1 | // |
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2 | // ******************************************************************** |
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3 | // * License and Disclaimer * |
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4 | // * * |
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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 | // Implementation of the HETC88 code into Geant4. |
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28 | // Evaporation and De-excitation parts |
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29 | // T. Lampen, Helsinki Institute of Physics, May-2000 |
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30 | |
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31 | #include "globals.hh" |
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32 | #include "G4ios.hh" |
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33 | #include "Randomize.hh" |
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34 | #include "G4Neutron.hh" |
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35 | #include "G4Proton.hh" |
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36 | #include "G4Deuteron.hh" |
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37 | #include "G4Triton.hh" |
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38 | #include "G4Alpha.hh" |
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39 | #include "G4ParticleTable.hh" |
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40 | #include "G4Nucleus.hh" |
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41 | #include "G4BertiniEvaporationChannel.hh" |
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42 | |
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43 | |
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44 | G4BertiniEvaporationChannel::G4BertiniEvaporationChannel() |
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45 | { |
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46 | verboseLevel = 0; |
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47 | } |
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48 | |
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49 | |
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50 | G4BertiniEvaporationChannel::~G4BertiniEvaporationChannel() |
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51 | { |
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52 | } |
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53 | |
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54 | |
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55 | void G4BertiniEvaporationChannel::setVerboseLevel( G4int level ) |
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56 | { |
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57 | verboseLevel = level; |
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58 | } |
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59 | |
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60 | |
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61 | void G4BertiniEvaporationChannel::setNucleusA( G4int a ) |
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62 | { |
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63 | nucleusA = a; |
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64 | } |
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65 | |
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66 | |
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67 | void G4BertiniEvaporationChannel::setNucleusZ( G4int z ) |
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68 | { |
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69 | nucleusZ = z; |
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70 | } |
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71 | |
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72 | |
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73 | G4int G4BertiniEvaporationChannel::getParticleA() |
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74 | { |
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75 | return particleA; |
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76 | } |
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77 | |
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78 | |
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79 | G4int G4BertiniEvaporationChannel::getParticleZ() |
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80 | { |
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81 | return particleZ; |
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82 | } |
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83 | |
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84 | |
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85 | void G4BertiniEvaporationChannel::setExcitationEnergy(G4double energy ) |
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86 | { |
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87 | excitationEnergy = energy; |
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88 | } |
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89 | |
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90 | |
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91 | void G4BertiniEvaporationChannel::setPairingCorrection( G4int isCorrection ) |
