,,'qy - cosmic ray subsystem · c zr90 c high c i127 prot gain 2 13 2 14 16 22 24 26 28 30 40...
TRANSCRIPT
C C FIbE NAME: 1HlLOZ.CET C C MODES GAINS
4 2
I ISEE HETl CALIB (ENTERED 2/9/Rl) THK R
rn
k C ELEM
A 1 c1 A2
c2 c2 c3 c3 c4 c4 82 81
P
t CHANNLS
4096 4096 4096 4096 4096 4096 4096 4096 4096 4096 4096
Low OFFSET
- -.51 1.60 .94 .33
1.35 .12
1.76 64 07 05
1.19
EST 7 1 i 6 7 7 5 5 4 7 4
PE?I 7 7 7 3 7 5 5 4 7 4 7 3 3 3 1 I I
THRESHOLDS
.63 .13
.62 .12 2 . 5 .5
4.68 .92 4.68 .02 4.66 .Y2
4.69 .92 4.69 .92 2.13 . 3 1.02 .3
4.66 e92
G A I N HIGH G FSMEV 953.
OFFSET
17952. 2494.
17%: 17999. 0.
1.5 17964. ,,'qy 1.87
1. 0. 0.
1.76
4910.
5143.
AIN FSHEV 200. 197.1 3603 3533. 3680: 747. 755. 3646. 3683. 3615. 1016.
SPACING 0
2600 6 8 4 7 ~
0 1800 550
1750 5 5 0
5 6 0 560
1770 5 60
2550 560
0 55400
0 a 0
x33
PIDIIJS CllWV 1h156 16156
1
16156 1 1
17131 1 17131 17131 1
1 17131 17131
1 17131 1
1 17131 1 17131 17131 1 17131
1 17131
1 16156 2
1 16156 2 16156 3 16156 3 16156 1
A 1 P2 cz c1
6 BST c3
b BST 8 2
6 EST s asT Cl
H1
c4 c3 C 2
k C 1 2 BOTH GN CHl CH2 CH3 SUM CHI Cg2 CH3 SUM
6 5 . 4 3 -105. SLANT 1 SLANT 2
SA1 SA2 SA 1 1. .6 .375 -39. 1. SB SB ? SB sa 2
1. i. 1. - 6 0 . 1. 1. 1 . -60.
m
k NUMRER OF SPECIES C MODES ' LO GAIN H I GAIN
2 12 4 P
? LOW C N A M E
HE3- HE4- LI6- 8E9- c12- Bll- N 1 4 - 016- F19- VE20 NA23 MG24
GAIN: 2 2 2 4 3 5 6 7 A 9 10 1 1 12
P 3.0149 4.0015
6.00
1 1 .oo 9.00
12.00 14.r)O 15.98 18.99 22.99 23.95 19.99
? HIGH GAIk: PROT 1 DEUT
1.0073 1 2.0135
HE3- HE4.9
2 3.0149 2 4 . 0 C 1 5
-81-
Table 17. HET I1 Detector Description f o r Low Z Stopping Modes
C IT ISEE HET2 CALIt? (EhlTEWEI) 2 / 9 / 8 1 ) TYK R
C FILE N A Y & : 1 H Z W Z . C E T C C MODES GAINS
C C c ELEM
A 1
c1 A2
c 2
c 2 c 3
El: c 4
0 2 81
E kHANNLS
4096 4096 4096
4096 4096 4096 4096 4096
4096 4096
4096 C E
4 2
NO. THICK AWP-AS7 0 16 1 149
7
2 153 1
3 2915 2
0 8 4 3
4 2 9 3 0 7
0 1 7 1 4
4 2 9 0 0 7
5 2430 4
0 142 5 2930
7 5 2 9 2 0
5 0 1 4 8
6 6 2930
7
0 74 6 7 .
7 2225 fJ 2125
7 7 7
0 O b1 3 3 7
DFFSLT
-.27 1.70
-.04 .94
1.68 .13
1.57 1.07 9.03 -.os 1.09
40”
9ST 7 7
6 7
7 3
.13.
5 4
4 7
3 1 2
7 1 7
P E i.1 7 7 7 4 5 7 5 4 4 7
7 3
7 3
7 1
7 7
T H R E S H O L D S
.h3 .13
2 .49 .75 . 62 . 1 2
4.65 .?2
4.65 - 9 2 4.6R - 9 2 4.68 e92 4.69 .92 4.69 - 9 2
2.04 - 3 1.00 .3
OFFSET - .20
. G O
2
30 b * O O 1.89
= 96
-.31 . of4
1.43
HIGH
. ds
SPAClCG 0
6C47F! 7 6 G U
0 1 8 0 0
9 5 0
1750 550
5 6 0 5 6 0
1970 560
2550 5f1q
0 55400
I) 0 0
PPOTUS CURV 1015h 161Sfi 1
1 1 4 1 5 6 1 17131 17131
1 1
17131 1 1
17131 1 7 1 3 1 1
1 17131 1 17131 1 17131 1 17131 1 16156 16156
16156 3 16156 1 16156 3
!E; 1
t 1 2 BOTH GN C H 1 CH2 CH3 SUM C H 1 Cl42 CH3 SIJN SA1 SA2 SA 1 1-
SB s0 2 -6 .375 -39 . 1. .6 5.43 -105.
SR SR 2 1, 1. 1. -60.
1 1. 1. 1. - 6 0 .
SLANT 1 SLLhiT 7
k NUMBER OF SPECIES C MODES LO GAIN H I GAIN
2 1 2 4
? LOW C NAME
HE4- HE3-
L I 7 -
811- BE9-
c12- N14- 016- F19- NE20 NA23 MG24
C
GAIN : z 2 2 3 4
6 7 0
10 9
5
i i 1 2
HIGH GAIN: PROT 1 DEUT
1 .0073 HE3-
1 2 .0136
, HE4- 2 4.0c15 2 3.0149
- 8 2 -
.t . ... . . .
Table 18. HET I Detector Description f o r High 2 Stopping Modes
I ISEE HETl CALIB (ENTERED 2/9/81) THK B C C FILE NAME: IH1HIZ.OET C C MODES
4 GAINS
2 .C C C ELEM
A 1 Cl A2
c2
c3 c2
E: c4 02 B l
E CHANNLS
4096 4096 4096 4096 4096 4096
4096 4096 4096 4096 4096
E
NO. THICK 0 16 2 151 1 148 3 2920 0 81 4 2925 0 171 4 2900 2 2U90
5 2925 0 140 6 2935 0 68 7 2150 8 2 3 0 0
0 33 0 84
5 2 M
AM P I-AST 7 2 1 3 7 4 7 4 7 5 5 6 7 6 7
7 7 3
,OFFSET FSMEV 1.60 0.51
953. .94 17i13: - 3 3 11992. l:$i 17999. 2494. 1.78 17984.
4910. .07 17859.
1.19 .OS 18128.
5143.
LOW GAIN
s 64
BST 7 1 7 s 3
3 1 $
5
i 2
7
PEN THRESHOLDS 7 e63 - 1 3 1
7 e 6 2 el2 2 2.5 .5 7 5 4.68 .92 7 5 4.68 .92 4 4.66 -92 7 4 4.66 .92 7 3 4.69 .92 3 4.69 .92 7 7 2.13 .3 1 1.02 . 3 7 7
OFFSET HIGH
q 6.
1.5 0 .
1 .8$ 1
0. 0.
1.76
GAIN FSMEV 200.
197.1 3533. 3603.
* 3680.
755. 747.
3683. 3646. 3615. 1016.
SPRCINS 68478 2600
0
550 1750 550
560 560
1770 560 560
2550 55400
0 0 0 0
1 800
R P D US CURV 16i56 1 16156 1 16156 1 17131 1
1 : I :% f 17131
17131 1 17131 1
16156 3 16156 3 16156 16156 1
f w l 1
P S T A 1
AST c1 AST A2
AST c3 AST C2 PEN 6 BST 01 @ST 82 PEN 6 BST C4 PEN 6 EST c3 PEN 6 BST C2 PEN c1
5: 1 2 BOTH GN CHI CH2 CH3 SUM CHI CH2 CH3 SUM
SLANT 1 SLANT 2 SA1 SA2 SA 1 1.
SB SB 2 .6 .375 -39. 1. .6 5.43 -105.
SB s0 2 1. 1. 1. -60. 1. 1. 1. -60. C
C C MODES LO GAIN HI GAIN
NUMBER OF SPECIES 2 10 1
rn
k LOW C N A M E
SI28 AL27 S32- CA40 AR36 TI48 CR52 FE56 NI58 ZN64
C ZR90 C HIGH C I127
PROT
GAIN 2
13 2 14 16
22 24 26 28 30 40
GAIN: 5 3
1
1:
1.0
-83-
Table 19. HET I1 Detector Description for High 2 Stopping Modes
I1 ISEE HET2 CPLIB (ENTERED 2/9/81) THK B C C FILE NAME: IH2HIZ.DET E MODE1 GAINS
2 E
ELEM A 1 c1 A2
c2 c2 c3
c4 c3
c4 B2 B1
I t EHANNLS 4096 4096 4096 4096 4096 4096
4096 -4096 4096
1%
E
NO. 'THICK 0 16 1 149 2 153 U 04 3 2915 4 2930 0 171 4 2900 5 2930 0 142 5 2930 6 2920 0 148 0 74 6 2930 7 2225 8 2125
" 0 61 0 3 3
OFFSET -. 27 LOW G
1.70
4 7 5
6 5
6 7 7 7 7 7 7
AIN FSME V 958. 938.
18128. 18243. 17630. 2542.
17938. 4998.
17375. 18068. 5150.
BST 7 7 7 6 7 J i 4 7
7 3 3 7 2 1 7 7
i 7 2 7 75 5 4 7 4 3 7 3 7 7 7 1
.63 s 6 2
2.49 4.65
4:60 4 65
4.69 4.68
4.69 2.04 1 .oo
.13
.12
.75
.92
* 92 92
e 92 .9?
.92 . 3 e3
6p57; 2 6 0 0
0 1e00 5 50 1750 550 560 560
1770 560
2550 560
0 55400
0 n
v 6
OFFSET FSMEV e 6 0
- 0 2 0 202.1 10'5.6
2 3687. 3712.
e 30 3548. 1 .oo
- 9 6 785.
1.89 R00.
3619. .OR 3517.
-.31 s .43 3677. 1053.
HIGH GAIH
0 a?
RADIUS 16156 16156 1 hl56
17131 17131 17131 17131 17131 17131 17131 17131 17131 17131 17131 16156 16156 161 56 16156 1b156
C U R V 1 1
1 1
1 1 1 1 1 1
1 1 1 1 2 2 3 3 1
AST A 1
AST c2 PST c 1
AST c3 PEN 6 RST PI BST e2 PER s RST c3 PEF! S HST C4
PEli c 1 PEN 6 RST C2
AST a2
k c 1 2 BO'TH GN CH1 CH2 CH3 SUM CH1 CH2 CH3 SlJM SA1 SA2 SA 1 1.
