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 | // ------------------------------------------------------------------- |
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28 | // GEANT 4 class file |
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29 | // |
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30 | // CERN, Geneva, Switzerland |
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31 | // |
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32 | // File name: G4ContinuumGammaTransition |
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33 | // |
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34 | // Authors: Carlo Dallapiccola (dallapiccola@umdhep.umd.edu) |
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35 | // Maria Grazia Pia (pia@genova.infn.it) |
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36 | // |
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37 | // Creation date: 23 October 1998 |
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38 | // |
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39 | // Modifications: |
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40 | // |
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41 | // 15 April 1999, Alessandro Brunengo (Alessandro.Brunengo@ge.infn.it) |
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42 | // Added creation time evaluation for products of evaporation |
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43 | // 02 May 2003, Vladimir Ivanchenko change interface to G4NuclearlevelManager |
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44 | // |
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45 | // ------------------------------------------------------------------- |
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46 | // |
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47 | // Class G4ContinuumGammaTransition.cc |
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48 | // |
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49 | |
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50 | #include "G4ContinuumGammaTransition.hh" |
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51 | #include "G4VLevelDensityParameter.hh" |
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52 | #include "G4ConstantLevelDensityParameter.hh" |
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53 | #include "G4RandGeneralTmp.hh" |
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54 | // |
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55 | // Constructor |
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56 | // |
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57 | |
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58 | G4ContinuumGammaTransition::G4ContinuumGammaTransition( |
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59 | const G4NuclearLevelManager* levelManager, |
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60 | G4int Z, G4int A, |
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61 | G4double excitation, |
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62 | G4int verbose): |
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63 | _nucleusA(A), _nucleusZ(Z), _excitation(excitation), _levelManager(levelManager) |
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64 | { |
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65 | const G4PtrLevelVector* levels = _levelManager->GetLevels(); |
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66 | G4double eTolerance = 0.; |
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67 | if (levels != 0) |
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68 | { |
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69 | G4int lastButOne = _levelManager->NumberOfLevels() - 2; |
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70 | if (lastButOne >= 0) |
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71 | { |
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72 | eTolerance = _levelManager->MaxLevelEnergy() - levels->operator[](lastButOne)->Energy(); |
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73 | if (eTolerance < 0.) eTolerance = 0.; |
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74 | } |
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75 | } |
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76 | |
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77 | _verbose = verbose; |
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78 | _eGamma = 0.; |
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79 | _gammaCreationTime = 0.; |
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80 | |
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81 | _maxLevelE = _levelManager->MaxLevelEnergy() + eTolerance; |
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82 | _minLevelE = _levelManager->MinLevelEnergy(); |
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83 | |
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84 | // Energy range for photon generation; upper limit is defined 5*Gamma(GDR) from GDR peak |
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85 | _eMin = 0.001 * MeV; |
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86 | // Giant Dipole Resonance energy |
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87 | G4double energyGDR = (40.3 / std::pow(G4double(_nucleusA),0.2) ) * MeV; |
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88 | // Giant Dipole Resonance width |
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89 | G4double widthGDR = 0.30 * energyGDR; |
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90 | // Extend |
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91 | G4double factor = 5; |
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92 | _eMax = energyGDR + factor * widthGDR; |
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93 | if (_eMax > excitation) _eMax = _excitation; |
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94 | |
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95 | } |
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96 | |
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97 | // |
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98 | // Destructor |
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99 | // |
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100 | |
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101 | G4ContinuumGammaTransition::~G4ContinuumGammaTransition() {} |
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102 | |
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103 | // |
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104 | // Override GammaEnergy function from G4VGammaTransition |
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105 | // |
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106 | |
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107 | void G4ContinuumGammaTransition::SelectGamma() |
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108 | { |
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109 | |
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110 | _eGamma = 0.; |
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111 | |
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112 | G4int nBins = 200; |
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113 | G4double sampleArray[200]; |
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114 | G4int i; |
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115 | for (i=0; i<nBins; i++) |
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116 | { |
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117 | G4double e = _eMin + ( (_eMax - _eMin) / nBins) * i; |
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118 | sampleArray[i] = E1Pdf(e); |
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119 | |
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120 | if(_verbose > 10) |
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121 | G4cout << "*---* G4ContinuumTransition: e = " << e |
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122 | << " pdf = " << sampleArray[i] << G4endl; |
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123 | } |
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124 | G4RandGeneralTmp randGeneral(sampleArray, nBins); |
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125 | G4double random = randGeneral.shoot(); |
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126 | |
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127 | _eGamma = _eMin + (_eMax - _eMin) * random; |
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128 | |
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129 | G4double finalExcitation = _excitation - _eGamma; |
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130 | |
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131 | if(_verbose > 10) |
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132 | G4cout << "*---*---* G4ContinuumTransition: eGamma = " << _eGamma |
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133 | << " finalExcitation = " << finalExcitation |
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134 | << " random = " << random << G4endl; |
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135 | |
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136 | // if (finalExcitation < 0) |
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137 | if(finalExcitation < _minLevelE/2.) |
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138 | { |
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139 | _eGamma = _excitation; |
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140 | finalExcitation = 0.; |