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92 | { |
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93 | G4int residualZ = nucleusZ - particleZ; |
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94 | G4int residualA = nucleusA - particleA; |
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95 | |
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96 | // Note: pairing energy is zero for odd nucleon number. |
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97 | |
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98 | if ( isCorrection ) correction = pairingEnergyProtons( residualZ ) |
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99 | + pairingEnergyNeutrons( residualA - residualZ ); |
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100 | else correction = 0; |
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101 | } |
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102 | |
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103 | |
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104 | G4double G4BertiniEvaporationChannel::getProbability() |
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105 | { |
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106 | if ( verboseLevel >= 4 ) |
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107 | G4cout << "G4BerEvaporationChannel : probability of particle " << name |
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108 | << " is " << emissionProbability << G4endl; |
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109 | |
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110 | return emissionProbability; |
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111 | } |
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112 | |
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113 | |
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114 | G4String G4BertiniEvaporationChannel::getName() |
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115 | { |
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116 | return name; |
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117 | } |
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118 | |
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119 | |
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120 | void G4BertiniEvaporationChannel::setProbability( G4double newProb ) |
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121 | { |
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122 | emissionProbability = newProb; |
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123 | return; |
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124 | } |
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125 | |
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126 | |
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127 | G4double G4BertiniEvaporationChannel::getQ() |
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128 | { |
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129 | // The reaction Q is calculated by using the excess masses of the |
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130 | // secondary particle and the initial and residual nuclei |
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131 | G4int residualZ = nucleusZ - particleZ; |
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132 | G4int residualA = nucleusA - particleA; |
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133 | // G4int residualN = residualA - residualZ; |
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134 | // G4int nucleusN = nucleusA - nucleusZ; |
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135 | |
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136 | // All the following are by default in MeV |
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137 | const G4double e1 = G4NucleiProperties::GetMassExcess( residualA, residualZ ); |
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138 | const G4double e2 = G4NucleiProperties::GetMassExcess( nucleusA, nucleusZ ); |
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139 | |
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140 | return e1 - e2 + G4NucleiProperties::GetMassExcess( particleA, particleZ ); |
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141 | // In HETC88 : Mass excesses were calculated with the Cameron mass excess formula, |
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142 | // see Cameron, Canadian Journal of Physics, |
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143 | // vol. 35, 1957, p.1022 |
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144 | // Also mass excesses of particles were |
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145 | // 8.3675, 7.5851, 13.7279, 15.8381, 15.8195, 3.6092 for |
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146 | // n, p, D, T, 3He, 4He |
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147 | } |
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148 | |
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149 | |
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150 | G4double G4BertiniEvaporationChannel::getThresh() |
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151 | { |
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152 | G4double threshold = getQ() + getCoulomb(); |
