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Please see the license in the file LICENSE and URL above * 16 // * for the full disclaimer and the limitatio 16 // * for the full disclaimer and the limitation of liability. * 17 // * 17 // * * 18 // * This code implementation is the result 18 // * This code implementation is the result of the scientific and * 19 // * technical work of the GEANT4 collaboratio 19 // * technical work of the GEANT4 collaboration. * 20 // * By using, copying, modifying or distri 20 // * By using, copying, modifying or distributing the software (or * 21 // * any work based on the software) you ag 21 // * any work based on the software) you agree to acknowledge its * 22 // * use in resulting scientific publicati 22 // * use in resulting scientific publications, and indicate your * 23 // * acceptance of all terms of the Geant4 Sof 23 // * acceptance of all terms of the Geant4 Software license. * 24 // ******************************************* 24 // ******************************************************************** 25 // 25 // 26 /* 26 /* 27 * File: G4FPYNubarValues.hh 27 * File: G4FPYNubarValues.hh 28 * Author: B. Wendt (wendbryc@isu.edu) 28 * Author: B. Wendt (wendbryc@isu.edu) 29 * 29 * 30 * Created on July 11, 2011, 11:23 AM 30 * Created on July 11, 2011, 11:23 AM 31 */ 31 */ 32 32 33 /* * * * * * * * * * * * * * * * References 33 /* * * * * * * * * * * * * * * * References * * * * * * * * * * * * * * * * 34 * 34 * * 35 * 1. "Neutron Multiplicity Measurements of 35 * 1. "Neutron Multiplicity Measurements of Cf and Fm Isotopes", * 36 * D. C. Hoffman, G. P. Ford, J. P. Balag 36 * D. C. Hoffman, G. P. Ford, J. P. Balagna, and L. R. Veeser, Physical * 37 * Review C, 21.2, February 1980 37 * Review C, 21.2, February 1980 * 38 * 2. "Spontaneous Fission Properties and Li 38 * 2. "Spontaneous Fission Properties and Lifetime Systematics", * 39 * D. C. Hoffman, International Conferenc 39 * D. C. Hoffman, International Conference on Fifty Years Research in * 40 * Nuclear Fission, Berlin, Germany, 1989 40 * Nuclear Fission, Berlin, Germany, 1989 * 41 * 3. MCNP - A General Monte carlo N-Particl 41 * 3. MCNP - A General Monte carlo N-Particle Transport Code, Version 5, * 42 * X-5 Monte Carlo Team, Volume I: Overvi 42 * X-5 Monte Carlo Team, Volume I: Overview and Theory, April, 2005 * 43 * 4. ENDF database, Search parameters: ENDF 43 * 4. ENDF database, Search parameters: ENDF/B-VII.0; MF=1; MAT=452 * 44 * 5. Prompt Neutron Multiplicities for the 44 * 5. Prompt Neutron Multiplicities for the Transplutonium Nuclides, * 45 * N. E. Holden and M. S. Zucker, Brookha 45 * N. E. Holden and M. S. Zucker, Brookhaven National Lab, January, 1985 * 46 * 46 * * 47 * * * * * * * * * * * * * * * * References 47 * * * * * * * * * * * * * * * * References * * * * * * * * * * * * * * * */ 48 48 49 #ifndef G4FPYNUBARVALUES_HH 49 #ifndef G4FPYNUBARVALUES_HH 50 #define G4FPYNUBARVALUES_HH << 50 #define G4FPYNUBARVALUES_HH 51 << 52 #include "G4Types.hh" << 53 51 54 /** Evaluated nubar values for neutron induced 52 /** Evaluated nubar values for neutron induced fission. The data are represented 55 * as linear regression fits from experimenta 53 * as linear regression fits from experimental data in the form: v = mx + b, 56 * where x is the incident neutron energy. 54 * where x is the incident neutron energy. 