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 | // $Id: G4N14GEMProbability.cc,v 1.6 2009/09/15 12:54:17 vnivanch Exp $ |
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28 | // GEANT4 tag $Name: geant4-09-03-ref-09 $ |
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29 | // |
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30 | // Hadronic Process: Nuclear De-excitations |
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31 | // by V. Lara (Nov 1999) |
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32 | // |
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33 | |
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34 | |
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35 | #include "G4N14GEMProbability.hh" |
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36 | |
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37 | G4N14GEMProbability::G4N14GEMProbability() : |
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38 | G4GEMProbability(14,7,1.0) // A,Z,Spin |
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39 | { |
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40 | |
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41 | ExcitEnergies.push_back(2312.87*keV); |
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42 | ExcitSpins.push_back(0.0); |
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43 | ExcitLifetimes.push_back(60e-15*s); |
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44 | |
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45 | ExcitEnergies.push_back(3947.8*keV); |
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46 | ExcitSpins.push_back(1.0); |
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47 | ExcitLifetimes.push_back(3.1e-15*s); |
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48 | |
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49 | ExcitEnergies.push_back(4915.0*keV); |
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50 | ExcitSpins.push_back(0.0); |
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51 | ExcitLifetimes.push_back(5.3e-15*s); |
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52 | |
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53 | ExcitEnergies.push_back(5105.87*keV); |
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54 | ExcitSpins.push_back(2.0); |
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55 | ExcitLifetimes.push_back(8.6e-12*s); |
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56 | |
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57 | ExcitEnergies.push_back(5689.6*keV); |
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58 | ExcitSpins.push_back(1.0); |
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59 | ExcitLifetimes.push_back(6.9e-15*s); |
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60 | |
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61 | ExcitEnergies.push_back(5832.4*keV); |
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62 | ExcitSpins.push_back(3.0); |
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63 | ExcitLifetimes.push_back(12.5e-12*s); |
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64 | |
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65 | ExcitEnergies.push_back(6203.5*keV); |
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66 | ExcitSpins.push_back(1.0); |
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67 | ExcitLifetimes.push_back(86e-15*s); |
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68 | |
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69 | ExcitEnergies.push_back(6444.4*keV); |
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70 | ExcitSpins.push_back(3.0); |
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71 | ExcitLifetimes.push_back(435e-15*s); |
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72 | |
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73 | ExcitEnergies.push_back(7027.9*keV); |
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74 | ExcitSpins.push_back(2.0); |
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75 | ExcitLifetimes.push_back(3.7e-15*s); |
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76 | |
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77 | ExcitEnergies.push_back(7966.6*keV); |
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78 | ExcitSpins.push_back(2.0); |
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79 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.5E-3*keV)); |
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80 | |
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81 | ExcitEnergies.push_back(8487.7*keV); |
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82 | ExcitSpins.push_back(4.0); |
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83 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(27E-6*keV)); |
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84 | |
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85 | ExcitEnergies.push_back(8618*keV); |
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86 | ExcitSpins.push_back(0.0); |
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87 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7.0*keV)); |
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88 | |
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89 | ExcitEnergies.push_back(8790*keV); |
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90 | ExcitSpins.push_back(0.0); |
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91 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(460*keV)); |
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92 | |
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93 | ExcitEnergies.push_back(8909.1*keV); |
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94 | ExcitSpins.push_back(3.0); |
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95 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(19.7*keV)); |
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96 | |
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97 | ExcitEnergies.push_back(8961.2 *keV); |
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98 | ExcitSpins.push_back(5.0); |
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99 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7E-6*keV)); |
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100 | |
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101 | ExcitEnergies.push_back(8979*keV); |
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102 | ExcitSpins.push_back(2.0); |
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103 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(8*keV)); |
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104 | |
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105 | ExcitEnergies.push_back(9129*keV); |
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106 | ExcitSpins.push_back(2.0); |
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107 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1*keV)); |
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108 | |
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109 | ExcitEnergies.push_back(9170.8*keV); |
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110 | ExcitSpins.push_back(2.0); |
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111 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.074*keV)); |
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112 | |
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113 | ExcitEnergies.push_back(9386.0*keV); |
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114 | ExcitSpins.push_back(3.0); |
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115 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(15.6 *keV)); |
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116 | |
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117 | ExcitEnergies.push_back(9509*keV); |
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118 | ExcitSpins.push_back(2.0); |
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119 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(41*keV)); |
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120 | |
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121 | ExcitEnergies.push_back(9703 *keV); |
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122 | ExcitSpins.push_back(1.0); |
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123 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(15*keV)); |
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124 | |
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125 | ExcitEnergies.push_back(10063*keV); |
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126 | ExcitSpins.push_back(3.0); |
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127 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(10*keV)); |
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128 | |
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129 | ExcitEnergies.push_back(10101*keV); |
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130 | ExcitSpins.push_back(1.0); |
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131 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5*keV)); |
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132 | |
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133 | ExcitEnergies.push_back(10228*keV); |
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134 | ExcitSpins.push_back(1.0); |
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135 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(80*keV)); |
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136 | |
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137 | ExcitEnergies.push_back(10434*keV); |
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138 | ExcitSpins.push_back(2.0); |
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139 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(33*keV)); |