SB SI3 2 - 6 .375 -39. 1. .6 5.43 -10s.
1. 1. 1, -50. 1. 1. 1. -60.
SLANT 4 SLAtiT 2
SR sn 2 r- L
C NUMBER OF SPECIES C MODES LO G A I N HI GAIN
2 10 1
C C C
NAME z SI28 AL27 13
14 S32- 16 CA40 20 AR36 18 TI48 22 CR52 24 FE56 2 6
ZN64 30 NI58 28 ZR90 40 1127 53 PROT 1
LOW GAIN:
HIGH GPIL:
26.98 A
27.09 3:-8 39'96 47:95 51.94 55.97 57.94 63.93 127. a9.90
1.0
-84-
Table 20. HET I Detector Description for 2-Dimensional Stopping Modes: special run
c C ELEH
A 1 A2 c1 c 2
c 2 c 3
c 3 c 4
c 4
B1 02
R.5T
7 7 .
1 6
1 .63 .lj 7 -62 .60 7 2 2 . 5 . 5
7 5 4.68 .92
5 4.68 .02
7 4 4.66 .92
73 4.69 .Y2 4 4.66 .92
3 4.69 .92 7 i 2.13 2.1
1 1 1.02 .3
7
1 R O O 5 5 0 550
1750 560 5 b 0
1770 ' 6 0 5 6 0
2 5 5 0
55400 0
0 0 0
R 4 D T i I S
1 h15h 1h156
17131 16156
17131 17131
1 7 1 3 1 17131
171 31 1 7 1 3 1
17131
1 7 1 3 1 1 7 1 3 1
1 7 1 3 1 1615h 16156 16156 16156 16156
C l l P V 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 2 3 3
I CHANNLS OFFSET FSMEV
4096 1.60 953. OFFSET FSMEV 4096 -.51 931. 8. 2 0 0 . PST A 1 4096 .94 17833. J 197.1 4ST A2 4096 a33 17992. 3533. A S T C1 4096 -12 17999. 3603. PST cz 4096 1.35 2494. 4096 6 0 4910. 4096 1 -70 17934 . 1. 755 . 4096 1.87
RST R2 364b. PEN 6 HST C4
4096 4096 1-19 5143. 1.76 1016. PEN C l
PEN 6 BST C2
Low GAIN HIGH GAIN
6 . 0. 3660. A S T C3
1.5 747. PEN 6 BST 6 1
0. 36F3. PEN 6 9ST C3 0. 3615.
-07 17859 . .os 1 ~ 1 2 ~ .
C c C c 1 2 BOTH G N CHI CH2 CH3 SllY CH1 c1.12 cu3 SUM
SA1 SA2 SA 1 1. SB SB 2
- 6 - 3 7 5 -39. 1. .6 5 . 4 3 -105. SB SH 2 1. . 1. 1. - 0 0 .
1. - 6 0 .
SLANT 1 SLANT 2
C I. 1. C C MODES Lr! G A I N H I GAIN
C C LOW G A I N : C NAME
HE4- z 2 4 .0015
A C C HIGH G A I N :
OEUT ?ROT
1 2.0136 1 1.9073
HE3- 2 3.0149 HE4- 2 4.0015
N U M B E R OF SPECIES 2 1 4
1
-85-
.. .
C c ELEM
A 1
C l A2
c 2
c 3 c 2
c 4 c 3
c 4
82 81
r
NO. T H I C K AMP-AS7 0 16 1 1 4 9
7
2 1 5 3 1 2
3 2 9 1 5 0 64
3 7
4 2930 0 1 7 1
4
4 2900 4 7
5 2930 0 142
5 7
2 H:2: 6 5
SB 0 1 4 8 8 29;: 7 h 7
7 2225 8 2125
7 7
0 3 3 7
9ST 9 7
6 7 7 5
f 4
4 7
3
3 7 7 2
9 1
7
P E 1.1 9 7
2 7
7 5 7
4 5
7 4 9 3
9 3
7 1 7 7
THPEPHOCDS S
.h3 - 1 3
2.49 .75 -62 -60
4.65 - 9 2
4.6R -92 4.65 -92
4.69 e92 4.68 - 9 2
4.69 .Q2 2.04 2.2 1.00 .3
J'ACTAG 0
2 6 0 0 0
1 R O O 5 5 0 5 5 0
1750 5 6 0 5 6 0
1 7 7 0 5 60 5 6 0
2550 0
55400 0 0 0
h?47k P A D l l l S CllRV
lhlSC. 1 l h 1 S h 1
17131 1 16156 1
17131 1 17131 1
17131 1 17131 1 1 7 1 3 1 1 17131 1
1 7 1 3 1 1 17131 1
17131 1 17131 1
16156 2 16156 2
16156 3 16156 3 16156 1
E LOW G A I N CHANNLS OFFSET FSYEV
4096 1.10 OFFSET 958.
FSMEV 4096 -.27 9 3 8 . 4096 -94 18128 . -.20
2 195.6 k S T A2
4096 - .04 16243. 0 b e 3667. AST C 1 4096 -13 17630. 3712. AST C2 4096 1.68 2542. .30 3548. AST C3 4096 1.07 4998. 1.00
9 6 785. P E ~ s a s T H I
4096 l e 5 9 17938, R O O . PST e2 4096 -e03 17375. 3619. PEN 6 PST C 4 4096 -.OS 18068. * 08
p.31 3517 3677:
PEht 6 BST C3 4096 1 -09 5150 . 1053 . PEP! C l PEN 6 BST c 2
1.43
H I G H G A I N
o 60 202.1 AST A 1
1:ss
E t.. SLAIT 1 c 1 2 BOTH GN CHI CH2 CH3 SUM C H 1 Ch2 CH3 SIIC
SLANT 2 SA1 SA2 SA 1 1.
SB SB 2 SB SB 2
06 .375, -39. 1. .6 5 . 4 3 -105. 1. 1. 1. - 6 0 . 1. 1. 1. -60. C c N U N B E R OF SPECIES
2 1 4 C MODES LO GAIM H I C A I N C
C NAME C LOW G A I N :
HE4- z A 2 4.0015 m
? H I G H G A I N : PROT 1 1.0073 DEUT HE3-
1 2.0136 2 3.0149
HE4- 2 4.0015
-86-
c o ~ r e s p o n d i n q oucs ~ h o w u in , T d b l e 23 : a special run i ~ a s
m d r u s i n q the d e t e c t o r d e s c r i p t i o r s shown i n T a b l e s 20 a n d 2 1 t o chalrqe t h o s e rtvpcnses scnedhat, I n Tdbles 2 2 t h r o u g h
Liz t h e HAXS cclumn sefers t o t h e isaxituum energy w h i c h uight De p o s s i o i e for e v e n t s f a i l i n g on t h a t p a r t i c u l a r ads5 l i n s ; t h a t enecqy is 11ot t h e same d 5 the 9cei l incJt ressonse erlcrqy
as discussed i n t h e n a i n document.
P . i q u r e 28 i l l u s t r a t e s the e f f e c t of t h e overlay p r i o r i t y parameter in t h e 3iiACd d e f i n i t i o n , T h e ase of t h i s parzlineter is i n t e n d e c as a n a i d i n d e t e r m i n i n g t h e num.her of c o u a t s to assiqc t o a pac t i c l e . A l t e K i m t i V e i y , a co r rec t iov to ca. lculated fluxes u s i n q f u i l T R A C K S might De iniide, S i n c e the re la t ive a w n d a n c e s of t h e o v e r l d ? p i n y species aay b o t
c e weii known, The B U X G E B d e f a u l t overlay p r i o r i t y L = 0 )
C ~ U S ~ S d full T B X Z to be qenexated f o r each aass l i n e species as t h o u q h nc o-ther Bass lines 0 V S X . l d p p e d t h a t miiSS
lines' da ta .
