[819] | 1 | // |
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| 2 | // ******************************************************************** |
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| 3 | // * License and Disclaimer * |
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| 4 | // * * |
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of * |
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and * |
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| 7 | // * conditions of the Geant4 Software License, included in the file * |
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These * |
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| 9 | // * include a list of copyright holders. * |
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| 10 | // * * |
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| 11 | // * Neither the authors of this software system, nor their employing * |
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| 12 | // * institutes,nor the agencies providing financial support for this * |
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| 13 | // * work make any representation or warranty, express or implied, * |
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| 14 | // * regarding this software system or assume any liability for its * |
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| 15 | // * use. Please see the license in the file LICENSE and URL above * |
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| 16 | // * for the full disclaimer and the limitation of liability. * |
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| 17 | // * * |
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| 18 | // * This code implementation is the result of the scientific and * |
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| 19 | // * technical work of the GEANT4 collaboration. * |
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| 20 | // * By using, copying, modifying or distributing the software (or * |
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| 21 | // * any work based on the software) you agree to acknowledge its * |
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| 22 | // * use in resulting scientific publications, and indicate your * |
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| 23 | // * acceptance of all terms of the Geant4 Software license. * |
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| 24 | // ******************************************************************** |
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| 25 | // |
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| 26 | // |
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| 27 | // This software was developed by Lawrence Livermore National Laboratory. |
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| 28 | // |
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| 29 | // Redistribution and use in source and binary forms, with or without |
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| 30 | // modification, are permitted provided that the following conditions are met: |
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| 31 | // |
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| 32 | // 1. Redistributions of source code must retain the above copyright notice, |
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| 33 | // this list of conditions and the following disclaimer. |
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| 34 | // 2. Redistributions in binary form must reproduce the above copyright notice, |
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| 35 | // this list of conditions and the following disclaimer in the documentation |
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| 36 | // and/or other materials provided with the distribution. |
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| 37 | // 3. The name of the author may not be used to endorse or promote products |
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| 38 | // derived from this software without specific prior written permission. |
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| 39 | // |
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| 40 | // THIS SOFTWARE IS PROVIDED BY THE AUTHOR ``AS IS'' AND ANY EXPRESS OR IMPLIED |
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| 41 | // WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF |
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| 42 | // MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO |
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| 43 | // EVENT SHALL THE AUTHOR BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, |
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| 44 | // SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, |
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| 45 | // PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS; |
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| 46 | // OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY, |
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| 47 | // WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR |
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| 48 | // OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF |
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| 49 | // ADVISED OF THE POSSIBILITY OF SUCH DAMAGE. |
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| 50 | // |
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| 51 | // Copyright (c) 2006 The Regents of the University of California. |
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| 52 | // All rights reserved. |
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| 53 | // UCRL-CODE-224807 |
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| 54 | // |
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| 55 | // $Id: G4fissionEvent.cc,v 1.2 2007/06/01 13:46:53 gcosmo Exp $ |
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| 56 | // |
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| 57 | |
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| 58 | #include "G4fissionEvent.hh" |
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| 59 | |
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| 60 | G4int G4fissionEvent::delayoption=0; |
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| 61 | G4int G4fissionEvent::correlationoption=0; |
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| 62 | G4int G4fissionEvent::nudistoption=3; |
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| 63 | G4int G4fissionEvent::Cf252ndistoption=0; |
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| 64 | G4int G4fissionEvent::Cf252nengoption=0; |
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| 65 | |
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| 66 | G4fissionEvent::G4fissionEvent(G4int isotope, G4double time, G4double nubar, G4double eng) { |
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| 67 | /* |
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| 68 | * Constructs a fission event with neutronNu neutrons and photonNu |
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| 69 | * photons. |
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| 70 | */ |
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| 71 | G4int i; |
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| 72 | |
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| 73 | neutronNu = 0; |
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| 74 | photonNu = 0; |
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| 75 | if (nubar == -1.) { |
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| 76 | /* spontaneous fission */ |
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| 77 | neutronNu = G4SmpSpNuDistData(isotope, Cf252ndistoption); |
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| 78 | photonNu = G4SmpSpNugDistData(isotope); |
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| 79 | } else { |
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| 80 | /* induced fission */ |
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| 81 | if (nudistoption == 0 || nudistoption == 1) { |
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| 82 | switch (isotope) { |
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| 83 | case 92235: |
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| 84 | neutronNu = G4SmpNuDistDataU235(eng,nudistoption); |
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| 85 | break; |
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| 86 | case 92238: |
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| 87 | neutronNu = G4SmpNuDistDataU238(eng); |
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| 88 | break; |
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| 89 | case 94239: |
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| 90 | neutronNu = G4SmpNuDistDataPu239(eng); |
