/******************* D2 Rate Parameter Information ****************************/
/* MODIFICATIONS: */
/* 920806 JPLPDS::RMONARREZ */
/* received by mail */
/* 92-08 EFRIED */
/* 920916 EFRIED */
/* last changes made */
/* Template: Parameter Template Rev: 19890121 */
/* */
/* Note: This template shall be completed for each combination */
/* of data set parameter name, instrument parameter */
/* name and instrument host id associated with a dataset. */
/* */
/* Hierarchy: PARAMETER */
OBJECT = PARAMETER
INSTRUMENT_HOST_ID = "VG1"
DATA_SET_PARAMETER_NAME = "D2 RATE"
INSTRUMENT_PARAMETER_NAME = "D2 RATE"
IMPORTANT_INSTRUMENT_PARMS = 1
END_OBJECT = PARAMETER
OBJECT = PARAMETER
INSTRUMENT_HOST_ID = "VG2"
DATA_SET_PARAMETER_NAME = "D2 RATE"
INSTRUMENT_PARAMETER_NAME = "D2 RATE"
IMPORTANT_INSTRUMENT_PARMS = 1
END_OBJECT = PARAMETER
/************************ D2 Rate Parameter Description ***********************/
/* MODIFICATIONS: */
/* 920806 JPLPDS::RMONARREZ */
/* received by mail */
/* 92-08 EFRIED */
/* 920916 EFRIED */
/* last changes made */
/* Template: Data Set Instrument Parameter Description Template Rev: 19890121 */
/* */
/* Note: This template shall be completed for any */
/* data set or instrument parameter description. */
/* */
/* Hierarchy: DSINSTPARMD */
OBJECT = DSINSTPARMD
DATA_SET_OR_INSTRUMENT_PARM_NM = "D2 RATE"
DATA_SET_OR_INST_PARM_DESC = "
The D2 detector is located behind the D1 detector in the TET
telescope, so that most of the electrons observed by D2 have
to penetrate D1 first. The D2 rate therefore applies to
higher energy electrons and the threshold energy is less
distinct than for D1, but is near 2.5 MeV. The rate can be
calculated from the electron differential flux in the same
way as the D1 RATE (see D1 RATE description) with the
following calibration table.
D2 response function:
| 11. 23. 41. 61. 80. 90. 100.
________|_________________________________________________
|
0.989 | 0.000 0.000 0.000 0.001 0.002 0.001 0.001
1.179 | 0.000 0.000 0.000 0.013 0.023 0.021 0.018
1.372 | 0.000 0.000 0.000 0.037 0.052 0.051 0.043
1.567 | 0.000 0.019 0.028 0.063 0.082 0.066 0.061
1.763 | 0.041 0.034 0.045 0.090 0.111 0.098 0.080
1.959 | 0.106 0.078 0.072 0.119 0.142 0.125 0.097
2.157 | 0.255 0.186 0.127 0.152 0.170 0.146 0.109
2.355 | 0.488 0.381 0.228 0.206 0.212 0.176 0.126
2.553 | 0.772 0.627 0.361 0.272 0.255 0.202 0.139
2.752 | 1.019 0.864 0.501 0.340 0.299 0.226 0.152
2.951 | 1.220 1.053 0.634 0.400 0.335 0.250 0.165
3.150 | 1.461 1.218 0.746 0.459 0.375 0.289 0.188
3.350 | 1.628 1.378 0.940 0.515 0.456 0.411 0.282"
END_OBJECT = DSINSTPARMD
|