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 | // For information related to this code contact: |
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31 | // CERN, IT Division, ASD group |
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32 | // CERN, Geneva, Switzerland |
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33 | // |
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34 | // File name: G4NuclearLevel |
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35 | // |
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36 | // Author: Maria Grazia Pia (pia@genova.infn.it) |
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37 | // |
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38 | // Creation date: 24 October 1998 |
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39 | // |
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40 | // Modifications: |
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41 | // |
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42 | // 09 Sep. 2002, Fan Lei (flei@space.qinetiq.com) |
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43 | // Added IC probability when calculate the channel probabilities in |
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44 | // MakeProbabilities(). |
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45 | // |
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46 | // 21 Nov. 2001, Fan Lei (flei@space.qinetiq.com) |
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47 | // Added K->N+ internal conversion coefficiencies and their access |
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48 | // functions. |
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49 | // |
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50 | // 15 April 1999, Alessandro Brunengo (Alessandro.Brunengo@ge.infn.it) |
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51 | // Added half-life, angular momentum, parity, emissioni type |
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52 | // reading from experimental data. |
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53 | // |
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54 | // ------------------------------------------------------------------- |
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55 | |
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56 | #include "G4NuclearLevel.hh" |
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57 | |
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58 | #include "globals.hh" |
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59 | |
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60 | G4int G4NuclearLevel::Increment(G4int aF) |
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61 | { |
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62 | static G4int instanceCount = 0; |
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63 | instanceCount+=aF; |
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64 | return instanceCount; |
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65 | } |
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66 | |
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67 | G4NuclearLevel::G4NuclearLevel(const G4double energy, const G4double halfLife, |
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68 | const G4double angularMomentum, |
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69 | const std::vector<double>& eGamma, |
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70 | const std::vector<double>& wGamma, |
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71 | const std::vector<double>& polarities, |
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72 | const std::vector<double>& kCC, const std::vector<double>& l1CC, |
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73 | const std::vector<double>& l2CC, const std::vector<double>& l3CC, |
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74 | const std::vector<double>& m1CC, const std::vector<double>& m2CC, |
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75 | const std::vector<double>& m3CC, const std::vector<double>& m4CC, |
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76 | const std::vector<double>& m5CC, const std::vector<double>& nPlusCC, |
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77 | const std::vector<double>& totalCC) |
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78 | |
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79 | { |
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80 | _energy = energy; |
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81 | _halfLife = halfLife; |
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82 | _angularMomentum = angularMomentum; |
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83 | unsigned int i; |
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84 | for (i=0; i<eGamma.size(); i++) |
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85 | { |
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86 | _energies.push_back(eGamma[i]); |
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87 | _weights.push_back(wGamma[i]); |
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88 | _polarities.push_back(polarities[i]); |
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89 | _kCC.push_back( kCC[i]); |
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90 | _l1CC.push_back( l1CC[i]); |
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91 | _l2CC.push_back( l2CC[i]); |
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92 | _l3CC.push_back( l3CC[i]); |
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93 | _m1CC.push_back( m1CC[i]); |
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94 | _m2CC.push_back( m2CC[i]); |
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95 | _m3CC.push_back( m3CC[i]); |
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96 | _m4CC.push_back( m4CC[i]); |
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97 | _m5CC.push_back( m5CC[i]); |
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98 | _nPlusCC.push_back( nPlusCC[i]); |
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99 | _totalCC.push_back( totalCC[i]); |
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100 | } |
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101 | _nGammas = _energies.size(); |
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102 | MakeProbabilities(); |
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103 | MakeCumProb(); |
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104 | // G4cout << "####### Incrementing "<<Increment(1)<<G4endl; |
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105 | } |
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106 | |
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107 | G4NuclearLevel::~G4NuclearLevel() |
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108 | { |
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109 | // G4cout << "####### Decrementing "<<Increment(-1)<<G4endl; |
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110 | } |
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111 | |
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112 | |
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113 | G4bool G4NuclearLevel::operator==(const G4NuclearLevel &right) const |
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114 | { |
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115 | return (this == (G4NuclearLevel *) &right); |
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116 | } |
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117 | |
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118 | |
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119 | G4bool G4NuclearLevel::operator!=(const G4NuclearLevel &right) const |
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120 | { |
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121 | return (this != (G4NuclearLevel *) &right); |
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122 | } |
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123 | |
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124 | |
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125 | G4bool G4NuclearLevel::operator<(const G4NuclearLevel &right) const |
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126 | { |
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127 | if (_energy < right.Energy()) return true; |
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128 | else return false; |
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129 | } |
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130 | |
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131 | |
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132 | const std::vector<double>& G4NuclearLevel::GammaEnergies() const |
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133 | { |
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134 | return _energies; |
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135 | } |
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136 | |
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137 | const std::vector<double>& G4NuclearLevel::GammaWeights() const |
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138 | { |
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139 | return _weights; |
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140 | } |
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141 | |
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142 | |
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143 | const std::vector<double>& G4NuclearLevel::GammaProbabilities() const |
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144 | { |
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145 | return _prob; |
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146 | } |
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147 | |
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148 | |
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149 | const std::vector<double>& G4NuclearLevel::GammaCumulativeProbabilities() const |
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150 | { |
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151 | return _cumProb; |
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152 | } |
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153 | |
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154 | |
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155 | const std::vector<double>& G4NuclearLevel::GammaPolarities() const |
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156 | { |
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157 | return _polarities; |
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158 | } |
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159 | |