Pocz ious of t h e job p r i n t o u t s fxcro I d S T A L C x u n s f o r the uata of Tables 2 2 - 2 4 is i n c l u u e d i n Tables 2 5 - 27. T h e y
show t h e exact o v e r l a y p r i c r i t y zsed for each of the c u x r e n t s t o p p i n q titodies, Yhere DO overlay p r i o f i t y is i u d i c a t e a , the BOXGEhi default value h a s nee11 used. CcmFLete IivlSTALC j o b
p x i n t o u t is i .uc iuded i n L i l i t r a t i o n Ecak I1 meut ioned a u o v e . Flqufes 29 - 32 shor t h e c a n p u t e r Ili3ACK.S f o r a f e u of: t h e
s t o p p i n y ;;lodes, Ccailplete ;r;ut;s to: d i ~~oiie!s dxe disu i ivai lable i n Book It
c
I. "
Table 22. BOXGEN Summary of Special 2-dimensional Stopping Mode Responses
e 2 0.98 117 0.9F 354 0.93 313 0.98 104 0 . 9 h 144 0.9h 391 0 .96 443 0.96
2.Y3 4.43
5 . 1 3
20.36 4-35
13.73 23.73 7 0 24
7 91 P 1
PS hY P 1 6171 F1
20:13 P 1
29.76 P1 34.70 F 1
1 0 I I A Z H + OEUT 79 9 IIAZH+ PROT 60 1 137 0.9A 1 05 4.45 6.85 P1
1 1 8 2 1?3 0.96 1:OS 2.94 4.56 P i 11 IIAZH+ HE3- 1Q5
I I A Z H + HE4- 114 2 444 312 0.98 1.04 5.15 7.96 P1 2 539 353 0 .98 1.04 4.36 6 .76 P1
IIB2H+ PROT 62 14 IIR2H+ DEUT 82
1 151 93 0 .96 1.03 19.44 29.27 P1
15 IIBZH+ HE3- 1 0 5 1 2 0 5 13b 0.96 1.03 13.10 19.84 P1
16 IIBZH+ HE4- l a 8 2 529 354 0.96 1.03 22.62 34 1 6 P1 2 5 9 9 402 0.96 1 - 0 3 19.29 29:34 P 1
-88-
1 IA2H+ PROT 62 1 136 90 0.98 1.05 2 IAZH+ DEU’I 79 3 IAZttt HE3- 103 2 491 321 0.9Q 1.C5
1 180 121 0.98 1.05 4 IA2H+ HE4- 115 2 543 367 0.98 1.05 5 IBZHi PROT 65 1 163 113 0.96 1.03 7 I82H+ DE”T HE3- 107 2 567 400 0.96 1 .C3
1 220 153 0.96 1.03 8 IBZH+ HE4- 121 2 642 453 0.96 1.03
196 IA2L+ BE9- 24: IA2L+ LI6- 4 212 141 0.9P 1-02 4 352 231 0.98 1.02 4 625 409 0.98 1.02 4 490 322 0.98 1.02
13 IA2L+ 1A2L+ N14- 71 89 4 793 517 0.4R 1.02 14 IAZL+ 016- 108 15 IA2L+ Fig- 70
4 974 633 0.9P 1.02 8 1184 767 0.98 1-02
16 IA2L+ NE20 79 8 1361 480 0.98 1.02 l7 18 IA2L+ g:ii 104 9 2 8 1792 1143 0.98 1.02 8 1601 1030 0.96 1-02
JHIL02.DET PIN E P A X E
4.34 2 . 8 8 5.10 4.35
20.15 23.69 13.64 20.21 5.44 5.91 6.72 7.82 8.47 9.06 9.25
10.25 10.08 10.90
6.76 PI 4.51 e1 7.91 PI 6 71 P1
29:69 P1 20.13 P1 34.70 Pi 29.76 P1 8.50 PO 10.60 PO 9.28 PO
12.35 Po 13.40 PO 14.39 Po 14.79 PO 16.13 Po 16.48 Po 17.62 Po
1HlHIZ.DET MIN E M A X E
20 IA2L+ SI28 69 16 2256 1430 0.08 1.07 11.69 19.02 P2 19 IA2L+ AL27 63 16 2049 1201 0.98 1.C2 11-03 17.91 P1 21 IA2L+ S32- 83 16 2762 1743 0.98 1.02 12.47 20.36 P1 22 IAZL+ AR36 98 16 3282 2062 0.98 1.02 13-11 71.54 P1 24 IA2L+ TI48 72 32 4560 2827 0.98 1.02 13.44 22.43 P1 25 IA2L+ CR52 80 32 5142 3154 0.98 1 . C Z 13.90 23.36 P2 26 IA2L+ ?E56 89 32 5754 3536 0.98 1.02 14.37 24.29 P3 28 IA2L+ ZN64 107 32 7017 4273 0.98 1.02 15.44 75.92 P1
23 IAZLi CA40 114 16 3845 2408 0.98 1.@2 13.77 22.71 PZ
27 IAZL+ N I 5 8 94 32 6303 3863 0.98 1-02 15.59 25.68 P2
IIAZH+ IIA2H+ IIA2H+ IIA2Hi IIR2H+ IIB2H+ IIBZH+ IIB2H+ IIAZL+ IIA2L+ IIAZL+ I I A2L+ IIA2L+ IIAZL+ IIA2L+ IIA2L+ IIA2L+ IIAPLt
63 83
108 119 63 64
105 118 39 43 57 71 108 89 70 79 104 97
1
2 1 2 1 2 4 4
4 4
J 4 A A d
4
a
91 121 320 365 103 139 412 364
231 1 50
322 4n9 517 632 7 6 7 A R O
1 G?9 1142
0.9‘) 0.98 0.9P 0.9R 0.96 0.96 O.Q6 0.9P 0.96
0.96 0.99 0.9P 0.9R 0.98 n.9e 0.98 0.4R 0 . o e
f - 0 5 I .05 1.05 1 .05 1 . @ 3 1.03 1 .C3 1 .C3 1 .n2 1.02 1.02 1 .OL 1.0% 1 . c 7 1.c2 1 .n>
1 .O?
1 .r2
IH2LnZ.DET P I N E P A X E 4.35 2.49 5.11 4.30 19.20 12;99 22.58 1Y.26
4 . 9 8
7 . 8 s 6.75 8.50 9.10
111.12 Y.2Q
1 0 . 2 9 1 0 . 9 5
5.94
6.85 PJ 4.56 P1 7.96 Pi 6.76 Pi
29.27 P1 19.84 PI 29.34 P1 7.81 PO 9.33 PO
10.66 P O 12.41 P O 13.48 P O 14.47 PO 14.61 PO 16.5e PO 16.22 Po 17.72 PO
34.18 PI
1
I .07 1 . 7 4 2 . 5 2 3 . l o 3.d7 3 . 5 0 3 . ? h
L . 5 H 4.44
5 . 5 1
1P.02 p l 1 9 . 1 3 P ? 2 ~ , . 4 h PI 2 1 . 6 7 PI 2 2 . 5 7 PI 73.51 P Z 24.44 P3 25.64 PZ 7 6 . 0 k PI
22.~4 ~2
Table 24. BOXGEN Summary of 3-dimensional Stopping Mode Responses (1 of 2)
BOXGEM TABLE' TAPE 11 V R T T T E N 13-FER-HI
FILE ISEE
3 5 4
7 6
8 9
10 11 12
1 4 13 15 1 6 17 18 19 20 21 22
2 5
27 26
28 29 30
ISEF: FILE
E
32 31
3 3 34 3 5
37 36
38
40 39
41 42
4 4 43
46 4s
47 4R
SO 49
FILE ISEE
51 52 53
55 54
5 6 5 7
50 58
6 0
62 5 1
6 3 6 4 65
!ijl DEllT PPOT
IA3H t1E3-
I63H PROT IA3H HF.4-
IB3H I)EUT 183H HE3- 1B3H hR4-
1A3L YE9- IA3L Llb- IA3L H11-
Ih3L N14- . IA3L C12-
IA3L 016-
IA3L E1E20 IA3L F l 9 -
IA3L NA23 IA3L MG24 TL3L tiK.3- IL3L HE4- 163L LIb- IR3L BE9- IB3L 811-
i8zk 1414- c 1 2 -
163L 016- IR3L t.19- 1B3L kE20 IB3L NA23 I B 3 L M624
70 9 3
120 135
1 0c 7 6
129 144
411 3 2
64 9 9 79
120 77 i l R
32 34 35 5 1 hR
, E 5 1 Oh 1 2 9
94 82
1 2 2 1 0 9
1;:
1 1
2 2
1 1 2 z 4 4
4 4 4 4 8 8
e" 2 2 4
4 4
4
4 4
8 8
P e
6 3 8 0
274 2 5 4
94 2 4 3 275
97 1 6 0 2 2 5 2R7 366 45 1
64 1 5 5 6
759 854
SO 57
105 1 7 3
4 8 5 3 9 3 596 68R 815 91 7
711
3:;
6 2 4 5
160 1 R 4
5 0 75
1 9 3 219
71
212
332 41@ 472 5 5 9 6 2 0
SR ti5
1 1 2 201 2 8 2
458 360
564 695
948 R 0 1
1067
: 2: 270
O Y
0 , O P
v. 96 n.se 0 . 4 6 0.96 (1.96 0.9P 0 . 9 6 0.9n
0 . 9 h 0.9P
0.9P 0.98 0 .96 0.96
o .ya 0.98
0 . 9 8 0.48 0 . 5 @ 0 . 9 8 0.98 0.98 0 .96 Q.98 0.98 0. 08 0.98
G:& 1 . C S J .(1S 1 .05 1 .05 1 0 3 1 . 0 3
1 .ti3 1 - 0 3
1.02 1 .07 1.02 1 .c2 1.02 1 0 2
1 .G7 1 - 0 2 1 - 0 2
1 .*7 1 .GL 1.02
I . c 7 1 .U?
1 . O ? 1 .e? 1 . 0 2 1 . 0 2 1.02 1 .G2 1 .1;2
1 . t 7
0.39 4.26
6.34 7.47
74.65 19.h5 35.12 79.12
9.7h d.02
1 u . 00 11.65 12.64 13.57 13.93 15.20 15.52
29.19 3 4 e 2 1
36.57 4 C . 1 R 46.07 53.79 5H. 6 2 h3.1Y 05.43
73.57 71.54
79.16
1 6 . 5 8
58.36 39.59 hk.65 59-56 70.P7 42.02 h 3 . 3 h 71 .Ob
80.94 73.57 92.97
l l h . 8 1 323.26
195.75 133.00
150.00 16l.RR
P 3 . 3 ? 71.10 H9.37 Y H . 3 8
113.11 132.56 144.83
1b2.33 156.46
183.41 1 7 8 . 0 k
19h,O5
I G U . ~ ~
HETl CALIR (ENTERED 2 / 9 / 8 1 ) THK B MODE PART RECS SCALE ENOCH P A X 1 SPRFACF M 1 r . l E M A X I..
