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fe4da5cc | 1 | * |
2 | * $Id$ | |
3 | * | |
4 | * $Log$ | |
5 | * Revision 1.1.1.1 1995/10/24 10:21:32 cernlib | |
6 | * Geant | |
7 | * | |
8 | * | |
9 | #include "geant321/pilot.h" | |
10 | *CMZ : 3.21/02 29/03/94 15.41.23 by S.Giani | |
11 | *-- Author : | |
12 | SUBROUTINE GPRELA | |
13 | C. | |
14 | C. ****************************************************************** | |
15 | C. * * | |
16 | C. * Initialise energy loss due to direct pair-production and * | |
17 | C. * nuclear interactions by muons. * | |
18 | C. * * | |
19 | C * A, Direct pair production <======= * | |
20 | C * * | |
21 | C. * The DE/DX expression of MANDO and RONCHI(NUOVO CIMENTO * | |
22 | C. * 9(1952),517) is used which attempts to account for the effect * | |
23 | C. * of atomic electron screening. The screening correction is * | |
24 | C. * applied above the energy limit defined by C. RICHARD-SERRE * | |
25 | C. * (CERN 71-18). * | |
26 | C. * * | |
27 | C * B, Nuclear interactions <======= * | |
28 | C. * * | |
29 | C. * the following expression derived from the Williams-Weizsacker * | |
30 | C. * relation for the virtual photon flux is used : * | |
31 | C. * * | |
32 | C. * DE/DX = FACTOR * XSEC * E * | |
33 | C. * * | |
34 | C. * where, * | |
35 | C. * FACTOR = 2. * N * ALPHA / PI * | |
36 | C. * XSEC = total photo-nuclear cross-section assumed to * | |
37 | C. * be independent of energy. Value of 140 mubarns * | |
38 | C. * calculated by averaging the results of Hesse * | |
39 | C. * et al(Phys. Rev. Lett 25(1970),613). * | |
40 | C. * * | |
41 | C. * ==>Called by : GPHYSI * | |
42 | C. * Author G.Patrick ********* * | |
43 | C. * * | |
44 | C. ****************************************************************** | |
45 | C. | |
46 | #include "geant321/gcbank.inc" | |
47 | #include "geant321/gcjloc.inc" | |
48 | #include "geant321/gcmulo.inc" | |
49 | #include "geant321/gcmate.inc" | |
50 | #include "geant321/gcphys.inc" | |
51 | #include "geant321/gconsp.inc" | |
52 | #include "geant321/gccuts.inc" | |
53 | #include "geant321/gctrak.inc" | |
54 | DATA XSEC /140.E-30/ | |
55 | DATA FACTOR/2.7976238E+21/ | |
56 | C. | |
57 | C. ------------------------------------------------------------------ | |
58 | C. | |
59 | IF(Z.LT.1.) GOTO 999 | |
60 | ICHAN=IEKBIN | |
61 | T = ELOW(ICHAN) | |
62 | T1 = 10.**(EKBIN(1)+(ICHAN-0.5)/GEKA) | |
63 | IF(T.LT.1.)GO TO 999 | |
64 | E = T+EMMU | |
65 | E1 = T1+EMMU | |
66 | IF(JMIXT.EQ.0)THEN | |
67 | C | |
68 | C Element | |
69 | C | |
70 | DEDX = GPRELM(Z,T,PPCUTM) | |
71 | DEDX = AVO*DENS*DEDX/A | |
72 | * | |
73 | * *** auxiliary integration point for Range tables | |
74 | IF(ICHAN.NE.NEK1) THEN | |
75 | DEDX1 = GPRELM(Z,T1,PPCUTM) | |
76 | DEDX1 = AVO*DENS*DEDX1/A | |
77 | ENDIF | |
78 | ELSE | |
79 | C | |
80 | C Compound/Mixture | |
81 | C | |
82 | NLMAT = Q(JMA+11) | |
83 | NLM = IABS(NLMAT) | |
84 | DEDX = 0. | |
85 | DEDX1 = 0. | |
86 | DO 10 L=1,NLM | |
87 | J = JMIXT+NLM+L | |
88 | AA = Q(J-NLM) | |
89 | ZZ = Q(J) | |
90 | WMAT = Q(J+NLM) | |
91 | S = GPRELM(ZZ,T,PPCUTM) | |
92 | S = WMAT*S/AA | |
93 | DEDX = DEDX+AVO*DENS*S | |
94 | * | |
95 | * *** auxiliary integration point for Range tables | |
96 | IF(ICHAN.NE.NEK1) THEN | |
97 | S = GPRELM(ZZ,T1,PPCUTM) | |
98 | S = WMAT*S/AA | |
99 | DEDX1 = DEDX1+AVO*DENS*S | |
100 | ENDIF | |
101 | 10 CONTINUE | |
102 | ENDIF | |
103 | C | |
104 | C Nuclear interactions | |
105 | C | |
106 | IF(IMUNU.EQ.0.AND.E.GE.10.) THEN | |
107 | DENU=DENS*FACTOR*XSEC*E | |
108 | * | |
109 | * *** auxiliary integration point for Range tables | |
110 | IF(ICHAN.NE.NEK1) THEN | |
111 | DENU1=DENS*FACTOR*XSEC*E1 | |
112 | ENDIF | |
113 | ELSE | |
114 | DENU=0.0 | |
115 | DENU1=0.0 | |
116 | ENDIF | |
117 | IF(DEDX.LT.0.)DEDX=0. | |
118 | IF(DENU.LT.0.)DENU=0. | |
119 | JEL2=LQ(JMA-2) | |
120 | Q(JEL2+ICHAN)=Q(JEL2+ICHAN)+DEDX+DENU | |
121 | * | |
122 | * *** auxiliary integration point for Range tables | |
123 | IF(ICHAN.NE.NEK1) THEN | |
124 | IF(DEDX1.LT.0.)DEDX1=0. | |
125 | IF(DENU1.LT.0.)DENU1=0. | |
126 | WS(NEKBIN*2+ICHAN)=WS(NEKBIN*2+ICHAN)+DEDX1+DENU1 | |
127 | ENDIF | |
128 | C | |
129 | 999 END |