57 * \n \n Value 1: The isotope in ZZZAAA forma 55 * \n \n Value 1: The isotope in ZZZAAA format 58 * \n Value 2: 'x' of the linear regression f 56 * \n Value 2: 'x' of the linear regression fit multiplied by 10^13 59 * \n Value 3: 'b' of the linear regression f 57 * \n Value 3: 'b' of the linear regression fit multiplied by 10^4 60 * \n \n See Reference 4 for further informat 58 * \n \n See Reference 4 for further information 61 */ 59 */ 62 static const G4int NeutronInducedNubar_[][3] = 60 static const G4int NeutronInducedNubar_[][3] = { 63 // Default << 61 // Default 64 {0, 1476773, 29881}, << 62 {0, 1476773, 29881}, 65 // Thorium << 63 // Thorium 66 {90227, 818327, 20647}, << 64 {90227, 818327, 20647}, {90229, 936480, 20872}, {90232, 1252285, 21061}, 67 {90229, 936480, 20872}, << 65 // Proactinum 68 {90232, 1252285, 21061}, << 66 {91231, 1030251, 22480}, 69 // Proactinum << 67 // Uranium 70 {91231, 1030251, 22480}, << 68 {92232, 1070000, 31300}, {92233, 1218868, 25043}, 71 // Uranium << 69 {92234, 1230006, 23673}, {92235, 1392331, 24336}, 72 {92232, 1070000, 31300}, << 70 {92236, 1353849, 23717}, {92237, 1502160, 24911}, 73 {92233, 1218868, 25043}, << 71 {92238, 1343405, 24911}, 74 {92234, 1230006, 23673}, << 72 // Neptunium 75 {92235, 1392331, 24336}, << 73 {93237, 1485790, 26362}, {93238, 1476892, 25150}, 76 {92236, 1353849, 23717}, << 74 // Plutonium 77 {92237, 1502160, 24911}, << 75 {94238, 1479368, 28950}, {94239, 1477500, 28505}, 78 {92238, 1343405, 24911}, << 76 {94240, 1518313, 28030}, {94241, 1496809, 29443}, 79 // Neptunium << 77 {94242, 1575406, 28100}, 80 {93237, 1485790, 26362}, << 78 // Americium 81 {93238, 1476892, 25150}, << 79 {95241, 1425195, 30827}, {95242, 1337871, 32717}, 82 // Plutonium << 80 {95243, 1305739, 32737}, 83 {94238, 1479368, 28950}, << 81 // Curium 84 {94239, 1477500, 28505}, << 82 {96242, 1720000, 34400}, {96243, 1220064, 34329}, 85 {94240, 1518313, 28030}, << 83 {96244, 1839123, 32444}, {96245, 1166218, 35968}, 86 {94241, 1496809, 29443}, << 84 {96246, 1223446, 36153}, {96248, 2080000, 34900}, 87 {94242, 1575406, 28100}, << 85 // Californium 88 // Americium << 86 {98249, 1796326, 38876}, {98251, 2416144, 41400}, 89 {95241, 1425195, 30827}, << 87 // Einsteinium 90 {95242, 1337871, 32717}, << 88 {99254, 2438676, 40832}, 91 {95243, 1305739, 32737}, << 89 // Fermium 92 // Curium << 90 {100255, 2499442, 43924}, 93 {96242, 1720000, 34400}, << 91 // End of array 94 {96243, 1220064, 34329}, << 92 {-1, -1, -1} }; 95 {96244, 1839123, 32444}, << 96 {96245, 1166218, 35968}, << 97 {96246, 1223446, 36153}, << 98 {96248, 2080000, 34900}, << 99 // Californium << 100 {98249, 1796326, 38876}, << 101 {98251, 2416144, 41400}, << 102 // Einsteinium << 103 {99254, 2438676, 40832}, << 104 // Fermium << 105 {100255, 2499442, 43924}, << 106 // End of array << 107 {-1, -1, -1}}; << 108 93 109 /** Recommended Gaussian widths for neutron in 94 /** Recommended Gaussian widths for neutron induced fission. 110 * \n Column 1: The isotope in ZZZAAA format 95 * \n Column 1: The isotope in ZZZAAA format 111 * \n Column 2: The width multiplied by 10^6 96 * \n Column 2: The width multiplied by 10^6 112 * \n \n See Reference 3 for further informat 97 * \n \n See Reference 3 for further information 113 */ 98 */ 114 // Still need: a lot 99 // Still need: a lot 115 static const G4int NeutronInducedNubarWidth_[] 100 static const G4int NeutronInducedNubarWidth_[][2] = { 116 // Default << 101 // Default 117 {0, 1210000}, << 102 {0, 1210000}, 118 // Uranium << 103 // Uranium 119 {92233, 1144900}, << 104 {92233, 1144900}, {92235, 1183744}, {92238, 1245456}, 120 {92235, 