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141 | } |
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142 | |
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143 | if (finalExcitation < _maxLevelE && finalExcitation > 0.) |
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144 | { |
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145 | G4double levelE = _levelManager->NearestLevel(finalExcitation)->Energy(); |
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146 | G4double diff = finalExcitation - levelE; |
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147 | _eGamma = _eGamma + diff; |
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148 | } |
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149 | |
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150 | _gammaCreationTime = GammaTime(); |
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151 | |
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152 | if(_verbose > 10) |
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153 | G4cout << "*---*---* G4ContinuumTransition: _gammaCreationTime = " |
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154 | << _gammaCreationTime/second << G4endl; |
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155 | |
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156 | return; |
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157 | } |
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158 | |
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159 | G4double G4ContinuumGammaTransition::GetGammaEnergy() |
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160 | { |
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161 | return _eGamma; |
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162 | } |
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163 | |
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164 | G4double G4ContinuumGammaTransition::GetGammaCreationTime() |
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165 | { |
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166 | return _gammaCreationTime; |
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167 | } |
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168 | |
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169 | |
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170 | void G4ContinuumGammaTransition::SetEnergyFrom(const G4double energy) |
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171 | { |
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172 | |
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173 | if (energy > 0.) _excitation = energy; |
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174 | return; |
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175 | |
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176 | } |
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177 | |
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178 | |
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179 | G4double G4ContinuumGammaTransition::E1Pdf(G4double e) |
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180 | { |
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181 | G4double theProb = 0.0; |
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182 | |
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183 | if( (_excitation - e) < 0.0 || e < 0 || _excitation < 0) return theProb; |
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184 | |
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185 | G4ConstantLevelDensityParameter ldPar; |
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186 | G4double aLevelDensityParam = ldPar.LevelDensityParameter(_nucleusA,_nucleusZ,_excitation); |
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187 | |
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188 | G4double levelDensBef = std::exp(2.0*std::sqrt(aLevelDensityParam*_excitation)); |
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189 | G4double levelDensAft = std::exp(2.0*std::sqrt(aLevelDensityParam*(_excitation - e))); |
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190 | |
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191 | if(_verbose > 20) |
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192 | G4cout << _nucleusA << " LevelDensityParameter = " << aLevelDensityParam |
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193 | << " Bef Aft " << levelDensBef << " " << levelDensAft << G4endl; |
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194 | |
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195 | // Now form the probability density |
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196 | |
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197 | // Define constants for the photoabsorption cross-section (the reverse |
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198 | // process of our de-excitation) |
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199 | |
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200 | // G4double sigma0 = 2.5 * _nucleusA * millibarn; |
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201 | G4double sigma0 = 2.5 * _nucleusA; |
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202 | |
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203 | G4double Egdp = (40.3 / std::pow(G4double(_nucleusA),0.2) )*MeV; |
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204 | G4double GammaR = 0.30 * Egdp; |
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205 | |
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206 | G4double normC = 1.0 / (pi * hbarc)*(pi * hbarc); |
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207 | |
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208 | G4double numerator = sigma0 * e*e * GammaR*GammaR; |
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209 | G4double denominator = (e*e - Egdp*Egdp)* (e*e - Egdp*Egdp) + GammaR*GammaR*e*e; |
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210 | // if (denominator < 1.0e-9) denominator = 1.0e-9; |
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211 | |
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212 | G4double sigmaAbs = numerator/denominator ; |
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213 | |
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214 | if(_verbose > 20) |
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215 | G4cout << ".. " << Egdp << " .. " << GammaR |
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216 | << " .. " << normC << " .. " << sigmaAbs |
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217 | << " .. " << e*e << " .. " << levelDensAft/levelDensBef |
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218 | << G4endl; |
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219 | |
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220 | // theProb = normC * sigmaAbs * e*e * levelDensAft/levelDensBef; |
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221 | theProb = sigmaAbs * e*e * levelDensAft/levelDensBef; |
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222 | |
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223 | return theProb; |
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224 | } |
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225 | |
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226 | |
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227 | G4double G4ContinuumGammaTransition::GammaTime() |
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228 | { |
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229 | |
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230 | G4double GammaR = 0.30 * (40.3 / std::pow(G4double(_nucleusA),0.2) )*MeV; |
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231 | G4double tau = hbar_Planck/GammaR; |
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232 | |
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233 | G4double tMin = 0; |
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234 | G4double tMax = 10.0 * tau; |
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235 | G4int nBins = 200; |
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236 | G4double sampleArray[200]; |
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237 | |
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238 | for(G4int i = 0;i<nBins;i++) |
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239 | { |
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240 | G4double t = tMin + ((tMax-tMin)/nBins)*i; |
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241 | sampleArray[i] = (std::exp(-t/tau))/tau; |
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242 | } |
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243 | |
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244 | G4RandGeneralTmp randGeneral(sampleArray, nBins); |
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245 | G4double random = randGeneral.shoot(); |
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246 | |
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247 | G4double creationTime = tMin + (tMax - tMin) * random; |
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248 | |
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249 | return creationTime; |
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250 | } |
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251 | |
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252 | |
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253 | |
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254 | |
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256 | |
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262 | |
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