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Geant4/processes/hadronic/models/fission/src/G4SmpNuDistDataU233_235_MC.cc

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Differences between /processes/hadronic/models/fission/src/G4SmpNuDistDataU233_235_MC.cc (Version 11.3.0) and /processes/hadronic/models/fission/src/G4SmpNuDistDataU233_235_MC.cc (Version 10.0.p3)


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 51 // Copyright (c) 2006 The Regents of the Unive     51 // Copyright (c) 2006 The Regents of the University of California.
 52 // All rights reserved.                            52 // All rights reserved.
 53 // UCRL-CODE-224807                                53 // UCRL-CODE-224807
 54 //                                                 54 //
 55 //                                                 55 //
                                                   >>  56 // $Id: G4SmpNuDistDataU233_235_MC.cc 68799 2013-04-05 13:29:46Z gcosmo $
 56 //                                                 57 //
 57                                                    58 
 58 #include <cmath>                                   59 #include <cmath>
 59 #include "G4fissionEvent.hh"                       60 #include "G4fissionEvent.hh"
 60                                                    61 
 61 G4int G4fissionEvent::G4SmpNuDistDataU233_235_     62 G4int G4fissionEvent::G4SmpNuDistDataU233_235_MC(G4double nubar) {
 62                                                    63 
 63 /*                                                 64 /*
 64   Description                                      65   Description
 65     Sample Number of Neutrons from fission in      66     Sample Number of Neutrons from fission in U-233 and U-235 using 
 66     Zucker and Holden's tabulated data for U-2     67     Zucker and Holden's tabulated data for U-235
 67     The 11 P(nu) distributions are given as a      68     The 11 P(nu) distributions are given as a function of nubar, 
 68     the average number of neutrons from induce     69     the average number of neutrons from induced fission for the 
 69     11 different energies (0 to 10 MeV), based     70     11 different energies (0 to 10 MeV), based on the U-235 data 
 70     from Zucker and Holden.                        71     from Zucker and Holden.
 71 */                                                 72 */
 72                                                    73 
 73 /*                                                 74 /*
 74   Input                                            75   Input
 75     nubar    - average number of neutrons per      76     nubar    - average number of neutrons per fission
 76   Output                                           77   Output
 77     G4SmpNuDistDataU233_235_MC  - sampled mult     78     G4SmpNuDistDataU233_235_MC  - sampled multiplicity
 78                                                    79     
 79 */                                                 80 */
 80                                                    81 
 81   static G4double U235nu [11] [8] = {              82   static G4double U235nu [11] [8] = {
 82      {.0317223, .1717071, .3361991, .3039695,      83      {.0317223, .1717071, .3361991, .3039695, .1269459, .0266793, .0026322, .0001449},
 83      {.0237898, .1555525, .3216515, .3150433,      84      {.0237898, .1555525, .3216515, .3150433, .1444732, .0356013, .0034339, .0004546},
 84      {.0183989, .1384891, .3062123, .3217566,      85      {.0183989, .1384891, .3062123, .3217566, .1628673, .0455972, .0055694, .0011093},
 85      {.0141460, .1194839, .2883075, .3266568,      86      {.0141460, .1194839, .2883075, .3266568, .1836014, .0569113, .0089426, .0019504},
 86      {.0115208, .1032624, .2716849, .3283426,      87      {.0115208, .1032624, .2716849, .3283426, .2021206, .0674456, .0128924, .0027307},
 87      {.0078498, .0802010, .2456595, .3308175,      88      {.0078498, .0802010, .2456595, .3308175, .2291646, .0836912, .0187016, .0039148},
 88      {.0046272, .0563321, .2132296, .3290407,      89      {.0046272, .0563321, .2132296, .3290407, .2599806, .1045974, .0265604, .0056322},
 89      {.0024659, .0360957, .1788634, .3210507,      90      {.0024659, .0360957, .1788634, .3210507, .2892537, .1282576, .0360887, .0079244},
 90      {.0012702, .0216090, .1472227, .3083032,      91      {.0012702, .0216090, .1472227, .3083032, .3123950, .1522540, .0462449, .0107009},
 91      {.0007288, .0134879, .1231200, .2949390,      92      {.0007288, .0134879, .1231200, .2949390, .3258251, .1731879, .0551737, .0135376},
 92      {.0004373, .0080115, .1002329, .2779283,      93      {.0004373, .0080115, .1002329, .2779283, .3342611, .1966100, .0650090, .0175099}
 93     };                                             94     };
 94   static G4double U235nubar [11] = {               95   static G4double U235nubar [11] = {
 95       2.4140000,                                   96       2.4140000, 
 96       2.5236700,                                   97       2.5236700, 
 97       2.6368200,                                   98       2.6368200, 
 98       2.7623400,                                   99       2.7623400, 
 99       2.8738400,                                  100       2.8738400, 
100       3.0386999,                                  101       3.0386999, 
101       3.2316099,                                  102       3.2316099, 
102       3.4272800,                                  103       3.4272800, 
103       3.6041900,                                  104       3.6041900, 
104       3.7395900,                                  105       3.7395900, 
105       3.8749800                                   106       3.8749800
106     };                                            107     };
107   G4double fraction, r, cum;                      108   G4double fraction, r, cum;
108   G4int engind, nu;                               109   G4int engind, nu;
109                                                   110 
110 /*                                                111 /* 
111   Check if nubar is within the range of experi    112   Check if nubar is within the range of experimental values
112 */                                                113 */
113   if(nubar >= U235nubar[0] && nubar <= U235nub    114   if(nubar >= U235nubar[0] && nubar <= U235nubar[10]) {
114 /*                                                115 /*
115      Use Zucker and Holden Data                   116      Use Zucker and Holden Data
116 */                                                117 */
117      engind = 1;                                  118      engind = 1;
118      while (nubar > U235nubar[engind]){ engind    119      while (nubar > U235nubar[engind]){ engind++;}
119      // Loop checking, 11.03.2015, T. Koi      << 
120      fraction = (nubar-U235nubar[engind-1])/(U    120      fraction = (nubar-U235nubar[engind-1])/(U235nubar[engind]-U235nubar[engind-1]);
121      if(fisslibrng() > fraction) engind--;        121      if(fisslibrng() > fraction) engind--;
122                                                   122 
123      r = fisslibrng();                            123      r = fisslibrng();
124      nu = 0;                                      124      nu = 0;
125      cum = U235nu[engind][0];                     125      cum = U235nu[engind][0];
126      while (r > cum && nu < 7){                   126      while (r > cum && nu < 7){ 
127      // Loop checking, 11.03.2015, T. Koi      << 
128        nu++;                                      127        nu++;
129        cum += U235nu[engind][nu];                 128        cum += U235nu[engind][nu];
130      }                                            129      }
131      return nu;                                   130      return nu;
132   } else {                                        131   } else {
133 /*                                                132 /*
134      Use Terrell's formula                        133      Use Terrell's formula
135 */                                                134 */
136      return (G4int) G4SmpTerrell(nubar);          135      return (G4int) G4SmpTerrell(nubar);
137   }                                               136   }
138 }                                                 137 }
139                                                   138