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153 | return threshold; |
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154 | } |
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155 | |
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156 | |
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157 | G4double G4BertiniEvaporationChannel::getCoulomb() |
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158 | { |
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159 | G4int residualZ = nucleusZ - particleZ; |
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160 | G4int residualA = nucleusA - particleA; |
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161 | const G4double factor = 0.84696; // = e / ( 4 pi epsilon_0 r0 ) * 10^-6, r0=1.7E-15 |
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162 | // In HETC88 this factor was 0.88235, perhaps due to different r0 |
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163 | |
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164 | G4double coulomb = factor * particleZ * qmFactor() * residualZ / |
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165 | ( std::pow( G4double(residualA), 0.33333333 ) + rho ) * MeV; |
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166 | |
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167 | if ( verboseLevel >= 10 ) |
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168 | G4cout << " G4BertiniEvaporationChannel::getThresh() " << G4endl |
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169 | << " residualZ " << residualZ << G4endl |
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170 | << " residualA " << residualA << G4endl |
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171 | << " qmFactor " << qmFactor() << G4endl |
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172 | << " Q " << getQ() << G4endl |
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173 | << " rho " << rho << G4endl |
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174 | << " part Z " << particleZ << G4endl |
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175 | << " (correction) " << correction << G4endl; |
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176 | |
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177 | return coulomb; |
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178 | } |
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179 | |
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180 | |
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181 | G4double G4BertiniEvaporationChannel::qmFactor() |
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182 | { |
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183 | // Coefficient k_p for empirical cross section |
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184 | // formula presented in Dostrovsky, Phys. Rev., |
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185 | // vol. 116, 1959 |
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186 | return 0; |
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187 | } |
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188 | |
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189 | |
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190 | G4double G4BertiniEvaporationChannel::getLevelDensityParameter() |
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191 | { |
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192 | G4int residualZ = nucleusZ - particleZ; |
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193 | G4int residualA = nucleusA - particleA; |
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194 | G4double b0 = 8; |
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195 | G4double y0 = 1.5; |
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196 | |
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197 | G4double temp = ( residualA - 2.0 * residualZ ) / residualA; |
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198 | G4double smallA = residualA * ( 1.0 + y0 * std::pow( temp, 2. ) ) / b0 / MeV; |
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199 | |
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200 | // In HETC98 b0 = b0(E). |
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201 | |
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202 | return smallA; |
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203 | } |
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204 | |
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205 | |
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206 | void G4BertiniEvaporationChannel::isotropicCosines( G4double & u, G4double & v, G4double & w ) |
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207 | { |
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208 | // Samples isotropic random direction cosines. |
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209 | G4double CosTheta = 1.0 - 2.0 * G4UniformRand(); |
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210 | G4double SinTheta = std::sqrt( 1.0 - CosTheta * CosTheta ); |
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211 | G4double Phi = twopi * G4UniformRand(); |
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212 | |
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213 | u = std::cos( Phi ) * SinTheta; |