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140 | |
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141 | ExcitEnergies.push_back(10540*keV); |
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142 | ExcitSpins.push_back(1.0); |
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143 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(140*keV)); |
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144 | |
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145 | ExcitEnergies.push_back(10811*keV); |
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146 | ExcitSpins.push_back(5.0); |
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147 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.39*eV)); |
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148 | |
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149 | ExcitEnergies.push_back(11050*keV); |
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150 | ExcitSpins.push_back(3.0); |
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151 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2*keV)); |
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152 | |
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153 | ExcitEnergies.push_back(11070*keV); |
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154 | ExcitSpins.push_back(1.0); |
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155 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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156 | |
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157 | ExcitEnergies.push_back(11240*keV); |
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158 | ExcitSpins.push_back(3.0); |
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159 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20*keV)); |
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160 | |
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161 | ExcitEnergies.push_back(11290*keV); |
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162 | ExcitSpins.push_back(2.0); |
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163 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(180*keV)); |
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164 | |
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165 | ExcitEnergies.push_back(11357*keV); |
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166 | ExcitSpins.push_back(1.0); |
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167 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30*keV)); |
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168 | |
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169 | ExcitEnergies.push_back(11513.6*keV); |
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170 | ExcitSpins.push_back(3.0); |
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171 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7.0*keV)); |
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172 | |
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173 | ExcitEnergies.push_back(11680*keV); |
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174 | ExcitSpins.push_back(2.0); |
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175 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(150*keV)); |
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176 | |
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177 | ExcitEnergies.push_back(11741*keV); |
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178 | ExcitSpins.push_back(2.0); |
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179 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40*keV)); |
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180 | |
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181 | ExcitEnergies.push_back(11761*keV); |
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182 | ExcitSpins.push_back(4.0); |
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183 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(78*keV)); |
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184 | |
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185 | ExcitEnergies.push_back(11807*keV); |
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186 | ExcitSpins.push_back(2.0); |
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187 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(119*keV)); |
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188 | |
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189 | ExcitEnergies.push_back(11874*keV); |
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190 | ExcitSpins.push_back(2.0); |
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191 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(101*keV)); |
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192 | |
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193 | ExcitEnergies.push_back(12200*keV); |
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194 | ExcitSpins.push_back(2.0); |
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195 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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196 | |
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197 | ExcitEnergies.push_back(12408*keV); |
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198 | ExcitSpins.push_back(3.0); |
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199 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(37*keV)); |
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200 | |
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201 | ExcitEnergies.push_back(12418*keV); |
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202 | ExcitSpins.push_back(4.0); |
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203 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(41*keV)); |
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204 | |
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205 | ExcitEnergies.push_back(12594*keV); |
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206 | ExcitSpins.push_back(3.0); |
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207 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(48*keV)); |
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208 | |
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209 | ExcitEnergies.push_back(12688*keV); |
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210 | ExcitSpins.push_back(3.0); |
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211 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(22*keV)); |
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212 | |
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213 | ExcitEnergies.push_back(12792*keV); |
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214 | ExcitSpins.push_back(4.0); |
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215 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(18*keV)); |
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216 | |
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217 | ExcitEnergies.push_back(12819*keV); |
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218 | ExcitSpins.push_back(4.0); |
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219 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(8*keV)); |
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220 | |
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221 | ExcitEnergies.push_back(12923*keV); |
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222 | ExcitSpins.push_back(4.0); |
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223 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(25*keV)); |
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224 | |
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225 | ExcitEnergies.push_back(13166*keV); |
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226 | ExcitSpins.push_back(1.0); |
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227 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(15*keV)); |
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228 | |
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229 | ExcitEnergies.push_back(13192*keV); |
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230 | ExcitSpins.push_back(3.0); |
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231 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(65*keV)); |
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232 | |
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233 | ExcitEnergies.push_back(13243*keV); |
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234 | ExcitSpins.push_back(2.0); |
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235 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(92*keV)); |
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236 | |
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237 | ExcitEnergies.push_back(13300*keV); |
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238 | ExcitSpins.push_back(2.0); |
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239 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000*keV)); |
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240 | |
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241 | ExcitEnergies.push_back(13656*keV); |
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242 | ExcitSpins.push_back(3.0); |
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243 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(90*keV)); |
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244 | |
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245 | ExcitEnergies.push_back(13714*keV); |
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246 | ExcitSpins.push_back(3.0); |
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247 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(105*keV)); |
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248 | |
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249 | ExcitEnergies.push_back(13710*keV); |
