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Geant4/processes/hadronic/models/fission/src/G4SmpSpNuDistData.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 "G4fissionEvent.hh"
 59 
 60 #define nSPfissIso 8
 61 #define nSPfissn 11
 62 
 63 G4int G4fissionEvent::G4SmpSpNuDistData(G4int isotope, G4int Cf252option) {
 64 
 65 /*
 66   Description
 67     Sample Number of Neutrons from spontaneous fission 
 68     (a) from the neutron multiplicity data for 
 69         U-238, Pu-238, Pu-240, Pu-242, Cm-242, Cm-244
 70            using Holden and Zucker's tabulated data
 71         Cf-252 using either Spencer's tabulated data or 
 72            Boldeman's data
 73     (b) from Terrell's approximation using nubar for
 74         Th-232, 
 75         U-232, U-233, U-234, U-235, U-236,
 76         Np-237, 
 77         Pu-239, Pu-241, 
 78         Am-241, 
 79         Bk-249
 80            using Ensslin's data.
 81 */
 82 
 83 /*
 84   Input
 85     iso          - isotope
 86     Cf252option  - 0 to use Spencer's tabulated data
 87                    1 to use Boldeman's data
 88   Output
 89     G4SmpSpNuDistData - sampled multiplicity
 90                       -1 is the isotope has 
 91                          no multiplicity data,
 92                          nor any nubar data
 93 */
 94  
 95   G4int i, index;
 96   G4double sum, nubar;
 97   G4double r;
 98 
 99   static G4double sfnu [nSPfissIso][nSPfissn] = { 
100     {0.0481677,0.2485215,0.4253044,0.2284094,0.0423438,0.0072533,
101      0.0000000,0.0000000,0.0000000,0.0000000,0.0000000},
102 
103     {0.0631852,0.2319644,0.3333230,0.2528207,0.0986461,0.0180199,
104      0.0020407,0.0000000,0.0000000,0.0000000,0.0000000},
105 
106     {0.0679423,0.2293159,0.3341228,0.2475507,0.0996922,0.0182398,
107      0.0031364,0.0000000,0.0000000,0.0000000,0.0000000},
108 
109     {0.0212550,0.1467407,0.3267531,0.3268277,0.1375090,0.0373815,
110      0.0025912,0.0007551,0.0001867,0.0000000,0.0000000},
111 
112     {0.0150050,0.1161725,0.2998427,0.3331614,0.1837748,0.0429780,
113      0.0087914,0.0002744,0.0000000,0.0000000,0.0000000},
114 
115     {0.0540647,0.2053880,0.3802279,0.2248483,0.1078646,0.0276366,
116      0.0000000,0.0000000,0.0000000,0.0000000,0.0000000},
117 
118     {0.0021100,0.0246700,0.1229000,0.2714400,0.3076300,0.1877000,
119      0.0677000,0.0140600,0.0016700,0.0001000,0.0000000},
120 
121     {0.0020900,0.0262100,0.1262000,0.2752000,0.3018000,0.1846000,
122      0.0668000,0.0150000,0.0021000,0.0000000,0.0000000} };
123 
124 /*
125   sample the spontaneous fission neutron number distribution
126 */
127   index = -1;
128 
129   if (isotope == 92238) index = 0;
130   else if (isotope == 94240) index = 1;
131   else if (isotope == 94242) index = 2;
132   else if (isotope == 96242) index = 3;
133   else if (isotope == 96244) index = 4;
134   else if (isotope == 94238) index = 5;
135   else if (isotope == 98252 && Cf252option == 0) index = 6;
136   else if (isotope == 98252 && Cf252option == 1) index = 7;
137 
138   if (index != -1) { 
139     r=fisslibrng();
140 
141     sum = 0.;
142     for (i = 0; i < nSPfissn-1; i++) {
143       sum = sum + sfnu[index][i];
144       if (r <= sum || sfnu[index][i+1] == 0.) return i;
145     }
146     //
147     // Fall through
148     //
149     G4cout << " Random number out of range in SmpSpNuDistData " << G4endl;
150     return -1;
151 
152   } else {
153 // There is no full multiplicity distribution data available
154 // for that isotope, let's try to find a nubar for it in
155 // N. Ensslin, et.al., "Application Guide to Neutron
156 // Multiplicity Counting," LA-13422-M (November 1998)
157 // and use Terrell's approximation
158     nubar = G4SmpSpNubarData(isotope);
159     if (nubar != -1.) {
160       return (G4int) G4SmpTerrell(nubar);
161     } else {
162 // There is no nubar information for that isotope, return -1,
163 // meaning no data available for that isotope
164       return -1;
165     }
166   }
167 }
168