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214 | v = std::cos( Phi ) * CosTheta, |
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215 | w = std::sin( Phi ); |
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216 | |
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217 | return; |
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218 | } |
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219 | |
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220 | |
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221 | G4double G4BertiniEvaporationChannel::pairingEnergyProtons(G4int Z) |
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222 | { |
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223 | // Pairing energy for protons P(Z), see |
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224 | // Cameron, Nuclear Level Spacings, p. 1040 |
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225 | // Canadian Journal of Physics, vol 36, 1958 |
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226 | G4double table [130] = { |
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227 | 0.00000000E+00, 0.54399996E+01, 0.00000000E+00, 0.27599993E+01, 0.00000000E+00, |
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228 | 0.33399992E+01, 0.00000000E+00, 0.26999998E+01, 0.00000000E+00, 0.18999996E+01, |
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229 | 0.00000000E+00, 0.21199999E+01, 0.00000000E+00, 0.21299992E+01, 0.00000000E+00, |
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230 | 0.15399990E+01, 0.00000000E+00, 0.14199991E+01, 0.00000000E+00, 0.15099993E+01, |
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231 | 0.00000000E+00, 0.17299995E+01, 0.00000000E+00, 0.14399996E+01, 0.00000000E+00, |
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232 | 0.14499998E+01, 0.00000000E+00, 0.13699999E+01, 0.00000000E+00, 0.10899992E+01, |
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233 | 0.00000000E+00, 0.13599997E+01, 0.00000000E+00, 0.14199991E+01, 0.00000000E+00, |
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234 | 0.13299990E+01, 0.00000000E+00, 0.11999998E+01, 0.00000000E+00, 0.99999988E+00, |
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235 | 0.00000000E+00, 0.11599998E+01, 0.00000000E+00, 0.12799997E+01, 0.00000000E+00, |
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236 | 0.13799992E+01, 0.00000000E+00, 0.13799992E+01, 0.00000000E+00, 0.13199997E+01, |
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237 | 0.00000000E+00, 0.10399990E+01, 0.00000000E+00, 0.11099997E+01, 0.00000000E+00, |
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238 | 0.11299992E+01, 0.00000000E+00, 0.12099991E+01, 0.00000000E+00, 0.14299994E+01, |
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239 | 0.00000000E+00, 0.11499996E+01, 0.00000000E+00, 0.98999995E+00, 0.00000000E+00, |
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240 | 0.90999997E+00, 0.00000000E+00, 0.91999996E+00, 0.00000000E+00, 0.99999988E+00, |
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241 | 0.00000000E+00, 0.11099997E+01, 0.00000000E+00, 0.12299995E+01, 0.00000000E+00, |
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242 | 0.84999996E+00, 0.00000000E+00, 0.97999996E+00, 0.00000000E+00, 0.71999997E+00, |
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243 | 0.00000000E+00, 0.79999995E+00, 0.00000000E+00, 0.76999998E+00, 0.00000000E+00, |
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244 | 0.88999999E+00, 0.00000000E+00, 0.91999996E+00, 0.00000000E+00, 0.79999995E+00, |
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245 | 0.00000000E+00, 0.80999994E+00, 0.00000000E+00, 0.69000000E+00, 0.00000000E+00, |
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246 | 0.69999999E+00, 0.00000000E+00, 0.75999999E+00, 0.00000000E+00, 0.72999996E+00, |
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247 | 0.00000000E+00, 0.79999995E+00, 0.00000000E+00, 0.73999995E+00, 0.00000000E+00, |
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248 | 0.72999996E+00, 0.00000000E+00, 0.71999997E+00, 0.00000000E+00, 0.71999997E+00, |
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249 | 0.00000000E+00, 0.71999997E+00, 0.00000000E+00, 0.70999998E+00, 0.00000000E+00, |
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250 | 0.69000000E+00, 0.00000000E+00, 0.67999995E+00, 0.00000000E+00, 0.65999997E+00, |
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251 | 0.00000000E+00, 0.60999995E+00, 0.00000000E+00, 0.41999996E+00, 0.00000000E+00, |
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252 | 0.35999995E+00, 0.00000000E+00, 0.40999997E+00, 0.00000000E+00, 0.48999995E+00 |
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253 | }; |
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254 | if ( Z>130 ) throw G4HadronicException(__FILE__, __LINE__, " G4BertiniEvaporationChannel: pairing energy for protons called with too large Z " ); |
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255 | return table[ Z-1 ]*MeV; |
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256 | } |
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257 | |
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258 | |
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259 | G4double G4BertiniEvaporationChannel::pairingEnergyNeutrons(G4int N) |