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160 | const std::vector<double>& G4NuclearLevel::KConvertionProbabilities() const |
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161 | { |
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162 | return _kCC; |
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163 | } |
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164 | |
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165 | const std::vector<double>& G4NuclearLevel::L1ConvertionProbabilities() const |
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166 | { |
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167 | return _l1CC; |
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168 | } |
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169 | |
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170 | const std::vector<double>& G4NuclearLevel::L2ConvertionProbabilities() const |
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171 | { |
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172 | return _l2CC; |
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173 | } |
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174 | |
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175 | const std::vector<double>& G4NuclearLevel::L3ConvertionProbabilities() const |
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176 | { |
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177 | return _l3CC; |
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178 | } |
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179 | |
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180 | const std::vector<double>& G4NuclearLevel::M1ConvertionProbabilities() const |
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181 | { |
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182 | return _m1CC; |
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183 | } |
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184 | |
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185 | const std::vector<double>& G4NuclearLevel::M2ConvertionProbabilities() const |
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186 | { |
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187 | return _m2CC; |
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188 | } |
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189 | |
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190 | const std::vector<double>& G4NuclearLevel::M3ConvertionProbabilities() const |
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191 | { |
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192 | return _m3CC; |
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193 | } |
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194 | |
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195 | const std::vector<double>& G4NuclearLevel::M4ConvertionProbabilities() const |
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196 | { |
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197 | return _m4CC; |
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198 | } |
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199 | |
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200 | const std::vector<double>& G4NuclearLevel::M5ConvertionProbabilities() const |
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201 | { |
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202 | return _m5CC; |
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203 | } |
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204 | |
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205 | const std::vector<double>& G4NuclearLevel::NPlusConvertionProbabilities() const |
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206 | { |
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207 | return _nPlusCC; |
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208 | } |
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209 | |
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210 | const std::vector<double>& G4NuclearLevel::TotalConvertionProbabilities() const |
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211 | { |
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212 | return _totalCC; |
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213 | } |
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214 | |
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215 | G4double G4NuclearLevel::Energy() const |
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216 | { |
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217 | return _energy; |
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218 | } |
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219 | |
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220 | G4double G4NuclearLevel::AngularMomentum() const |
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221 | { |
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222 | return _angularMomentum; |
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223 | } |
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224 | |
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225 | G4double G4NuclearLevel::HalfLife() const |
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226 | { |
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227 | return _halfLife; |
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228 | } |
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229 | |
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230 | |
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231 | G4int G4NuclearLevel::NumberOfGammas() const |
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232 | { |
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233 | return _nGammas; |
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234 | } |
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235 | |
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236 | |
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237 | void G4NuclearLevel::PrintAll() const |
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238 | { |
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239 | G4cout << "---- Level energy = " << _energy << ", angular momentum = " |
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240 | << _angularMomentum << ", half life " << _halfLife |
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241 | << ", " << _nGammas << " photons" << G4endl; |
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242 | G4int i; |
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243 | G4cout << " Gammas: "; |
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244 | for (i=0; i<_nGammas; i++) { G4cout << _energies[i] << " "; } |
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245 | G4cout << G4endl << " Weights: "; |
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246 | for (i=0; i<_nGammas; i++) { G4cout << _weights[i] << " "; } |
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247 | G4cout << G4endl << " Relative transition probabilities "; |
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248 | for (i=0; i<_nGammas; i++) { G4cout << _prob[i] << " "; } |
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249 | G4cout << G4endl << " Cumulative probabilities: "; |
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250 | for (i=0; i<_nGammas; i++) { G4cout << _cumProb[i] << " "; } |
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251 | G4cout << G4endl << " Polarities: "; |
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252 | for (i=0; i<_nGammas; i++) { G4cout << _polarities[i] << " "; } |
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253 | G4cout << G4endl; |
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254 | |
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255 | return; |
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256 | } |
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257 | |
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258 | |
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259 | void G4NuclearLevel::MakeProbabilities() |
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260 | { |
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261 | G4double sum = 0.; |
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262 | G4int i = 0; |
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263 | for (i=0; i<_nGammas; i++) |
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264 | { |
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265 | sum += _weights[i]*(1+_totalCC[i]); |
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266 | } |
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267 | |
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268 | for (i=0; i<_nGammas; i++) |
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269 | { |
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270 | if (sum > 0.) { _prob.push_back(_weights[i]*(1+_totalCC[i])/ sum); } |
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271 | else { _prob.push_back(1./_nGammas); } |
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272 | } |
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273 | return; |
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274 | } |
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275 | |
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276 | |
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277 | void G4NuclearLevel::MakeCumProb() |
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278 | { |
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279 | if (_nGammas > 0) |
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280 | { |
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281 | G4double sum = _prob[0]; |
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282 | _cumProb.push_back(sum); |
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283 | |
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284 | G4int i = 0; |
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285 | for (i=1; i<_nGammas; i++) |
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286 | { |
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287 | sum += _prob[i]; |
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288 | _cumProb.push_back(sum); |
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289 | } |
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290 | } |
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291 | return; |
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292 | } |
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293 | |
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294 | |
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295 | |
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