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fe4da5cc | 1 | * |
2 | * $Id$ | |
3 | * | |
4 | * $Log$ | |
5 | * Revision 1.1.1.1 1995/10/24 10:21:23 cernlib | |
6 | * Geant | |
7 | * | |
8 | * | |
9 | #include "geant321/pilot.h" | |
10 | *CMZ : 3.21/02 29/03/94 15.41.21 by S.Giani | |
11 | *-- Author : | |
12 | SUBROUTINE GDECAY | |
13 | C. | |
14 | C. ****************************************************************** | |
15 | C. * * | |
16 | C. * Control routine for generation of particle decays. * | |
17 | C. * * | |
18 | C. * MODE(I) I'th decay mode of current particle * | |
19 | C. * BRATIO(I) branching ratio for I'th decay mode of * | |
20 | C. * current particle. * | |
21 | C. * * | |
22 | C. * ==>Called by : GHSTOP,GTHADR,GTNEUT,GTMUON * | |
23 | C. * Author G.Patrick ********* * | |
24 | C. * * | |
25 | C. ****************************************************************** | |
26 | C. | |
27 | #include "geant321/gcbank.inc" | |
28 | #include "geant321/gctrak.inc" | |
29 | #include "geant321/gconsp.inc" | |
30 | #include "geant321/gcking.inc" | |
31 | #include "geant321/gckine.inc" | |
32 | #include "geant321/gcunit.inc" | |
33 | #include "geant321/gcphys.inc" | |
34 | #if defined(CERNLIB_USRJMP) | |
35 | #include "geant321/gcjump.inc" | |
36 | #endif | |
37 | DIMENSION BAREA(7) | |
38 | DIMENSION BETA(4) | |
39 | DIMENSION BRATIO(6) | |
40 | DIMENSION MODE(6) | |
41 | DIMENSION NTYPE(3) | |
42 | DIMENSION PCM(4,3) | |
43 | DIMENSION XM(3) | |
44 | DIMENSION RNDM(1) | |
45 | LOGICAL ROTATE | |
46 | C. | |
47 | C. ------------------------------------------------------------------ | |
48 | C. | |
49 | C Search for parent particle in decay list. | |
50 | C | |
51 | C | |
52 | KCASE = NAMEC(5) | |
53 | NGKINE = 0 | |
54 | IF(IDCAY.EQ.2) THEN | |
55 | DESTEP = DESTEP+GETOT | |
56 | ISTOP = 2 | |
57 | GO TO 99 | |
58 | ENDIF | |
59 | DMASS = AMASS | |
60 | JPA = LQ(JPART-IPART) | |
61 | JDK1 = LQ(JPA-1) | |
62 | JDK2 = LQ(JPA-2) | |
63 | IF (JDK1.LE.0) GO TO 90 | |
64 | IF (JDK2.LE.0) GO TO 90 | |
65 | DO 5 I=1,6 | |
66 | BRATIO(I)=Q(JDK1+I) | |
67 | MODE(I)=IQ(JDK2+I) | |
68 | 5 CONTINUE | |
69 | C | |
70 | C Generate branching ratio and select decay mode. | |
71 | C | |
72 | NBR = 1 | |
73 | BAREA(1) = 0. | |
74 | DO 10 I=2,7 | |
75 | BRADD = BRATIO(I-1) | |
76 | IF (BRADD.EQ.0.) GO TO 20 | |
77 | NBR = NBR+1 | |
78 | BAREA(I) = BAREA(I-1)+BRADD | |
79 | 10 CONTINUE | |
80 | C | |
81 | 20 CALL GRNDM(RNDM,1) | |
82 | BRAND = 100.*RNDM(1) | |
83 | IF (BRAND.GE.BAREA(NBR)) GO TO 99 | |
84 | ID = IABS((LOCATF(BAREA,NBR,BRAND))) | |
85 | C | |
86 | C Unpack decay mode. | |
87 | C | |
88 | MXX = MODE(ID) | |
89 | NTYPE(1) = MOD(MXX,100) | |
90 | NTYPE(2) = MOD(MXX/100,100) | |
91 | JP1 = LQ(JPART-NTYPE(1)) | |
92 | JP2 = LQ(JPART-NTYPE(2)) | |
93 | XM(1) = Q(JP1+7) | |
94 | XM(2) = Q(JP2+7) | |
95 | IF (MXX.LT.10000)THEN | |
