily to 0.55-1.95 MeV protons. This discriminator level corresponding to this flux is set to L or H by command. If the level is set to L, this field will be fill.

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.55 MeV proton will also contribute to this flux.

Low energy

0.55

High energy

1.95

Units

MeV

Nominal 10-minute average HFT spin-averaged flux based on counting rate F3 responding primarily to 0.68-1.56 MeV/n (for He) Z>=2 nuclei.

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.68 MeV/n helium nucleus will also contribute to this flux.

Low energy

0.68

High energy

1.56

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F4 responding primarily to 0.8-4.9 MeV/n (for He) Z>=2 nuclei.

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.8 MeV/n Carbon nucleus will also contribute to this flux.

Low energy

0.8

High energy

4.9

Units

MeV/n

Nominal 10-minute average HFT spin-averaged flux based on counting rate F3 responding primarily to 1.28-8.5MeV/n (for Sulphur) Z>=12 nuclei.

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 1.28 MeV/n Sulphur nucleus will also contribute to this flux.

Low energy

1.28

High energy

8.5

Units

MeV/n

Nominal 10-minute average HFT spin-averaged fluxes based on counting rate F2s, which split directionality of the F2 fluxes using 32 spin sectors. The counting rate responds primarily to protons in the energy ranges 0.29-6.7 MeV or 0.55-1.95 MeV, depending on whether the F2 threshold is set low or high respectively. The state of the F2 threshold is low if column 23 contains fill, and high if column 22 contains fill. See Anglin et al. , J. Geophys. Res., 102, 1, 1997 for more detailed discussion of using the HFT F2S sectored rate.

Since the energy range is defined entirely by a discriminator level on the single 18 micron thick silicon detector, other high energy nuclei with energy losses in the detector greater than that of a normally incident 0.29 or 0.55 MeV proton (depending on the state of the F2 discriminator) will also contribute to these fluxes. Since the total accumulation time in each sector is less than 20 seconds in the nominal 10 minute averaging period, statistical accuracy of these sectored fluxes in a single averaging interval is usually poor except in large flux enhancements, most commonly produced by large solar energetic particle events, but also by the high radiation levels in Jupiter's magnetosphere.

Size

32

Elements

Index	Name	Units	Valid min	Valid max	Fill value
1	F2S1	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
2	F2S2	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
3	F2S3	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
4	F2S4	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
5	F2S5	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
6	F2S6	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
7	F2S7	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
8	F2S8	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
9	F2S9	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
10	F2S10	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
11	F2S11	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
12	F2S12	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
13	F2S13	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
14	F2S14	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
15	F2S15	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
16	F2S16	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
17	F2S17	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
18	F2S18	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
19	F2S19	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
20	F2S20	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
21	F2S21	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
22	F2S22	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
23	F2S23	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
24	F2S24	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
25	F2S25	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
26	F2S26	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
27	F2S27	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
28	F2S28	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
29	F2S29	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
30	F2S30	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
31	F2S31	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999
32	F2S32	(counts/(s*cm^2*sr*MeV))	0.0	1.00E+06	-999

Low energy

0.29

High energy

6.7

Units

MeV