R E k IHIFiIZ.[)ET
Pl c'1 P 1
P1 e1
Pl P I Pl PO PC PO PO PO PO
P2 P 1
P 1 02 P1 P i
PO PO
P 0 PO PO
P1 PO
P1 P2
P3
IA3L AL27 6 9 16 9R4 698 0.46 l.C? 1 6 . 8 s 165 .89 P 1
IA3L 532- 92 1 6 1 3 4 6 OR7 0.98 1.02 1 9 - 1 4 191 33 P1 IA3L S I 2 8 76 16 10R9 d 0 l 0.4s 1 . 0 2 1 7 . l h 177.02 P2
IA3L AR36 1 0 9 16 1627 1 1 8 6 0.9P 1.C7 20.23 2 0 4 1 9 1 P1 IA3L CA40 1 2 7 16 1916 1397 0 . 9 8 1.02 2 1 . 3 3 21A.10 P2 IA3L TT46 8 0 32 2 3 0 9 1666 0.96 1.G7 2 1 . 0 4 219 0 3 P I IA3L CR52 90 32 2643 1AAS 0 . 9 8 1.02 21.89 231147 P2 IA3L F256 101 32 2 9 9 5 216R 0.9b j . 0 9 22.75 243.53 P 3 IA3L NIS8 1 1 1 32 3 3 1 7 23n8 0 9 P 1.02 2 4 , h O 260.45 F2 JA3L 21464 1 2 5 32 374b 2689 p:9R 1 .02 24.58 2h6.55 P 1 I83L AL27 74 16 1057 1231 0.98 1.02 111.03 203 04 P i
IB3L 532- 9 9 1 6 1445 1680 0.9P 1 . 0 2 42.Y7 234.6b P1 I R 3 L ST28 8 1 1 6 1 1 7 0 1 3 6 1 0 . 9 8 1 . C 2 1 6 . 2 h 21h:e7 P;
IR3L CA40 1 3 6 1 6 2 0 5 9 2393 C.CR J . O ? 105.34 26b.14 P 2
IP3L CAS2 S6 32 7941 3309 n.3R 1.07 111.2L ? P d , L O P2
I 6 3 L 2'164 1 2 8 32 4679 4094 0 . 9 h ~ . r ? 12p.63 37p.74 P I
I B ~ L A P ~ C , 1 1 6 1 6 1742 2035 ~ i . 9 ~ 1.02 99 .29 251.73 PI IR3L T I 4 8 85 3 2 24Rl 2889 O.Yb 1.04 105.h3 2 6 9 . 3 6 P l
In318 FF:56 1 O P 32 3 2 1 9 3749 (1.96 1 .C7 1 1 6 - 6 3 3UI!.17 P3 I H ~ L :IISR 1 1 9 32 3s6n 4044 0 . 4 ~ 1 . ~ 2 174.31 371.45 P%
I I A 3 H IJA3H T IA3H IIA3H IIB3H IIR3H I I B 3 p I I P 3 n IIA3Ia
I IA3L IIA3L
IIA3L 11 A3L I I h 3 L TTA3L
71
1 7 1 3 4
1 3 b 161
1 6
1 2 9 1 4 5
3 4
6.4 4 8
h 0 100 1 7 7
74
1
2 1 i 1 1
2 2
A
4
4 4
4 R
*
4 s 6 1
143 1 5 9
48 b h
160 1 9 2 76
1 1 6
71 1 156
2 6 9 331 4o9
-90-
Table 24. BOXGEN Summary of 3-dimensional Stopping Mode Responses (2 of 2)
6 6 TIA3L NE20 8R 67 I I A 3 L NA23 1 0 3
8 647 A71 0.98 1 . 0 2 15.28 14 32 P 2 68 I IA3L HG24 115 6 9 I I L 3 L HE3- 32 2 50 53 0.98 1 . 0 2 33.73 83.36 P I
8 863 627 0 .96 1:02 16.68 162.51 P2
7 1 I16 L L I T - 36 7 2 II63L ' RE9- 51 7 3 II63L 811- 6 9 7 4 I I 6 3 L C12- 86
4 245 256 0.98 1.02 45.41 113.06 PO 7 5 I I B 3 L 1914- 1 0 7 7 6 I I 8 3 L 016- 1 3 0 77 I IB3L F19- a 3
4 490 8 664 z.!; 0199 1:02 64.49 162.26 P 1
78 I I R S NE20 9 5 7 9 I I P 3 L NA23 1 1 1
696 725 0.98 1.02 70.52 178.00 P2 8 0 I IB3L MC24 1 2 4 8 928 967 0.98 1.02 78-02 197.97 P2
a 766 557 0.9~ I 02 1s .h t 158:65
70 I I L ~ L n ~ 4 - 35 2 57 60 0.98 1 . ~ 2 28.77 71.07 P I 1 1 3 119 0.98 1.02 33.07 81.88 PO 1 1 7 5 1 8 3 0.9R 1.02 39.61 98.34 Po
4 398 41s 0.98 1.02 57.79 144 77 PO o 98 1 02 62.28 156:41 PO
e 825 e59 0.98 1.02 72.51 183.33 P I
4 312 326 0.98 1.02 53.03 132.50 PO
FILE MODE PART RECS S C A L E ENDCH M A X 1 I S E E HET2 C A L I 6 [ENTERED 2 / 9 / 8 1 ) THK P
SPREPCS MStd E # A X E R E W IH2HIZ.nET
8 1 IIA3L A627 70 1 6 994 69b 0.98 1.02 16.95 3 6 6 . 5 4 PI 82 IIA3L S I 2 8 76 1 6 1 1 0 0 798 0.9R 1.C2 17.99 177.72 P2 8 3 I IA3L ,532- 9 2 1 6 1 3 5 9 9R3 0.9R 1.02 19.25 192.09 P 1 85 I IA3L CA40 1 2 9 1 6 1936 1392 0 98 1.02 21.45 218.97 P2 87 I IA3L CR52 91 32 2671 1879 0 98 1 0 2 P2.03 232.41 P 2 86 I IA3L TT48 R O 32 2333 1 6 6 0 0:9P 1.02 21.17 219.91 P 1
89 IIA3L 8 1 5 8 1 1 2 32 3351 2380 0 ' 4 8 1.02 24.97 261.52 P2 90 I IA3L ZP64 126 32 3784 2680 0'9R 1 0 2 2 4 ~ 7 3 267.64 P 1 9 1 I I 8 3 L AL27 74 1 6 1070 1115 o:98 1102 79.86 202.46 P i 9 2 I I 6 3 L S I 2 8 8 2 16 1 1 8 4 2 3 0.98 1.02 05.03 216.77 P2 9 3 I B3L 532- 9 9 1 6 1 4 6 3 1512 0 98 1.02 91.62 234.58 P 1 9 4 I I B 3 L AR36 1 1 8 1 6 1 7 6 4 1834 0:98 1.02 97.84 251.62 P 1
8 4 I I A ~ L ~ ~ 3 6 110 1 6 1 6 3 8 l i e 1 0.98 1 . 0 2 2 0 . 3 6 2 0 5 . 8 ~ P I
e a I I A ~ L ~ ~ 5 6 1 0 2 32 3025 2161 O'QR 1:02 22.89 244.52 e3
9 s I I B ~ L C A ~ O 1 3 8 1 6 2 0 8 s 2167 0.98 1.02 103.79 268.02 P P 9 7 I I B ~ L C P S ~ 9 7 ;$ 2877
2996 o 98 1.02 109.60 284.86 p2 9 6 I I B 3 L T I 4 8 86 32 2513 2616 0.98 1.02 104.07 269.24 PI
98 I I B 3 L FE56 1 0 9 9 9 I I B 3 L NI58 120 32 3614 3760 0 .98 1 0 2 122.46 321.35 P2
3261 3395 0198 1.02 114k95 300.03 P3 1 0 0 I I B 3 L ZN64 135 32 4082 4094 0.98 1:02 125.02 329.09 P 1
EQUAL OVERLAY PRIORITY
M1
M2
M3
LINE AREAS ARE NOT USED IN THIS CASE
M1
M2 M1 > M2 M3 PRIORITY
LINES HERE INDICATE FINAL TRACK DEFINITION
M3
M1
M2
M3
M1 e M2 > M3 PRIORITY
Figure 28. Examples of the E f fec t o f t he Over l ay P r i o r i t y Parameters
-91-
Table 25 . INSTALC Summary Showing O v e r l a y P r i o r i t y f o r P a r t i c l e Mass L ines - INSTALC ou tpu t fo r Tab le 2 2
(1 of 2 )
ISEE*)-RESPONSE- I N S T A L L A W . . _. . . . - . . . .
C---- . .DETf f .FOR~-Bf . -S i i1 l+G2D .DET- ..TRACK -FILE- SHlHGODoTQK C I ISEE H E T l C A L I B (3/7/81) A2.62 ABOVE CH 12 I N HGREORCU
b
FROM FILE 1- 16 M U L T I P L I C A T I O N F A C T O R S = i . ooooo'
C A - S T O P P I N G H I G H G A I N
l.;. w 0 ~.
. . . . . . . . .
C
I A 2 H P R O 1 1 1.007
NE-U T A B L E F O R 1 A 2 I N RECORDS 23a6 2389 THRESHOL- 4.43200 C E I L I N G = 6062700 . . - . . .
c 'eax SPREAWFACTORS=- 0 . ~ 8 0 1.050 OVERLAY PRTVRITY ' 1 4. 432 6.759 16 3810 .sz ........ L ....... as . . . 136 . . . - 3 . . .
REPttAC€N6-MWE?A.2-- -fBR PROfON .- C DETECTOR FILE I H ~ H G 2 D . D E T c x ~ S E E H R I CALIB ( 3 / 7 / e ~ ) ~2.132 ABOVE CH 12 I N HGRECRCU
, ....... ._ .
'C . A-STOPPING - '
*TRACK F I L E , IHlHG?D.TRK H I G H GAIN
-92-
Table 25. INSTALC Summary Showing Overlay Priority for Particle Mass Lines - INSTALC output for Table'22
(2 of 2)
-mPLACSUG .*ODE 182 . .FOR HE4 -
e---... *-7nPPf))* - . . ...- I , . . -_
THRE SHOLOI 20.23799 C E I L I N G = 2 9 e J O 8 O O
c 11 ISEE HET2 C A L I B ( 2 / 9 / 8 1 ) A 2 . 8 2 A a O V E CH 1 2 I N HG RE RUT C W E C T O R FILE I H 2 H G 2 D &ET
C
.TRACK F ILE IHZHG2D.TRK - H I G H GAZN-
8 3
2
1
1.050 O V E R L A Y P R I O R I T Y 1
3 4.447 6.841 48 36:02
:431 2434 6.65200
A 2 r B 2 - A B W e . C H 1 2 I N HG RE RUT
HlGH G A I N .TRACK F ILE IHZHG2D.TkK
c c BOX SPREAD FACTOR- 0.980 .I.IXO OVERLAY PRIORITY I
.$IA2M-..-DEU.%- ' . I.-. . 2,014 72 I 111 * 182 3
2-936 4.561 48 3b02
NEW TABLE FOR I I A 2 I N R E C O R D S 2 4 3 8 2439
R E P L A C I N G #ODE I I A 2 FOR DEUTRON C ..-.gI. XSEE . HET2 C A L I 8 (2/9/819 A 2 . 8 2 A B O M , CH 1 2 I N HG RE RUT
c A-STOPPING
-..Tm-.----- P " o 9 3 ( 5 6 0 . - C E l t i N 6 ~ ' 4 ~ 4 3 3 0 0
'+C Z € T E W W - F ! L E ~ ' ! H i M G 2 D ~ D E Y STRACK FILE IHZHG2D.TRK H I G H G A I N c- -- ...*:... - .. .-. . . ..
c BOX SPREAD FACTORS= a. kea 1.040 O V E R L A Y P R I O R I T Y 1
-3 5.145 7. so3
' 4 4 0 2445 7.682043
~ 2 . ~ 2 A a o w en 12 IN HG RE *TRACK. F ILE I H 2 H G 2 D . f R
H I G H G A I N
48 3602
RUT K
- C - ' .~-SPR€AD-FAC-'TORS= :. OOSBO . 1.040 .O.VER&AY P R I O R I T Y 1 I 1 A 2 M M4
107 2 326 ?I39 3 2 4.002 4.362 6.761 . 48 3602
'RU"TliBCe' FOR X1A2 IN' RECORDS' 2 4 4 e 2 4 5 1 THRESnb- +e36200 C E I L I N G = REJ?L*UIG..YODE L I A Z E D R HE4
6.64900
C 11 ISEE HET2 C A L I 6 f 2/9/81 1 h2.62 ABOVE CH 1 2 T N HG RE RUT C DETECTOR FILE IH2HG2D .DET e. . -B--s.Mppxw . . ... ..-.. C C IfB2H 'e-* ~~~ SPRe-AD .... ..L.. PACTOR?. 0.060 1 . 0 3 0 O V E R L A Y P R I O R I T Y I
55 I 1 .DO7
1 97 IS1 3
sTEACK FILE I H 2 H G 2 O ~ T k K H I G H G A I N
1'9.443 2F.270 306 3 7 7 6
Uer..TAaLE..F& I162 ..IM..RECORDS 2452 2455 THRESHOL03 1 9 . 4 4 2 9 9 C E I L I N G = R E P L A C I N G MODE 1192 FOR PROTON
28.96700
C DETECTOR FILE I H 2 H G 2 0 &Et .TRACK FILE I H 2 H G 2 D e T R K ~ - * ~ M . . . - H E T E . eAtsm-t-e/wet 8 A z . 8 e ABOVE CH 12 I N HG RE RUT
. '"L- f ' ' ---.. B--Srn.??ING . . ,. ._ H I G Y G A I N
I c .._ .. C E O X S-PkEAE-kACTOR!& 0.960 1.030 O V E R L A Y P R I O R I T Y t I I B 2 H M 3 2 3.015 22.623 3 4 . 1 7 7 306 -- .. w.. --9t)-- .--- .p - -.._-... NEW TABLE FOR I182 I N RECORDS 2461 2466
355- ' ' - 5P9 - ' 3. '
THRESHAP, - R E K X F I H G ~I3O€-ITB2'TOR'~HE3
22ot2299 CEIL,IIN,G= 34* 0560 0
C I f -1SESE M T 2 C A L I B (2/9/81) A 2 . 6 2 ABOVE CH 12 I N HG RE RUT
C 8 -STOPPING C
A - - -Q~,ESJ-OR-E.ILE-~IJi2ffi2D .DEf,, .. STRACK F ILE IH2HGPD.TRK HIGH GAIN
. . .