96 | C | |
97 | C Two body decay. | |
98 | C | |
99 | NGKINE = 2 | |
100 | IF (TLIFE.LT.1.E-15) THEN | |
101 | XMTOT = XM(1)+XM(2) | |
102 | DO 30 I=1,1000 | |
103 | C-- Create Lorentz distributed energy with FWHM HBAR/TLIFE. | |
104 | C-- (via integral-transformation of Lorentz-distribution) | |
105 | C-- (M.Guckes) | |
106 | CALL GRNDM(RNDM,1) | |
107 | RMASS = DMASS | |
108 | 1 + 3.291086E-25/TLIFE * TAN(PI*(RNDM(1)-0.5)) | |
109 | IF (RMASS.GE.XMTOT) GO TO 40 | |
110 | 30 CONTINUE | |
111 | WRITE(CHMAIL,1000) IPART, NTYPE(1), NTYPE(2) | |
112 | CALL GMAIL(0,0) | |
113 | NGKINE=0 | |
114 | GO TO 99 | |
115 | 40 DMASS = RMASS | |
116 | END IF | |
117 | CALL GDECA2(DMASS,XM(1),XM(2),PCM) | |
118 | ELSE | |
119 | C | |
120 | C Three body decay. | |
121 | C | |
122 | NTYPE(3) = MXX/10000 | |
123 | NGKINE = 3 | |
124 | JP3 = LQ(JPART-NTYPE(3)) | |
125 | XM(3) = Q(JP3+7) | |
126 | IF (TLIFE.LT.1.E-15) THEN | |
127 | XMTOT = XM(1)+XM(2)+XM(3) | |
128 | DO 31 I=1,1000 | |
129 | C-- Create Lorentz distributed energy with FWHM HBAR/TLIFE. | |
130 | C-- (via integral-transformation of Lorentz-distribution) | |
131 | CALL GRNDM(RNDM,1) | |
132 | RMASS = DMASS | |
133 | 1 + 3.291086E-25/TLIFE * TAN(PI*(RNDM(1)-0.5)) | |
134 | IF (RMASS.GE.XMTOT) GO TO 41 | |
135 | 31 CONTINUE | |
136 | WRITE(CHMAIL,1000) IPART, NTYPE(1), NTYPE(2), NTYPE(3) | |
137 | CALL GMAIL(0,0) | |
138 | NGKINE=0 | |
139 | GO TO 99 | |
140 | 41 DMASS = RMASS | |
141 | END IF | |
142 | CALL GDECA3(DMASS,XM(1),XM(2),XM(3),PCM) | |
143 | ENDIF | |
144 | C | |
145 | C LORENTZ boost into LAB system defined along parent vector | |
146 | C followed by rotation back into GEANT system. | |
147 | C | |
148 | P0 = VECT(7) | |
149 | E0 = SQRT(P0*P0+DMASS*DMASS) | |
150 | BETA(1) = 0. | |
151 | BETA(2) = 0. | |
152 | BETA(3) = -P0/E0 | |
153 | BETA(4) = E0/DMASS | |
154 | CALL GFANG(VECT(4),COSTH,SINTH,COSPH,SINPH,ROTATE) | |
155 | C | |
156 | DO 60 K=1,NGKINE | |
157 | IF (P0.LE.0.) THEN | |
158 | DO 59 I = 1,3 | |
159 | 59 GKIN(I,K) = PCM(I,K) | |
160 | ELSE | |
161 | CALL GLOREN (BETA, PCM(1,K), GKIN(1,K)) | |
162 | ENDIF | |
163 | IF(ROTATE) CALL GDROT (GKIN(1,K),COSTH,SINTH,COSPH,SINPH) | |
164 | GKIN(4,K)=SQRT(GKIN(1,K)**2+GKIN(2,K)**2+GKIN(3,K)**2+XM(K)**2) | |
165 | GKIN(5,K)=NTYPE(K) | |
166 | TOFD(K)=0. | |
167 | GPOS(1,K) = VECT(1) | |
168 | GPOS(2,K) = VECT(2) | |
169 | GPOS(3,K) = VECT(3) | |
170 | 60 CONTINUE | |
171 | GO TO 99 | |
172 | C | |
173 | C No branching ratio defined. Call user routine | |
174 | C | |
175 | #if !defined(CERNLIB_USRJMP) | |
176 | 90 CALL GUDCAY | |
177 | #endif | |
178 | #if defined(CERNLIB_USRJMP) | |
179 | 90 CALL JUMPT0(JUDCAY) | |
180 | #endif | |
181 | C | |
182 | 99 RETURN | |
183 | 1000 FORMAT(' ***** GDECAY ERROR : Not enough energy available for ', | |
184 | + 'decay of resonance',I3,' to',3I3,'; no decay.') | |
185 | END |