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260 | { |
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261 | // Pairing energy for neutrons P(N), see |
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262 | // Cameron, Nuclear Level Spacings, p. 1040 |
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263 | // Canadian Journal of Physics, vol 36, 1958 |
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264 | G4double table[200] = { |
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265 | 0.00000000E+00, 0.59799995E+01, 0.00000000E+00, 0.27699995E+01, 0.00000000E+00, |
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266 | 0.31599998E+01, 0.00000000E+00, 0.30099993E+01, 0.00000000E+00, 0.16799994E+01, |
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267 | 0.00000000E+00, 0.17299995E+01, 0.00000000E+00, 0.21699991E+01, 0.00000000E+00, |
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268 | 0.17399998E+01, 0.00000000E+00, 0.17500000E+01, 0.00000000E+00, 0.17199993E+01, |
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269 | 0.00000000E+00, 0.16299992E+01, 0.00000000E+00, 0.14099998E+01, 0.00000000E+00, |
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270 | 0.12899990E+01, 0.00000000E+00, 0.14699993E+01, 0.00000000E+00, 0.13199997E+01, |
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271 | 0.00000000E+00, 0.14599991E+01, 0.00000000E+00, 0.14399996E+01, 0.00000000E+00, |
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272 | 0.14599991E+01, 0.00000000E+00, 0.15199995E+01, 0.00000000E+00, 0.15099993E+01, |
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273 | 0.00000000E+00, 0.14699993E+01, 0.00000000E+00, 0.14499998E+01, 0.00000000E+00, |
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274 | 0.12799997E+01, 0.00000000E+00, 0.12299995E+01, 0.00000000E+00, 0.12699995E+01, |
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275 | 0.00000000E+00, 0.61999995E+00, 0.00000000E+00, 0.75999999E+00, 0.00000000E+00, |
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276 | 0.12299995E+01, 0.00000000E+00, 0.12199993E+01, 0.00000000E+00, 0.13999996E+01, |
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277 | 0.00000000E+00, 0.13599997E+01, 0.00000000E+00, 0.12999992E+01, 0.00000000E+00, |
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278 | 0.12899990E+01, 0.00000000E+00, 0.12399998E+01, 0.00000000E+00, 0.12799997E+01, |
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279 | 0.00000000E+00, 0.12399998E+01, 0.00000000E+00, 0.11999998E+01, 0.00000000E+00, |
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280 | 0.94000000E+00, 0.00000000E+00, 0.99999988E+00, 0.00000000E+00, 0.10499992E+01, |
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281 | 0.00000000E+00, 0.53999996E+00, 0.00000000E+00, 0.59999996E+00, 0.00000000E+00, |
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282 | 0.75000000E+00, 0.00000000E+00, 0.75000000E+00, 0.00000000E+00, 0.84999996E+00, |
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283 | 0.00000000E+00, 0.96999997E+00, 0.00000000E+00, 0.10199995E+01, 0.00000000E+00, |
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284 | 0.10499992E+01, 0.00000000E+00, 0.10599995E+01, 0.00000000E+00, 0.10699997E+01, |
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285 | 0.00000000E+00, 0.10599995E+01, 0.00000000E+00, 0.10499992E+01, 0.00000000E+00, |
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286 | 0.10199995E+01, 0.00000000E+00, 0.96999997E+00, 0.00000000E+00, 0.90999997E+00, |
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287 | 0.00000000E+00, 0.82999998E+00, 0.00000000E+00, 0.73999995E+00, 0.00000000E+00, |
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288 | 0.65999997E+00, 0.00000000E+00, 0.60999995E+00, 0.00000000E+00, 0.60999995E+00, |
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289 | 0.00000000E+00, 0.89999998E+00, 0.00000000E+00, 0.51999998E+00, 0.00000000E+00, |
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290 | 0.80999994E+00, 0.00000000E+00, 0.67999995E+00, 0.00000000E+00, 0.71999997E+00, |
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291 | 0.00000000E+00, 0.76999998E+00, 0.00000000E+00, 0.67999995E+00, 0.00000000E+00, |
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292 | 0.66999996E+00, 0.00000000E+00, 0.79999995E+00, 0.00000000E+00, 0.67999995E+00, |
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293 | 0.00000000E+00, 0.63999999E+00, 0.00000000E+00, 0.57999998E+00, 0.00000000E+00, |
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294 | 0.54999995E+00, 0.00000000E+00, 0.56999993E+00, 0.00000000E+00, 0.56999993E+00, |
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295 | 0.00000000E+00, 0.54999995E+00, 0.00000000E+00, 0.59999996E+00, 0.00000000E+00, |
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296 | 0.57999998E+00, 0.00000000E+00, 0.57999998E+00, 0.00000000E+00, 0.60999995E+00, |
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297 | 0.00000000E+00, 0.63000000E+00, 0.00000000E+00, 0.64999998E+00, 0.00000000E+00, |
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298 | 0.65999997E+00, 0.00000000E+00, 0.64999998E+00, 0.00000000E+00, 0.64999998E+00, |
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299 | 0.00000000E+00, 0.63999999E+00, 0.00000000E+00, 0.63999999E+00, 0.00000000E+00, |