37 76
A+--- BOK--SPRE.AD.-FACTQ+ . 0.960 1.030. O V E R L A Y P R I O R l T Y I 1162H E 4 . 1 1 8 2 379 5s9 3
T H R E S H O L P 1 9 . 2 9 3 0 0 C E I L I N G = 29.06299
2 4 0002 19-293 29.341 3 O t 3776
- N E W 'TABCE' FOR' I182 IN' RECURDS 2 4 6 7 '2473
REPLACING HOOE 1x82 FOR w4 . - . . . . . -
-93-
Table 26. INSTALC Summary Showing Overlay P r i o r i t y f o r Par t ic le Mass L i n e s - INSTALC ou tpu t for Table 23
(1 of 7 )
-L ..... ,..--... ..... - ... C B O Y SPkEAO FACT3RS= 0.960 1.030 OVIRLAY J R l O R I T Y 1 182 H HEQ 2 4.002 ;-: 200207 29.764 274 ? E O 8
F E W TABLE FOK I 8 2 I N FBC3FDS 1919 1F26 --I- ................................. f3-b .-- - *-..-.t&--ap-h*-l -
_- -... ...............
-94-
Table 26. INSTALC Summary Showinq Overlay P r i o r i t y f o r Particle Mass Lines - INSTALC ou tpu t for Table 23
( 2 of 7 )
....... __ . - ........... . . . . . . . ........
... .- .. R E R - .
I H l L 5 Z o T P K . . .
8.497 256 3 t 3 4
FE R ~ H I L C ~ .TRK
9.2R 4 259 3 6.34
2634 10.59R 256
l 2 e 3 . 9 6 256 2654
1 3 . 4 0 4 256 3634
YEW Ti l ce FE FL
--.c - c
' C C
3634
... 3c34 .-
-95-
Table 26 . INSTALC Summary Showing Overlay P r i o r i t y f o r Particle Mass L i n e s - INSTALC o u t p u t f o r Table 23
(3 of 7 )
<-.- C
C
RIOPITY I 21.539 256
IHlY1Z.TKK GE R
. . .
3634
3634
3634'
.. .
. ._ .
-96-
Table 26. INSTALC Summary Showing Overlay Priority for Particle Mass Lines - INSTALC output for Table 23
( 4 of 7)
360 2
Table 26 . INSTALC Summary Showing Overlay P r i o r i t y f o r Par t ic le Mass Lines - INSTALC o u t p u t f o r Table 23
( 5 of 7 )
2P.270 K I O R I T Y
30 6 1
3776
l H 2 L C Z .T F; 'RK E F
30 5 I
3776
I H2CCZ - 1 K .c I;
-G K
3 776
7 . 911 2 8 8 3602
,F: lH2L
9. 334 288 3602
13.656 2 E 8 ..... .- ..... __ .
3602 . -
.... _... . . ..-- . . R E R
-98-
Table 26. INSTALC Summary Showing Overlay Priority for Particle Mass Lines - INSTALC output for Table 23
(6 of 7)
IIXtL 016 R 15 e 9 9 0 IC1 572 475 a
9.397
C ECX SPFEkD F A C T ? ~ S = ' 3'.99O - 1.929 . I I 4 2 L N A 2 3 1 1 .-_ ._ 8 L - - __._ f3 ____._._ 329. ...___ 110.1 .A.. _ _ 22.Sf0 10.288
TWRFSUC!LD= NEW T48L E FCf I I A 2 I N F E C G F D S 2088 2092
. .. .....
16.235112 CEI, P I G = 16.57899 . . . . . . . . .
I € . - 2 2 3 283
1 H 2 L C Z TF K Q F F
14.575 288
. . I H 2 Y 12 0 TPIC
RE R
. . . . .
. . . . . 360 2
3602
36Q? . .
360 2
Table 26. INSTALC Summary Showing Over l ay P r io r i ty fo r Particle Mass Lines - INSTALC output for Table 2 3
( 7 of 7 )
. . . 360 2
-100-
Table 27. INSTALC Summary Showing Over l ay P r io r i ty for Particle Mass Lines - INSTALC o u t p u t for Table 24
(1 of 12)
IHlLCZ QTRK F F F
10005Q0
22 e
22 6
2% 6
736
736
Table 27. INSTALC Summary Showing Overlay Priority for Particle Mass Lines - INSTALC output for Table 2 4
( 2 of 12)
C r r
1 . 0 2 0 R. 763
€ 7 1 1 6 7 4
2 /9 /81) TI< a SO. 93900
LOW G4IV . T P 4 C < FI , , F
80.939 769
I H 1LCZ T R K F E E
50
1 . 0 2 3 12 .641
4 7 2 2174
1 1 8.806S9
L C 3 W G 4 I Q
118.807 768
R E R I H I L C Z . T F K
5 0
r
' P I T P I T Y 1 4 5 . 7 5 5
I H l L " . I . T F
2 7 5 q
r y F ;
51'
-102-
Table 27. INSTALC Summary Showing Overlay Priority for Particle 1las.s Lines - INSTALC output for Table 24
(3 of 12)
4
-103-
Table 27. INSTALC Summary Showing Overlay P r i o r i t y f o r Particle Mass Lines - INSTALC ou tpu t fo r Table 24
(4 of 12)
56 C
560
56 0
5 6 0
560.
50
53
Table 27. INSTALC Summary Showing Overlay Priority for Particle Mass Lines - INSTALC output for Table 24
(5 of 12)
5 6 0
-105-
Table 2 7 . INSTALC Summary Showing Overlay P r io r i ty fo r P a r t i c l e Mass L ines - INSTALC output for Table 2 4
(6 of 12)
- @ C Y S'T.EbD FACT??:= 3.980 1.323 C V E K L A Y = R I O ? I T Y 1 .
C I 1 % 1445 4 2 167 L 532 16 3 1 . 9 R 0 92.971 234.683 256 560
NEY TAB1 E FDF I R J IW F e C " f 3 ; 2242 2244 1 3 R E SHI11. D= 92.Q7?90 C E I L I N G = C E D L A C I F'G *FOE I n 3 Fm= 3 32
234.21 999
t C DETECTOF FILE I H I H I Z . D E ~
1 I SEE H E T l C 4 L 13 ( E V T E F E 3 2/9/Rl ) TH< 9
C O - S T O F P I F ! G L C W G A I N c
r T R 4 C Y = I , F 1HlHIZ.TFK PE R
c c
793 L T I * -
NE* T A E L E FOF. I 8 3 IN RECCF35 2251 2252 THRE SHK'l O= C I I S E E H E T l C A L I 3 ( E V T F F E 3 2/9/l31) T i < R 5 DETECTPW F L E I H l H I Z .DEr . TQ&C< F I - E I H l H l Z .TPK - 8 - S T O F P I W G C C BCX S P F E A D F L C T P F S z 0.4t .O 1.520 O V E R L A Y Q F I O R I T Y 2 I R ? 1 C E T ? 24 51.940
NEW T A B L E FCF I83 IV F E C C F D j 2253 22535 T H f i E S H P L D = 11 I e24 103 CEIL I N G =
C D E T E C T O F F ILE I H l H I Z .DET * T R A C Y F I - F IHlHlZ.TRK c B - q T O P P I U G C C I B I L FESh
E I I X SDREPC) F C T T ? e F . y 3.900 1.020 T V Z f i L P Y P R I C R I T Y 3
W"J T A R L E F C F In3 IF! TECPFT)'i 225€ 2258 T L( RE SHOC. 0- 116 -67739 CE I L I N C = K F C L A C I N ' G Y C D E 193 FEZ FF56
299.67281
C 1 I S E E HET1 C A L I 3 (E ' ITTFE3 7/9/81 ) TH< ? C O E T E C T P C F ILE 1HlHlZ.DFT r 8 - S T P P P I K G C
RCY S'PEAD FACTCDSI- 3.980 1.020 C I V E K - P Y P F ! O C I T Y 1
-3 32 2 2481 22 47.950 105.617 269.359 259 5 6 0
4
1 3 5 . 6 1 5 3 9 C E I L I N G = 268.88989 CE 9
1 1 w G A I h '
99 32 2 2841 111.241 284.987 259 560
Q
c 1 I S E E HETl C A L I 3 (EVTEECr'D 2/9/81 ) T i < 9 2 e 4 . 5 3 1 9 ~
RE: R
LCd G41'1
101 32 2e 55 .930 116.678 300.166 259 56J
2 3219 4
kF R * T c A C < F I - C 1 H I t ' l Z . T S Y
1 . m C 9 I V
Table 2 7 . INSTALC Summary Showing Overlay P r i o r i t y for Particle Mass Lines - INSTALC output for Table 24
(7 of 12)
19 4
194
194
70 4
70 4
70 4
7 5 0
re
-107-
Table 27. INSTALC Summary Showing Overlay Priority for Particle Mass Lines - INSTALC output for Table 24
(8 of 12)
T HFiS 5HC1 D= NEW TAB1 E F C F I I A 3 I F ' F FC!?FD3 2 2 8 7 2 2 8 7
C I 1 I S E E HET2 C A L I n ( E N r F r E 3 2 / 9 / 0 1 ) THK 5 7.37593 C E I L ING= 67.71 1 0 0
C DETECTCF F I L E 11-42-77 .DEr . T D ~ C < F I - E 11421 n-r .TFK [: . A - S T C P P I N G C C W7 S P R E A D F A C T ? P 5 = @ e 9 8 0 1 e023 I I A Y L REO 4 9 . 0 0 0 8.811 31.?48 900 1 8
FF R
LC;W G 4 1 N
93..329 B O O 1 8
I H 2 L C Z .TFK R F 9
-108-
T a b l e 27. INSTALC Summary Showing O v e r l a y P r i o r i t y f o r particle Piass Lines - INSTALC output for T a b l e 24
( 9 of 1 2 )
3 57
1
-103-
Table 27. INSTALC Summary Showing Overlay Priority for Particle !.lass Lines - INSTALC output for Table 24
(10 of 12) -. r.--rr.-r-.-, "~~,~.-~,.~~.~~r-IL-)-."i"....:-_i .. . . . I < :. I . %*.&+ -... :..-YCIII..
