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Geant4/processes/hadronic/models/fission/src/G4SmpNuDistDataPu239_241_MC.cc

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 51 // Copyright (c) 2006 The Regents of the University of California.
 52 // All rights reserved.
 53 // UCRL-CODE-224807
 54 //
 55 //
 56 //
 57 
 58 #include <cmath>
 59 #include "G4fissionEvent.hh"
 60 
 61 G4int G4fissionEvent::G4SmpNuDistDataPu239_241_MC(G4double nubar) {
 62 
 63 /*
 64   Description
 65     Sample Number of Neutrons from fission in Pu-239 and Pu-241 using 
 66     Zucker and Holden's tabulated data for Pu-239
 67     The 11 P(nu) distributions are given as a function of nubar, 
 68     the average number of neutrons from induced fission for the 
 69     11 different energies (0 to 10 MeV), based on the Pu-239 data 
 70     from Zucker and Holden.
 71 */
 72 
 73 /*
 74   Input
 75     nubar    - average number of neutrons per fission
 76   Output
 77     G4SmpNuDistDataPu239_241_MC  - sampled multiplicity
 78     
 79 */
 80 
 81   static G4double Pu239nu [11] [9] = {
 82      {.0108826, .0994916, .2748898, .3269196, .2046061, .0726834, .0097282, .0006301, .0001685},
 83      {.0084842, .0790030, .2536175, .3289870, .2328111, .0800161, .0155581, .0011760, .0003469},
 84      {.0062555, .0611921, .2265608, .3260637, .2588354, .0956070, .0224705, .0025946, .0005205},
 85      {.0045860, .0477879, .1983002, .3184667, .2792811, .1158950, .0301128, .0048471, .0007233},
 86      {.0032908, .0374390, .1704196, .3071862, .2948565, .1392594, .0386738, .0078701, .0010046},
 87      {.0022750, .0291416, .1437645, .2928006, .3063902, .1641647, .0484343, .0116151, .0014149},
 88      {.0014893, .0222369, .1190439, .2756297, .3144908, .1892897, .0597353, .0160828, .0029917},
 89      {.0009061, .0163528, .0968110, .2558524, .3194566, .2134888, .0729739, .0213339, .0020017},
 90      {.0004647, .0113283, .0775201, .2335926, .3213289, .2356614, .0886183, .0274895, .0039531},
 91      {.0002800, .0071460, .0615577, .2089810, .3200121, .2545846, .1072344, .0347255, .0054786},
 92      {.0002064, .0038856, .0492548, .1822078, .3154159, .2687282, .1295143, .0432654, .0075217}
 93     };
 94   static G4double Pu239nubar [11] = {
 95       2.8760000,
 96       3.0088800,
 97       3.1628300,
 98       3.3167800,
 99       3.4707300,
100       3.6246800,
101       3.7786300,
102       3.9325800,
103       4.0865300,
104       4.2404900,
105       4.3944400
106     };
107   G4double fraction, r, cum;
108   G4int engind, nu;
109 
110 /* 
111   Check if nubar is within the range of experimental values
112 */
113   if(nubar >= Pu239nubar[0] && nubar <= Pu239nubar[10]) {
114 /*
115      Use Zucker and Holden Data
116 */
117      engind = 1;
118      while (nubar > Pu239nubar[engind]){ engind++;}
119      // Loop checking, 11.03.2015, T. Koi
120      fraction = (nubar-Pu239nubar[engind-1])/(Pu239nubar[engind]-Pu239nubar[engind-1]);
121      if(fisslibrng() > fraction) engind--;
122 
123      r = fisslibrng();
124      nu = 0;
125      cum = Pu239nu[engind][0];
126      while (r > cum && nu < 8){ 
127      // Loop checking, 11.03.2015, T. Koi
128        nu++;
129        cum += Pu239nu[engind][nu];
130      }
131      return nu;
132   } else {
133 /*
134      Use Terrell's formula
135 */
136      return (G4int) G4SmpTerrell(nubar);
137   }
138 }
139