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300 | 0.63000000E+00, 0.00000000E+00, 0.60999995E+00, 0.00000000E+00, 0.58999997E+00, |
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301 | 0.00000000E+00, 0.54999995E+00, 0.00000000E+00, 0.38999999E+00, 0.00000000E+00, |
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302 | 0.35999995E+00, 0.00000000E+00, 0.39999998E+00, 0.00000000E+00, 0.39999998E+00, |
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303 | 0.00000000E+00, 0.39999998E+00, 0.00000000E+00, 0.39999998E+00, 0.00000000E+00, |
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304 | 0.39999998E+00, 0.00000000E+00, 0.39999998E+00, 0.00000000E+00, 0.39999998E+00 |
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305 | }; |
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306 | if ( N > 200 ) throw G4HadronicException(__FILE__, __LINE__, " G4BertiniEvaporationChannel: pairing energy for neutrons called with too large Z " ); |
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307 | return table[ N-1 ]*MeV; |
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308 | } |
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309 | |
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310 | |
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311 | G4double G4BertiniEvaporationChannel::cameronShellCorrectionP(G4int Z) |
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312 | { |
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313 | // Gives the binding energy correction depending in Z |
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314 | // due to shell correction and pairing energies in MeV |
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315 | // |
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316 | // see Cameron, Canadian Journal of Physics, |
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317 | // vol. 35, 1957, p.1022 |
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318 | G4double table[130] = { |
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319 | 0.26169998E+02, 0.19250000E+02, 0.24209991E+02, 0.20919998E+02, 0.23149994E+02, |
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320 | 0.18009995E+02, 0.19549988E+02, 0.16939987E+02, 0.19729996E+02, 0.17069992E+02, |
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321 | 0.18209991E+02, 0.14990000E+02, 0.16009995E+02, 0.12040000E+02, 0.13270000E+02, |
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322 | 0.11089998E+02, 0.12169999E+02, 0.10259998E+02, 0.11040000E+02, 0.84099998E+01, |
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323 | 0.97899990E+01, 0.73599997E+01, 0.81499996E+01, 0.56299992E+01, 0.58799992E+01, |
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324 | 0.31699991E+01, 0.33199997E+01, 0.81999993E+00, 0.18299999E+01, 0.96999997E+00, |
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325 | 0.23299999E+01, 0.12699995E+01, 0.29199991E+01, 0.16099997E+01, 0.29099998E+01, |
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326 | 0.13499994E+01, 0.23999996E+01, 0.88999999E+00, 0.17399998E+01, 0.35999995E+00, |
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327 | 0.94999999E+00, -0.64999998E+00, -0.39999995E-01, -0.17299995E+01, -0.95999998E+00, |
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328 | -0.28699999E+01, -0.20499992E+01, -0.40499992E+01, -0.33999996E+01, -0.57199993E+01, |
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329 | -0.37499990E+01, -0.41299992E+01, -0.24199991E+01, -0.28499994E+01, -0.10099993E+01, |
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330 | -0.13299990E+01, 0.53999996E+00, -0.20000000E-01, 0.17399998E+01, 0.75000000E+00, |
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331 | 0.22399998E+01, 0.99999988E+00, 0.19799995E+01, 0.78999996E+00, 0.15399990E+01, |
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332 | 0.38999999E+00, 0.10799999E+01, 0.00000000E+00, 0.77999997E+00, -0.34999996E+00, |
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333 | 0.57999998E+00, -0.54999995E+00, 0.58999997E+00, -0.60999995E+00, 0.58999997E+00, |
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334 | -0.34999996E+00, 0.31999993E+00, -0.95999998E+00, -0.51999998E+00, -0.20799999E+01, |
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335 | -0.24599991E+01, -0.36399994E+01, -0.15499992E+01, -0.95999998E+00, 0.96999997E+00, |
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336 | 0.88000000E+00, 0.23699999E+01, 0.17500000E+01, 0.27199993E+01, 0.18999996E+01, |
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337 | 0.25499992E+01, 0.14599991E+01, 0.19299994E+01, 0.85999995E+00, 0.11699991E+01, |
---|
338 | 0.79999983E-01, 0.38999999E+00, -0.75999999E+00, -0.38999999E+00, -0.15099993E+01, |
---|
339 | -0.11699991E+01, -0.23599997E+01, -0.19499998E+01, -0.30599995E+01, -0.26199999E+01, |
---|
340 | -0.35499992E+01, -0.29499998E+01, -0.37499990E+01, -0.30699997E+01, -0.37899990E+01, |
---|
341 | -0.30599995E+01, -0.37699995E+01, -0.30499992E+01, -0.37799997E+01, -0.31199999E+01, |
---|
342 | -0.38999996E+01, -0.33499994E+01, -0.42399998E+01, -0.38599997E+01, -0.49199991E+01, |
---|
343 | -0.50599995E+01, -0.67699995E+01, -0.74099998E+01, -0.91799994E+01, -0.10160000E+02, |
---|
344 | -0.11120000E+02, -0.97599993E+01, -0.92299995E+01, -0.79599991E+01, -0.76499996E+01, |