C T 1 9 7 L = l o
RclX S3FEA3 FAC
- C a
L nW G A I V
c RCY SPREAD FACTCFS= 0.9~jo 1.070 r v z x r . ~ D F I C F I T Y 2 1 1 9 7 1 V E 3 0
99 s 13 19.990 70.515 173.001 290
2 6 9 6 4
529
5 1 8
52 8
528
1 8
1 8
1 9
1 9
-110-
Table 27. INSTALC Summary Showing Overlay P r i o r i t y f o r Particle Mass Lines - INSTALC o u t p u t f o r Table 24
(11 of 12)
C C I I171 C A $ O
f f Y SsPEb.7 F b C T ' ? S = 00980 11.020 ? V E n , b Y D C I O F 1 T V 2 23 39 -960 21.451 219.973 A 0 0
NEW T A B L E FCE 1 1 A 3 IN CECOFIDS 2343 2345 T H f F S H r L D= 21 e45799 C E I L I t ' G = 21 8.97290 PEP1 C C T F G W r D E I I I 3 FPC CC43 C - I 1 19EE. -!+ET2 EA+- I R f E U T E P E D 2/9/81 t TH< 9 C D E T E C T r F F I L E I H 2 H I Z .>El C C
A - S T P 3 0 I b l G 1 Q# G P I Y
C BCY S P R E A D F A C T r P S = 0.5eO 1.920 F V E R L A Y 9"lCr I T Y I I I A3L --T.IOR..-. . . .. . 1 2 - 470950.
VEW T A B L E F O F I I43 l U c c f P T . > f 23415 2347 J H FE S+PL D= 21 015399 C E I L lNG= 219.91193
? D E T E C T C F F I L E IH2HIZ.>El C P Z S T O P P I W G c C ... B Q X . S P K E A D . F A C T 3 R S = 0 - 9 8 0 1.020 J V Z f i L A Y P R I O R I T Y 2 I 1 A 7 L Cfie2
qrl 32 N C V TAPLE F O P X143 IP' F E C P P D S 2348 2349
I 267 1 4
C 11 ISEE H E T 2 C A I . . I E ( E F I T E c E 3 2/9/81) TH< 3 THRC'=HflLD= 22 . D 7 ? 9 D C E I - I N G = 232.405C5
12' I C P 13 36 4
P F 0 e T Q 4 C < F I - E 1 H 2 H I Z .TCU
7-4 32 1 2333 . 21.lbY 219.912 a00
4
I 1 I S E E H E T 2 C A L W ( E W E F E D 2/9/81) TH< 9 I-!? R . r n A C < F I L E I H ? H I Z .TRK 1 f3Y G A I V
24 51.940 22.033 232.406 303'
F F C 9 TPACC F I -F I H 2 H I Z e T F K
-111-
Table 27. INSTALC Summary Showing Overlay Priority for Particle Mass Lines - INSTALC output for Table 24
(12 of 12)
c C W Y 9 3 F E P . D F P C T ? Q S = 0.900 1.020 O V E C L A Y P K I O F I T Y 1 r 1071 m 3 h 13
1 1 1 1 5 i! 1764 4 35 -970 97.937 251.621 290
NEW T 4 R L E F C C I I R 3 I V I 'ECZRDS 2 3 € 6 2368 T HRE SHCl D= 07 e Y 3 h o 9 C E I L . Il : t= 2 5 1 . 0 . 3 4 0 0 C I f ISEE H E T 2 C A L I R ( E M T E F F D 2/9/81) THC 9
c c IXTECTCF FI-E 1 ~ 2 ~ 1 2 .mr
R F R
C (I I I R T L C R S 2
R f V S F E P D FPCT?:5- 0.980 1 . 3 F O 3 V E K - a Y D Q I C ' ? T Y 2
e9 2 4
32 NEW T68L E F C F I I R 3 1'4 CECORDS 2374 2376 TL) FF SHOC D= 107 - 5 3 3 9 7 C E I L I S G = 204.41 187 C 11 I S E E H E T 2 C P L I S (EFJTEFED 2/9/81) THY R C D E T C C T O P FILE I H 2 H I Z .3Er C A - -STOoPINC C C 0Pv S P G E A D F A C T P R 4 = 0.980 1.020 V J I R L A Y D F I l ? R I T Y 3 I I S T L FE56
NE* TAP! E F@C I I A 3 ' - i V C E C t ? O 3 5 2377 2379 THFESHPI D- I 1 1.35399 C E I L Ip.IG= S E O L A C I N G WCDE 1183 F O O F E S t C I 1 I S E E HE12 C 4 L I R (ENTEPE9 2/9/01) TH< '3 C D C T E C T r F F I L E I H 2 H I Z . D E T C 0 - S T O J P I V G LOW SA14 c C BclX S-F-EAD FACT,"RS= 0 . 9 8 0 1.020 O V E R L A Y D R I C R I T Y 2
5 1.940 2 2 R 7 7
109.600 784.860 290 4
*E R . T P 9 C < F I - E 1 H P H I Z . T R K
L O W G 4 1 N
lQ1 . 32 26 5 5 . 9 3 0
2 3281 114.951 30 '0 .032 290
a .
299.51784
R E fi r T R P C < F I - E I H 2 Y I Z . T F K
T I P ~ L N I ~ F ) 1 1 7 3 2 T 3 E 1 4
2 8 5 7 . 9 4 0 1 2 2 . 4 6 2 3 2 1 . 3 4 5 290
ME* T A B 1 E FOP I183 1 4 CEC3"05 2380 2383 T H FF SHOl O= 1 2 2 . 4 5 1 3 7 C E I - I ? ' G = 320.89786
II DETECTf" F I - E IH2H I Z . 3 E r
4
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520
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-112-
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Figure 29 . Computer Generated Track f o r A1 vs C 1 2 3 High Gain, C X P = 1
-113 -
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Figure 30 . Computer Generated Track fo r Proton Mode I B 2
-114-
' . 3rJ: .....
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i v D 4 i l a 1bG i U V 2'11) iau I O U 4 4 i l a b h "
Figure 31. Computer Generated Track f o r I31 vs B2 Low Gain Nodes -115-
- * e & / , 51-a,c/
... r~~,- l / . . . . . . . . .~. . . . . . . . . . . . . . . . . . . . , . . .~.* . . .* . . . . . . . . . . . . . . . . . .* . . . . . . . .* . . . . .* . .* .* . . . . . . . . . . .* . . . . .*- . . . . . . . . . . . . . - . . .
, - -. b .. - I
Figure 32. Conputgr Generated Track for R 1 vc, C432 Low Gain Modes
-116-
f
'lhe pcnetratinq track d e f i n i t i c n for the mode IPB low q a i n a l p h a TBACK is 5.hown in .tke fc l los r ing pages. T h e time p e r i o d sa%;lmarizcd f o r t h i s d a t a is t h t t g i v e n in T a b l e 3 of t h i s ciocaneut.
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-121-
-122-
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1
c C ELEM
2! c1 c 2
c 2 c 3 e 3 c 4
c 4
R2 0 1
C C CHANNLS
4096 4096 4096 4096 4096 4096 4096 4096 4096 4096 4096
NO. THICK PMP-AST 0 16
2 151 1 14A 3 2920 0 8 1
3 4 2925
7 D 1 7 1
4 4 2900
7 5 2939
4 0 143
5
5 291P z 6 2925 0 140
6 6 2935
1 0 68 9 7 1930 8 1915
1 1
0 33
i
0 84 4
OFFSET 0 . 0 0
FSMEV
0 . 0 0 4096.
0 0 0 4096.
e 00 4096. 4096
.oo 0.00
4096. 4096.
- 0 0 ~ 4096. 0.00 .oo 4096. 0 . 0 0 4096.
4096.
0.00 4096.
LOW GAIN
RST 7 7 7 6
5 7 7
4 5 7 4
7 3
3 7 2 1 7 7
PEN THRESHnLDS SPACING 7 0 3 7 2 7 5 7 5 4 7 4 3 7
.63
2.5 .62
4.60 4.68 4.66
4.66 4.69
4e69
2e13 1.02
: 1 ; .5
92
o 92
92
92
92
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03 .3
OFFSET FSMEV 4096.
d 4096.
6. 4096.
0 . 4096.
0 . 0 4096.
0 . 4096. 4096 e
0 . 0 0 4096. 0.
0.0 4096. 4096.
0 . 0 0 4096 e
H I G H GAIN
2
68314 2592
1851 0
671 672
1851 671
l 8 J l 672
671 672
247; 5 3 6 o i
0 0 0
RADIUS CIJRV 15960 15960 t 15960 1 17131 1 17131 1 11131 1 17131 1 17131 1
17131 1 17131 1
17131 1 17131 1 17131
15960 2 15960 3 15960 3 15960 1
175Zl 2 3
AST A 1
AST C l AST A2
AST c 2 AST c 3 PEN S EST B l BST 92 PEN S EST C4 PEN & BST C3 PEN 6 SST C2 PEN C l
SLAYT 1 C 1 2 BOTH GN C H 1 CHZ CH3 SUM C H l CH2 CH3 SUM
SA1 SL2 SA 1 1. S6 53 2
. .375 -39. 1. 6 5.43 -105. s0 S R 2
1. 1. 1. -60. 1. 1. 1. -60.
SLANT 2
-125-
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-126-
ra Y
X 0 (J K
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-129-
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-132-
-133-
x x %X x x xx
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-137-
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0 U
W e e w w W o e ~ o m m m m m m m
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N 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 ~ N Q W W ~ Q O ~ W d U W W ~ ~ ~ O d ~ ~ ~ ~ ~ O ~ W ~ N ............................................... ~ O O O O O O O O O O O O O O O O O ~ Q ~ W F ~ d N ~ ~ ~ ~ W O d ~ d O ~ N ~ ~ ~ W W ~ O ~ ~ U . .