1183744}, << 105 // Plutonium 121 {92238, 1245456}, << 106 {94239, 1299600}, {94241, 1322500}, 122 // Plutonium << 107 // End of array 123 {94239, 1299600}, << 108 {-1, -1} }; 124 {94241, 1322500}, << 125 // End of array << 126 {-1, -1}}; << 127 109 128 /** Evaluated nubar values for neutron induced 110 /** Evaluated nubar values for neutron induced fission. The data are represented 129 * as linear regression fits from experimenta 111 * as linear regression fits from experimental data in the form: v = mx + b, 130 * where x is the incident neutron energy. 112 * where x is the incident neutron energy. 131 * \n \n Value 1: The isotope in ZZZAAA forma 113 * \n \n Value 1: The isotope in ZZZAAA format 132 * \n Value 2: 'x' of the linear regression f 114 * \n Value 2: 'x' of the linear regression fit multiplied by 10^13 133 * \n Value 3: 'b' of the linear regression f 115 * \n Value 3: 'b' of the linear regression fit multiplied by 10^4 134 * \n \n See References 1, 2, 4, & 5 for furt 116 * \n \n See References 1, 2, 4, & 5 for further information 135 */ 117 */ 136 static const G4int SpontaneousNubar_[][3] = { 118 static const G4int SpontaneousNubar_[][3] = { 137 // Default << 119 // Default 138 {0, 25000}, << 120 {0, 25000}, 139 // Uranium << 121 // Uranium 140 {92238, 0, 20000}, << 122 {92238, 0, 20000}, 141 // Curium << 123 // Curium 142 {96244, 0, 26875}, << 124 {96244, 0, 26875}, {96246, 0, 29480}, {96248, 0, 31500}, 143 {96246, 0, 29480}, << 125 // Californium 144 {96248, 0, 31500}, << 126 {98250, 0, 25200}, {98252, 0, 37676}, 145 // Californium << 127 // Einsteinium 146 {98250, 0, 25200}, << 128 {99253, 0, 47000}, 147 {98252, 0, 37676}, << 129 // Fermium 148 // Einsteinium << 130 {100254, 0, 39800}, {100256, 0, 37300}, 149 {99253, 0, 47000}, << 131 // End of array 150 // Fermium << 132 {-1, -1, -1} }; 151 {100254, 0, 39800}, << 152 {100256, 0, 37300}, << 153 // End of array << 154 {-1, -1, -1}}; << 155 133 156 /** Recommended Gaussian widths for neutron in 134 /** Recommended Gaussian widths for neutron induced fission. 157 * See Reference 3 for further information. 135 * See Reference 3 for further information. 158 * \n Column 1: The isotope in ZZZAAA format 136 * \n Column 1: The isotope in ZZZAAA format 159 * \n Column 2: The width multiplied by 10^6 137 * \n Column 2: The width multiplied by 10^6 160 */ 138 */ 161 // Still need: 92238, 99253 139 // Still need: 92238, 99253 162 static const G4int SpontaneousNubarWidth_[][2] 140 static const G4int SpontaneousNubarWidth_[][2] = { 163 // Default << 141 // Default 164 {0, 1210000}, << 142 {0, 1210000}, 165 // Plutonium << 143 // Plutonium 166 {94238, 1288225}, << 144 {94238, 1288225}, {94240, 1324801}, {94242, 1347921}, 167 {94240, 1324801}, << 145 // Curium 168 {94242, 1347921}, << 146 {96242, 1190281}, {96244, 1216609}, {96246, 1205604}, {96248, 1227664}, 169 // Curium << 147 // Californium 170 {96242, 1190281}, << 148 {98250, 1488400}, {98252, 1550025}, {98254, 1476225}, 171 {96244, 1216609}, << 149 // Fermium 172 {96246, 1205604}, << 150 {100254, 1552516}, {100256, 1349007}, {100257, 1178983}, 173 {96248, 1227664}, << 151 // End of array 174 // Californium << 152 {-1, -1} }; 175 {98250, 1488400}, << 153 176 {98252, 1550025}, << 154 #endif /* G4FPYNUBARVALUES_HH */ 177 {98254, 1476225}, << 178 // Fermium << 179 {100254, 1552516}, << 180 {100256, 1349007}, << 181 {100257, 1178983}, << 182 // End of array << 183 {-1, -1}}; << 184 155 185 #endif /* G4FPYNUBARVALUES_HH */ << 186 156