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345 | }; |
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346 | if ( Z > 130 ) throw G4HadronicException(__FILE__, __LINE__, " G4BertiniEvaporationChannel: shell correction for protons called with too large Z " ); |
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347 | return table[ Z-1 ]*MeV; |
---|
348 | } |
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349 | |
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350 | |
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351 | G4double G4BertiniEvaporationChannel::cameronShellCorrectionN(G4int N) |
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352 | { |
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353 | // Gives the binding energy correction depending in N |
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354 | // due to shell correction and pairing energies in MeV |
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355 | // |
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356 | // see Cameron, Canadian Journal of Physics, |
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357 | // vol. 35, 1957, p.1022 |
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358 | G4double table[200] = { |
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359 | -0.83199997E+01, -0.15899999E+02, -0.11509999E+02, -0.14309999E+02, -0.11570000E+02, |
---|
360 | -0.15899999E+02, -0.13909999E+02, -0.16029999E+02, -0.12129999E+02, -0.13869999E+02, |
---|
361 | -0.12249998E+02, -0.14399999E+02, -0.13069999E+02, -0.15799998E+02, -0.13809999E+02, |
---|
362 | -0.14980000E+02, -0.12629999E+02, -0.13759999E+02, -0.11369999E+02, -0.12379998E+02, |
---|
363 | -0.92299995E+01, -0.96499996E+01, -0.76399994E+01, -0.91699991E+01, -0.80499992E+01, |
---|
364 | -0.97199993E+01, -0.88699989E+01, -0.10759999E+02, -0.86399994E+01, -0.88899994E+01, |
---|
365 | -0.65999994E+01, -0.71299992E+01, -0.47699995E+01, -0.53299990E+01, -0.30599995E+01, |
---|
366 | -0.37899990E+01, -0.17199993E+01, -0.27899990E+01, -0.92999995E+00, -0.21899996E+01, |
---|
367 | -0.51999998E+00, -0.18999996E+01, -0.44999999E+00, -0.21999998E+01, -0.12199993E+01, |
---|
368 | -0.30699997E+01, -0.24199991E+01, -0.43699999E+01, -0.39399996E+01, -0.60799999E+01, |
---|
369 | -0.44899998E+01, -0.45000000E+01, -0.31399994E+01, -0.29299994E+01, -0.10399990E+01, |
---|
370 | -0.13599997E+01, 0.69000000E+00, 0.20999998E+00, 0.21099997E+01, 0.13299990E+01, |
---|
371 | 0.32900000E+01, 0.24599991E+01, 0.42999992E+01, 0.33199997E+01, 0.47899990E+01, |
---|
372 | 0.36199999E+01, 0.49699993E+01, 0.36399994E+01, 0.46299992E+01, 0.30699997E+01, |
---|
373 | 0.40599995E+01, 0.24899998E+01, 0.32999992E+01, 0.14599991E+01, 0.20599995E+01, |
---|
374 | 0.50999999E+00, 0.73999995E+00, -0.11799994E+01, -0.12599993E+01, -0.35399990E+01, |
---|
375 | -0.39699993E+01, -0.52599993E+01, -0.41799994E+01, -0.37099991E+01, -0.20999994E+01, |
---|
376 | -0.16999998E+01, -0.79999983E-01, -0.17999995E+00, 0.94000000E+00, 0.26999998E+00, |
---|
377 | 0.11299992E+01, 0.79999983E-01, 0.90999997E+00, -0.30999994E+00, 0.48999995E+00, |
---|
378 | -0.77999997E+00, 0.79999983E-01, -0.11499996E+01, -0.22999996E+00, -0.14099998E+01, |
---|
379 | -0.41999996E+00, -0.15499992E+01, -0.54999995E+00, -0.16599998E+01, -0.65999997E+00, |
---|
380 | -0.17299995E+01, -0.75000000E+00, -0.17399998E+01, -0.77999997E+00, -0.16899996E+01, |
---|
381 | -0.77999997E+00, -0.15999994E+01, -0.75000000E+00, -0.14599991E+01, -0.66999996E+00, |
---|
382 | -0.12599993E+01, -0.50999999E+00, -0.10399990E+01, -0.52999997E+00, -0.18399992E+01, |
---|
383 | -0.24199991E+01, -0.45199995E+01, -0.47599993E+01, -0.63299990E+01, -0.67599993E+01, |
---|
384 | -0.78099995E+01, -0.57999992E+01, -0.53699999E+01, -0.36299992E+01, -0.33499994E+01, |
---|
385 | -0.17500000E+01, -0.18799992E+01, -0.60999995E+00, -0.89999998E+00, 0.89999974E-01, |
---|
386 | -0.31999993E+00, 0.54999995E+00, -0.13000000E+00, 0.69999999E+00, -0.59999999E-01, |
---|
387 | 0.48999995E+00, -0.19999999E+00, 0.39999998E+00, -0.21999997E+00, 0.35999995E+00, |
---|
388 | -0.89999974E-01, 0.57999998E+00, 0.11999995E+00, 0.75000000E+00, 0.14999998E+00, |
---|
389 | 0.69999999E+00, 0.16999996E+00, 0.11099997E+01, 0.88999999E+00, 0.18499994E+01, |
---|
390 | 0.16199999E+01, 0.25399990E+01, 0.22899990E+01, 0.31999998E+01, 0.29099998E+01, |
---|
391 | 0.38399992E+01, 0.35299997E+01, 0.44799995E+01, 0.41499996E+01, 0.51199999E+01, |
---|
392 | 0.47799997E+01, 0.57500000E+01, 0.53899994E+01, 0.63099995E+01, 0.59099998E+01, |
---|
393 | 0.68699999E+01, 0.63299990E+01, 0.71299992E+01, 0.66099997E+01, 0.72999992E+01, |
---|
394 | 0.63099995E+01, 0.62699995E+01, 0.48299999E+01, 0.44899998E+01, 0.28499994E+01, |
---|
395 | 0.23199997E+01, 0.57999998E+00, -0.10999995E+00, -0.97999996E+00, 0.80999994E+00, |
---|
396 | 0.17699995E+01, 0.33699999E+01, 0.41299992E+01, 0.55999994E+01, 0.61499996E+01, |
---|
397 | 0.72899990E+01, 0.73499994E+01, 0.79499998E+01, 0.76699991E+01, 0.81599998E+01, |
---|
398 | 0.78299990E+01, 0.83099995E+01, 0.80099993E+01, 0.85299997E+01, 0.82699995E+01 |
---|
399 | }; |
---|
400 | if ( N > 130 ) throw G4HadronicException(__FILE__, __LINE__, " G4BertiniEvaporationChannel: shell correction for protons called with too large N " ); |
---|
401 | return table[ N-1 ]*MeV; |
---|
402 | } |
---|
403 | |
---|