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1 h. c I-, Lr
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x % X x x
-141-
x x % X x x %X
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-142-
~ N N N ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ d ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ ~ O O O O O O O O O O O O
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N 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 O O O O O O O O O O O O O O O O O O h W W d ~ ~ h N d O O N O P d O W N P N P N W ~ Q ~ W N ~......................................***...*...*...........*.*.... ~0000000000O0030O000OOOOOOOOOOOOOOOOCOO~PNWO~~~WhNOPON~PON~PONOPh~
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-150-
-151-
. f
;jC.XGEi?J o u t p u t Los all 3 - d i m ~ n s i c n a f s t o p p i n g ittoaes, v h i c h
was used to o b t a i n DEAI) LAYES fiffiits, is ' g iven in the
F I L E 1 - 7 1 RECOROS TN 1 HLOCKS c I ISEE H E T l C P L B (EPITERED 2 / 9 / 8 1 ) MODIFIED F R O N WCOR,l 06-JAN-83
C DETECTOR FILE ICIGf.DET C A - S T O P P I N G
,TRACK F I L F 1 C I D E A D . T H C H I G H G A I N
4:
4
6 5
7 8
1 0 9
11 12
1 5 1 6 1 7 1 8
2 0 1 9
2 1
2 4 2 5
2 7 2 6
2A 2 9
3 1 30
32 33 3 4 3 5 3 6 37 33 3 9 4 0 4 1
43
4 5 44
46 47 4R 49 5 0 5 1 52 5 3 5 4 5 5
57 5 h
S,! 5 9 6 0 6 1 6 2 63
6 5 64
H
53
4 2
L * IA3H PROT 3 2
6 4 1
3 2 3 4 5 - 6 7 8
10 9
11 1 2
1 4 1 3
1 5 1 6
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2 2 2 1
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3 0 29
3 1 3 2 33
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4 1 40**
4 2 43 44 45 46 47
b 2 * *
1
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3 3 35
3 1 29 2 7
23 2 2 2 1 20 1 9
1 7 1 8
1 6 1 6 15 15 1 4 1 4 13 1 2
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11 11
1 1 1 0
1 0 10
9 9 9 9 9 8
8 8
8 8
8
7 R
7 7 7 7 6 6 6 6 6
6 6
32
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6 6 6
1.007 1
43 42 40 38 3 5 3 3 3 1 30 28 2 6 25 2 4 2 2 2 1 2 0 2 0 19 1 8 17 1 7 1 6 1 6 1 5
1 4 1 3 13 1 2 1 2 1 2 11 11 11 1 0 10 1 0 10 10
9 9 9 9 A 8 0 A R
7 R
7 7 7 7 7 7 7 5 6 6 6 6
tl
a a
64 6 6 5 7
4 4 5 0
3 6 3 9
3 3
2 6 2 4
2 1 20 19 18
32! 3;
fZ I S 15 1 4 1 3
1 2 1 3
1 2 1 2
11 11 11 11 10
9 9 9 9 9 9 9 9 8 8 4
8 8
8 R 7 7 7 7 7 7
7 7
6 6 6 6 6 6
6 6
6.3f36 6
8 2 7 1 6 1 5 4 48 43 3 9 3 6 33 3 1 29
25 27 2 4 23 2 1 2 0
1 R 1 7 17 16 1 6 15 15 1 4 1 4 1 3 1 2 1 2 12 1 2 11 11 I 1 11 10 10 10
9
9 9 9 e A Ec
P R (1 A
7 7 7 7 7 7
7 7
7 6 6
1:
;
SR.510 43
6.386 6.578 h.M90 7.290 7.763 R 292 8.870 9 406
101134 10.809 11.5@5 12.219
13.693 14.450 15.213 15.9R7
17:553 1 6 7 6 7
19.949
2 1 559 22:371 23.185 24.034 24 940 26.475 27;258 211.056 ?ti.P69 19.693 30.521 31,355 3 1 1 9 3
33 077
35.655
38.304 37.560
39.071 39.856 40.655 41.463 42 279 43 '125
44.378 44:033
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c 1 ISEE HETl CALI@. (ENTERED 2/9/@1) HODIFIETl F R O M REOP,l FILE 5 - 284 RECORDS IN 3 RLOCKS 06?JA#-83
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56.500 56:318
56.863 57.232 571 604 57:791 57.977 58.163 58.285 58.292 58 300 58:482
59:049 59.239 59.430 59.621 59 813 60 196 60'388 60:772 60.965 61.159 61.353 61.547 61 741 61 :935 62.129 62.324 62 520 62:715
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-171-
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-172-
PREFACE
Appendix G of t h e C a l i b r a t i o n of t h e High Energy Tele-
s c o p e s f o r t h e Voyager and I S E E Cosmic Ray Experiments
(CSC/TM-81/6280) has been expanded t o i n c l u d e a d i s c u s s i o n
o f t h e . r a n g e - e n e r g y r e l a t i o n . The a t t ached pages sh6ul.d
r e p l a c e t h e c o r r e s p o n d i n g p a g e s i n t h e o r i g i n a l d o c u m e n t .
Each r ev i s ion i s marked by a v e r t i c a l b a r i n t h e r i g h t
m a r g i n ; t h e d a t e of t h e r e v i s i o n i s shown- in the lower
r i g h t c o r n e r . The o r i g i n a l COMDEX number on t h e document
cover and t i t l e page should be changed to CSC/TM-81/628OUDl. , r
a
Revision 1, March 1 9 8 2
Revision 1, March ,1982
Proyraras o n the PDP 11/70
D. V, Eeames
P r o j r a a s have been written on the POP 11/70 t h a t allow gene ra - t i D n of rG:sponse t a h l 2 . s (g9boxesTT) for p a r t i c l e telescopes %hose S o B y l e x i t y does hot excee8.i that of t h e Voyager-ISZZ HET tele- sc3 p o s , Response is based upon an i n t e r n a l l y geuerated range/enecqy r e l a t i o n . , ~ D K s i l i c o n tbaL is ca l ib l - axed t o a f e u p e r c - c n t azcuracy €or p a r t i c i e species iron p r o t o n s t h r o u g h Fe at ewrqi s s from belou i HeV/AZU t h r o u g h ionization minimum (2.4
GeV/AHU) Zeavier s p 5 c i e s and t h i n n e r detector eleraents { < l o mi- c r o n s ) m y a i s o be ussi i t b u t with greater unce r t a in ty .
The pfaqran T E j T A ~tccepts a i e t e c t o r d e s c r i p t i o n . f i l e as i o p u t
dnd produces c a i c u i d t a d track f i l e s on disk f o r the detector .nod- es aud parr ; ic le ' speci2.s C e q u e s t e d .
The p r o q r a n PLOTPS uses . t h e t r ack Eile frorn TES1'A to produce
any nuaaber o€ p r i n t e x p l o t s of theore t ica l r a s p o n s e imtrices. , t he desir32 p l o t s afe selected interactively a t the CH'r" terminai,
The proqram S O l l G E X DL- AUTOBOX uses the track r i l e data fron TESTA to qenerate respouse t d b l e s in a f o r a s u i t a i t i e f o r i n p u t to t h a F L X P i i p r o q r a n on the I B E I 3 0 0 .
Revision 1, March 1982
fllost of the p h y s i c s of the detector s y s t e m a n d its response to p a r t i c l e s is 4eterQiaed by t h e TESTA progratcr; the main . t a sk of th2 othsr programs is to reformat t h e outpnt fxon TESTA,
g : I
The i n p u t to TESTA is a detector description f i l e s u c h as t h a . c
shown in F i g u r - e 12 b. Becords b e g i n u i n g xith C in the first cul- uan are t r z a t e d as c m r n a t ~ and are n o t ana lyzed by the program. A file for a new deteztDr is most e a s i l y created by copying and editificl d n old f i l e , u s i o g the commented colulan h e a d l n g s as a
t a n p l a t e .
_ _ m 1. f c a c u r e s of ~ : ? a detector file are as foilous:
part oE a n o u t p u t l v n u i e name*? to s i g n i f y telescope nuraber. The rwnainder of the r e m r d is a descriptive t i t l e that appears on gil c a l c u l z t e d output from a_i& 11/70 pror;rams based on this file. A a d i t i o n a i da t a ( r ange /ene rgy version auri f i l e mine) are l a t e r a p p e n d e d ta t h e t i t l e , b e g i n n i n q in coluan 58.
Revision 1, March 1982
2_,1. 3 g g t g g t z ~ = ~ ~ e e r aecagcis: one r e c o r d L O T each i t i u t i n q u i - I s h d b l c p h y s i c a l iaye.r i n t h e detector (maxiruuta 1 9 ) These re- c o r d s i n c l u d e a 2 charactec eletnent fldue a n d nuntber for each 6 k c t r i c a l l y lefineil 3 c t i v e element (r~zximuut 8) or Dlank and zero t o r dead l a y a r s T i t r e s h o l d e n e r g i e s a r e also s p e c i i i e d f3eV) in h i q h and 1311 g a i n f o r a c t i v e e l e n e n t s . E Y ~ E ~ l ayer is uef iced by a t h i c k n z s s , s p a c i n g to the n e x t l a p e r and r a u i u s , a l l i n mi.- czaris, a r i l d curvature i n d e x for c u r v e d e l e n e n t s . T h i c k n e s s e s need not h e i a teqafs , C o l u m n s 4,5 and 6 con tc i in pointers t h a t
d e f . i n e how t h e s i q n a l (the e n e r g y d e p o s i t e d in each l a y e r ) will De summed i?y p o i n t i n g to d samaing r e g i s t e r for e a c h mode. LAn a t t e E p t is made tr> duplicate t h e p r e a m p i i f i e r - s u m m i n g ampilfier- Pti4 c o n f i q s r a t i d u of a aET), akqisters number I and 2 u i l l be- COEE the ts> "delta E" eleiaerts. Both must exceed threshold to form a coinc idence , Bsgis te r 6 sums t h e a n t i - c o i n c i d e n c e signal, d l s t i n q u i s h i n g s t o p p i n g a n d p e n e t r a t i n g particles. E n e r g y depos-
i t e d in rcqisters 3 , 4 and 5 vilL .be c o n v e r t e d t o channels a n d than summe5 to prsduc= . . t h e W E ' $ p u l s e height. Register 7 coliects t h e u n o b s e r v e d snerqy frortl d e a d layers ,
Revision 1, March 1982
CH 1 * deita E l + C J t * d e l t a E2 + CH3 * E + SU9
~ i z k . ~ C Z B S S to a d e t e c t o r file, TdSTA proceeds 1;o calculate t r a c k d a t t i €or each qain and species l i s t e d on the file. For each such cAse, t h e s u b r o u t i n e TABLZ is invoked t o generate a ranqe/euzrqy t a b 1 2 t h a t will be u s e d f o r a l l uetactor modes re- q u e s t e d ,
F o r each deteccor model, t h e pfoyram first uaps the detecr;or
by surnrsing t h e t h i c k n e s s e s in t h e p r o p e r a i r e c - L i o n to d e t e r m i n e t h a p a r t i z l a ranqe t3 each p h y s i c a l . b o u n d a r y of che s y s t e m i r o n the f i r s t c o i n c i d e n c c (eleraents 1 and 2)' to t h e a n t i - c o i n c i d e n c - c s [elenegt 5 ) oc t 3 i o n i z a t i o n minimum f o r p e n e t r a t i n g parti- zhs. Ear t h e f i r s t ioter€ace with each active eleraent, the
range is then modifie,! s o t h a t t h e enexgy d e p o s i t e d i n the aetec-
to r exceeds t h r e s h o l d s .
