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G4SmpSpNuDistData.cc
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53 // UCRL-CODE-224807
54 //
55 //
56 //
57 
58 #include "G4fissionEvent.hh"
59 
60 #define nSPfissIso 8
61 #define nSPfissn 11
62 
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 }