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250 | ExcitSpins.push_back(1.0); |
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251 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(180*keV)); |
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252 | |
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253 | ExcitEnergies.push_back(14250*keV); |
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254 | ExcitSpins.push_back(3.0); |
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255 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(420*keV)); |
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256 | |
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257 | ExcitEnergies.push_back(14660*keV); |
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258 | ExcitSpins.push_back(2.0); |
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259 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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260 | |
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261 | ExcitEnergies.push_back(16800*keV); |
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262 | ExcitSpins.push_back(4.0); |
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263 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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264 | |
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265 | ExcitEnergies.push_back(16910*keV); |
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266 | ExcitSpins.push_back(5.0); |
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267 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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268 | |
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269 | ExcitEnergies.push_back(17170*keV); |
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270 | ExcitSpins.push_back(4.0); |
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271 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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272 | |
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273 | ExcitEnergies.push_back(18100*keV); |
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274 | ExcitSpins.push_back(2.0); |
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275 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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276 | |
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277 | ExcitEnergies.push_back(18100*keV); |
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278 | ExcitSpins.push_back(4.0); |
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279 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600*keV)); |
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280 | |
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281 | ExcitEnergies.push_back(18200*keV); |
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282 | ExcitSpins.push_back(3.0); |
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283 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400*keV)); |
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284 | |
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285 | ExcitEnergies.push_back(18400*keV); |
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286 | ExcitSpins.push_back(3.0); |
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287 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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288 | |
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289 | ExcitEnergies.push_back(18500*keV); |
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290 | ExcitSpins.push_back(5.0); |
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291 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(60 *keV)); |
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292 | |
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293 | ExcitEnergies.push_back(18800*keV); |
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294 | ExcitSpins.push_back(4.0); |
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295 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400*keV)); |
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296 | |
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297 | ExcitEnergies.push_back(20100*keV); |
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298 | ExcitSpins.push_back(1.0); |
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299 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500*keV)); |
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300 | |
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301 | ExcitEnergies.push_back(20800*keV); |
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302 | ExcitSpins.push_back(5.0); |
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303 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600*keV)); |
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304 | |
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305 | ExcitEnergies.push_back(20800*keV); |
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306 | ExcitSpins.push_back(4.0); |
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307 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500*keV)); |
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308 | |
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309 | ExcitEnergies.push_back(21300*keV); |
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310 | ExcitSpins.push_back(4.0); |
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311 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000*keV)); |
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312 | |
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313 | ExcitEnergies.push_back(21500*keV); |
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314 | ExcitSpins.push_back(3.0); |
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315 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500*keV)); |
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316 | |
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317 | ExcitEnergies.push_back(21700*keV); |
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318 | ExcitSpins.push_back(5.0); |
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319 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200*keV)); |
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320 | |
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321 | ExcitEnergies.push_back(23000*keV); |
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322 | ExcitSpins.push_back(1.0); |
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323 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3000*keV)); |
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324 | |
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325 | ExcitEnergies.push_back(23.3E3*keV); |
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326 | ExcitSpins.push_back(5.0); |
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327 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500*keV)); |
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328 | |
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329 | SetExcitationEnergiesPtr(&ExcitEnergies); |
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330 | SetExcitationSpinsPtr(&ExcitSpins); |
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331 | SetExcitationLifetimesPtr(&ExcitLifetimes); |
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332 | } |
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333 | |
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334 | |
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335 | G4N14GEMProbability::G4N14GEMProbability(const G4N14GEMProbability &) : G4GEMProbability() |
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336 | { |
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337 | throw G4HadronicException(__FILE__, __LINE__, "G4N14GEMProbability::copy_constructor meant to not be accessable"); |
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338 | } |
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339 | |
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340 | |
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341 | |
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342 | |
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343 | const G4N14GEMProbability & G4N14GEMProbability:: |
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344 | operator=(const G4N14GEMProbability &) |
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345 | { |
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346 | throw G4HadronicException(__FILE__, __LINE__, "G4N14GEMProbability::operator= meant to not be accessable"); |
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347 | return *this; |
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348 | } |
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349 | |
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350 | |
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351 | G4bool G4N14GEMProbability::operator==(const G4N14GEMProbability &) const |
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352 | { |
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353 | return false; |
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354 | } |
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355 | |
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356 | G4bool G4N14GEMProbability::operator!=(const G4N14GEMProbability &) const |
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357 | { |
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358 | return true; |
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359 | } |
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360 | |
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361 | |
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362 | |
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