Revision 1, March 1982
Each r d n g e p o i n t also corresponds to a g i v e n d e p t h i n the de-
tector uber; detcstor s p a c i n g d a t a are included. The d e p t h and detuctjr rsilii d e f i n e a iaaxiIl;lum inclination a n g l e aaa f o r r'iat aetectctrs, t h e respDnsc of a par t i c i a a t the uaxiaua a n g l e is c a l z u l a t e d For cucwed detectors, the "ex t r eme r e s p o n s e " curve ~ e p e n d s u p 3 u the c u x v a t u r u and a first orde r approximation f o r dET d e t e s t 3 r s is i n t e r n a l l y seneraced by TESTA,
A g e o n e t r y fac tor is also d e f i n e d at sach c a l c u l a t e d d e p t h . A
tin-concentric -element geometry factor is cafcuiated u s i n g radi; ~i che front aetector ( f i r s t detector with sum register pointer not equal t o 71, a n d the c u r r e n t d e t a c t o r for the Last detector p o i n t e r n o t equzl t o 7)'. The geometry factor is calculated a s shown in F i g u r e i of tht? indin documeat,
The c d l z u l a t i o n stlrts at the front of t h e t e lescope and pro- ceeds to greater and greater d e p t h . T h e geonetry factor a t d
q i v t t n d e p t h is taken 3s the minimum of t h e current ana p r e c e d i n g ones i n order to compensate to f i r s t order for detectors with l a r q e - r a d i u s s lements t h a t do not define the geometry.
ces requires an accur3te d e s c r i p t i o n of t h e s t o p g i n g process from 5bou.t 2 0 k z V / n u c i 2 o n f o r Iron n u c l e i in t h e f irst c h a n n e l of t h e VLET f v e r y lou e n e r g y t e l e scope ) t h r o u g h minimum i o n i z d t i o a at 2.4 SeV/!tuzleon, A t h i q h e n e r g i e s t h e stopping process is veil aescrihed b y t h e B Z l t I E - B L O C K f o r u u i a . Bodif i c a t i o n s of t h e i r formula a . l lou it to bz e x t a d e d down to energies where the p a r t i -
Revision 1, March 1982
c l e c a p t u r e s the f i z s t few o r 5 i t a i eiectrons. A t 'low energies u h e r c the b i n d i n g of o r t s i t a l e l e c t i o n s is approximatea by t h e Lbmas-Eermi moiai, he electronic s t o g p i n g power is appronimate-
l y l i n e a r in v s i o c i t y and a more colnpiex but v e l 1 aescribeii uu- c l e a r stopping power u e q i n s to d o n i n a t e the energy l o s s process.
( L i n u h a r d Scha r f f a n d S c h i o t . t , 1963, i * L S S I J )
throuqh d afclxiaam, i t is comaon to use empirical p o u e r lag expan- s i a n to f i t t h e i~easarements leg. R o r t h c i i f f e E S c h i l l i n g 1970)
i n t h i s work , ut? have preferred to modify t h e h i g h and low energy torms i n t 2 better aJreement and to u5e an empir ica l w e i g h t i n g
r'actor to s h i f t be tween them i n oraer to nerge smoothly l n t o t h e correct asymptotic LzehaiviDr.
T h e Thu inas -Fean i s - t d t i s t i c a l model of t h e atom resu1z.s i n a sinooth i l ependecce o n t h e atoiaic nuuber of t h e particle and of t h e stoppinq ma.teriaL. A Eore d i s c o n t i n u o u s b e h a v i o r a r i s i n g fron atontic s h e l l e f f e c t s has been ouserved jcf eg. . Z i e g i e r , 1378),
de h a v ~ inc lu i ie i a smdll eap i r i ca l c o r r e c t i o n ters B [Z) iu t h e e x p r r s s i o n €or t h e character is t ic v e l o c i t y of each eieraent to
cover a n y res idua l e f f e c t s of t h i s k i n d . This factor is found t o
vary more s r s o o t h l y thtrn e x p e c t e d and t o peak for S i l i c o n ions (stopping i n t h e Si d a t e c t o r s )
T h e available d a t a for i o n s s topping i n Si [or A l ) have been
considered i o d e t e r n i n i n g the fit constraints as well as da ta
from t h e ISEE- VLXT'r; which constrains the range e n e r g y T O T the heav ier elements withio an accuracy of 2 - 3 5 ,
Zarafiteters of t h e stopping Hiaterial, S i , are e x p l i c i t l y in- cluded i n t h e i o r m 1 i s a a s Z ( s t o p p i n g ) , B [ s t o p p i n g ) , t h e mean i o n i z a t i o n p o t e n t i a l , L ( s t o p p i n g ) = 1 7 3 . 5 eV and the d e n s i t y , p (stopping) = 2, 33 g/:m . However the adequac.1 of t h e fit fo r o the r inaterials h a s n ~ t b e e n s t u d i e d and should n o t be ausuued,
z
Revision 1, March 1 9 8 2
page i 7u
Our f a r & of t h z i3ETB2-ULOCK expres s ion wi th c h a r g e p i c k u t j ciif-
f e r s sliqhtly frou c h a t q i v e u ir B i c h s e l (1970) Let b hi2 t h e
particle v e l o c i t y (in u n i t s of the v e i o c i t y of light,^) ctnu Z itncl A be its A t o m i c n u n h e r and w e i g h t , r e s p e c t i v e i g . Let
characterize . tb2 par t ic les ' o r b i t a l elec-tron v e l o c i t y u h e r e 3 ( 2 )
is a paramatcr of orler 1 d e s c r i b e d pr2vionsI .y and g i v e n DY t h e
rab ie :
z z z
13 1 4 15
i .og 2 2 1,062 2 3 1 .O 24
7 . 4 7 5 16 1 I 0 25 8 .975 17 i .o 2b 9 - 99 19 1.0 27
is
B B
u h e r e , w ~ is t h e e lectron mass,
anu thg c o n s t a n t
Revision 1, March 1982
m L ~ A S ' l a t t e r v a l u e g i v d s units of Me'V/miuron u s e d i n the programs.
I n z l u d i n q t h e one i n t h e l o g a r i t h m p r e v e n t s a d i v e r g e n c e a t Lou velocities b u t b3s a i s o s t no effect i n tile r e g i o n v h e r e t h e
BETHE-BLOCK forut iiotuina.tes
Senerally s p e a k i n q , the BB form r i l l 5e valid for a > d 5 [see
eqo. I ) 3ud the LSS f o f n will be v a l i d for p <?*. Since t h o
t r f n s i t i o n a p p e a r s i a p r a c t i c e t o depenii on t h e electron charac- t e r i s t i c s :;f .thl t a r q a t a s uel l as t h e projec t i le , we define
/ " f
The f o l l o w i n q mod i f i ca t ions are Bade to t h e LSS form:
1 , A constant m u l t i p l i e r of t . 34 is i n c l u d e d [ o t h e r a u t h o r s
h a v e also found g q u a t i o n 8 to underestimate che s t o p p i n g pitid<?'?) .
3* A n e x p o n e n t i a i t h c t D C , s i m i l a r i n form t o t h e u e i g h t f a c t o r
Revision 1, March 1982
p a g e 172
I 1.133
The c o n t r i b u t i o n to t h e energy l o s s from nuclear : c o l l i s i o n s wds o b t a i n e d by f i t t i n g the T h o m a s - P e r d . s c a t t e r i n g f u n c t i o n [see
iSs f i q n r e I ) to t h e erupiricai form
f ( x ) = (. 077) [in;4SOOx) ) / ( I + 1,253~) (10)
an3 i n t e q f a t i n q to o a t a i n t h e d imeLs ion ie s s s t o p p i u g power
where
k' = 3 A X f. d 0 7 8 t 4 , C, 4: E/A ) (13)
i n t e r a s of t h e p3 i r t ic le a n e r g y E, and the constanzs d e f i n e d ia equat ions 12 anu 13 (ire
and
F i n a l l y , the f n i i ene rgy loss is d e f i n e d to be
' 06 I tu&.+ Revision 1, March 1 9 8 2
usir;c; an algorithm d e s c r i b e d elsewhere. The e n e r q y Loss Eo.rntalism d e s c r i b e d h e r e i n reiates t o programs
and output d e s c r i b e d 1s v e f s i o n SIB". Ear<lier (or l a t e r ) v e r s i o n s aay i n v o l v z a comple.ta1y d i f f e r e n t parameterizatiou.
* An output file n m 2 Any v a l i d file name may be e n t e r e d ; ISAE
c o n v e n t i o n U S ~ S d f i l e type .TBK w i t h n a m s L i k e l.CkiSET1. TBK.
The proqrara m a y . ~ e terairnated by entering d 2er iod l a s t e a d of a file ntlnie,
* An i n p u t detector f i l e maie (e.g,. XCALTI. DET)
I. S t e p p i n q p r e c i s i o n i p e r c e n t channel change per s t e p ; default 5 %)
* P r i n t conpress ion f l a q : trne- p r i n t every Line; f a l s e - p r i n t
e v e r y o t h e r s t e p for s i n g l e mode te iascupes, e v e r y 4th step for rnulti-rno.7e telescopes. This c o n t r o l s p r i n t e d output oulp-, itli s t e p s are recorded 3n t h e track f i l e . i ? a n g e / e n e r y y f . laq: true- a one p a g e coruplete r a n g e / e n e r g y loss t a b l e will be produzfti; for each p a r t i c l e species In the detec-
t 3 f fil2. A f u r t t i 2 r prompt for new values of cons taot s should b e d e f a u l t e d { / r e t u r n ) ; f a l s e - no 8-E table output
Revision 1, March 1982
page I74
T h e range j a e p t h ) in u.icrons The par t i c l e c n e r q y i u EeV/AEU
T h e r e s p o n s e f c h a n n a l s ) * The r e sponse [chan;ielsi) * The response c h a r n e l s 0
T h e name of a p h y s i c a l boundary when f i r s t e n c o u n t e r e u j X X for l e a d layers) T h .* dse -. are the p r e c i s e poiuts at which Ehe t h r e s h o l d is 3xcee;iait or the bouI;dary is reached, n o t the neax- a s t s tep .
The came of the s l a t c o n d i t i o n satisfied,if a n y * ha y e o m e t r y - f a z t o r (cis2 s t e r ) * The secant of t h e m x i m u m i n c l i n a t i o n aagle
T h e e n e r g y aslilt c h a n n e l response for the ex t f e se - r e sponse track a t the same d e p t h [three s e t s of eiltries)
The direct-access o u t p u t f i l e r e c o x a s contain s.imilar i n fo r - ination tL) that p. rFnted , The file is headed by i n d e x records f o r each spec ies th3L poiat to the data recoras for each mode.
Revision 1, March 1982