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| 91 | break; |
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| 92 | default: |
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| 93 | neutronNu = (G4int) G4SmpTerrell(nubar); |
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| 94 | break; |
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| 95 | } |
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| 96 | } else if (nudistoption == 2) { |
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| 97 | switch (isotope) { |
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| 98 | case 92232: |
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| 99 | case 92234: |
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| 100 | case 92236: |
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| 101 | case 92238: |
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| 102 | neutronNu = G4SmpNuDistDataU232_234_236_238(nubar); |
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| 103 | break; |
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| 104 | case 92233: |
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| 105 | case 92235: |
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| 106 | neutronNu = (G4int) G4SmpNuDistDataU233_235(nubar); |
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| 107 | break; |
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| 108 | case 94239: |
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| 109 | case 94241: |
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| 110 | neutronNu = G4SmpNuDistDataPu239_241(nubar); |
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| 111 | break; |
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| 112 | default: |
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| 113 | neutronNu = (G4int) G4SmpTerrell(nubar); |
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| 114 | break; |
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| 115 | } |
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| 116 | } else if (nudistoption == 3) { |
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| 117 | switch (isotope) { |
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| 118 | case 92232: |
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| 119 | case 92234: |
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| 120 | case 92236: |
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| 121 | case 92238: |
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| 122 | neutronNu = G4SmpNuDistDataU232_234_236_238_MC(nubar); |
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| 123 | break; |
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| 124 | case 92233: |
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| 125 | case 92235: |
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| 126 | neutronNu = (G4int) G4SmpNuDistDataU233_235_MC(nubar); |
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| 127 | break; |
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| 128 | case 94239: |
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| 129 | case 94241: |
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| 130 | neutronNu = G4SmpNuDistDataPu239_241_MC(nubar); |
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| 131 | break; |
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| 132 | default: |
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| 133 | neutronNu = (G4int) G4SmpTerrell(nubar); |
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| 134 | break; |
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| 135 | } |
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| 136 | } |
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| 137 | photonNu = G4SmpNugDist(isotope, nubar); |
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| 138 | } |
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| 139 | if (neutronNu > 0) { |
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| 140 | neutronEnergies = new G4double[ neutronNu ]; |
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| 141 | neutronVelocities = new G4double[ neutronNu ]; |
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| 142 | neutronDircosu = new G4double[ neutronNu ]; |
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| 143 | neutronDircosv = new G4double[ neutronNu ]; |
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| 144 | neutronDircosw = new G4double[ neutronNu ]; |
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| 145 | neutronAges = new G4double[neutronNu]; |
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| 146 | for (i=0; i<neutronNu; i++) { |
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| 147 | if (isotope == 98252) neutronEnergies[i] = G4SmpNEngCf252(Cf252nengoption); |
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| 148 | else neutronEnergies[i] = G4SmpWatt(eng, isotope); |
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| 149 | neutronVelocities[i] = G4SmpNVel( |
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| 150 | neutronEnergies[i], |
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| 151 | &(neutronDircosu[i]), |
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| 152 | &(neutronDircosv[i]), |
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| 153 | &(neutronDircosw[i]) |
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| 154 | ); |
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| 155 | neutronAges[i] = time; |
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| 156 | } |
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| 157 | } |
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| 158 | if (photonNu > 0) { |
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| 159 | photonEnergies = new G4double[photonNu]; |
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| 160 | photonVelocities = new G4double[photonNu]; |
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| 161 | photonDircosu = new G4double[photonNu]; |
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| 162 | photonDircosv = new G4double[photonNu]; |
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| 163 | photonDircosw = new G4double[photonNu]; |
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| 164 | photonAges = new G4double[photonNu]; |
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| 165 | for (i=0; i<photonNu; i++) { |
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| 166 | photonEnergies[i] = G4SmpGEng(); |
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| 167 | photonVelocities[i] = G4SmpPVel( |
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| 168 | photonEnergies[i], |
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| 169 | &(photonDircosu[i]), |
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| 170 | &(photonDircosv[i]), |
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| 171 | &(photonDircosw[i]) |
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| 172 | ); |
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| 173 | photonAges[i] = time; |
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| 174 | } |
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| 175 | } |
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| 176 | } |
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| 177 | |
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| 178 | G4fissionEvent::~G4fissionEvent() { |
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| 179 | if (neutronNu > 0) { |
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| 180 | delete [] neutronEnergies; |
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| 181 | delete [] neutronVelocities; |
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| 182 | delete [] neutronDircosu; |
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| 183 | delete [] neutronDircosv; |
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| 184 | delete [] neutronDircosw; |
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| 185 | delete [] neutronAges; |
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| 186 | } |
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| 187 | |
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| 188 | if (photonNu > 0) { |
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| 189 | delete [] photonEnergies; |
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| 190 | delete [] photonVelocities; |
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| 191 | delete [] photonDircosu; |
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| 192 | delete [] photonDircosv; |
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| 193 | delete [] photonDircosw; |
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| 194 | delete [] photonAges; |
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| 195 | } |
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| 196 | } |
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