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: G4Na23GEMProbability.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 "G4Na23GEMProbability.hh" |
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36 | |
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37 | G4Na23GEMProbability::G4Na23GEMProbability() : |
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38 | G4GEMProbability(23,11,3.0/2.0) // A,Z,Spin |
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39 | { |
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40 | |
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41 | ExcitEnergies.push_back(439.80*keV); |
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42 | ExcitSpins.push_back(5.0/2.0); |
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43 | ExcitLifetimes.push_back(1109.0e-3*picosecond); |
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44 | |
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45 | ExcitEnergies.push_back(2076.4*keV); |
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46 | ExcitSpins.push_back(7.0/2.0); |
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47 | ExcitLifetimes.push_back(28.0e-3*picosecond); |
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48 | |
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49 | ExcitEnergies.push_back(2390.9*keV); |
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50 | ExcitSpins.push_back(1.0/2.0); |
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51 | ExcitLifetimes.push_back(555.0e-3*picosecond); |
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52 | |
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53 | ExcitEnergies.push_back(2639.8*keV); |
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54 | ExcitSpins.push_back(1.0/2.0); |
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55 | ExcitLifetimes.push_back(69.0e-3*picosecond); |
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56 | |
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57 | ExcitEnergies.push_back(2703.7*keV); |
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58 | ExcitSpins.push_back(9.0/2.0); |
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59 | ExcitLifetimes.push_back(76.0e-3*picosecond); |
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60 | |
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61 | ExcitEnergies.push_back(2982.4*keV); |
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62 | ExcitSpins.push_back(3.0/2.0); |
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63 | ExcitLifetimes.push_back(3.5e-3*picosecond); |
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64 | |
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65 | ExcitEnergies.push_back(3678.3*keV); |
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66 | ExcitSpins.push_back(3.0/2.0); |
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67 | ExcitLifetimes.push_back(22.0e-3*picosecond); |
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68 | |
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69 | ExcitEnergies.push_back(3848.2*keV); |
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70 | ExcitSpins.push_back(5.0/2.0); |
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71 | ExcitLifetimes.push_back(90.0e-3*picosecond); |
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72 | |
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73 | ExcitEnergies.push_back(3914.7*keV); |
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74 | ExcitSpins.push_back(5.0/2.0); |
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75 | ExcitLifetimes.push_back(7.6e-3*picosecond); |
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76 | |
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77 | ExcitEnergies.push_back(4432.0*keV); |
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78 | ExcitSpins.push_back(1.0/2.0); |
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79 | ExcitLifetimes.push_back(0.19e-3*picosecond); |
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80 | |
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81 | ExcitEnergies.push_back(4775.6*keV); |
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82 | ExcitSpins.push_back(7.0/2.0); |
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83 | ExcitLifetimes.push_back(1.4e-3*picosecond); |
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84 | |
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85 | ExcitEnergies.push_back(5377.0*keV); |
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86 | ExcitSpins.push_back(5.0/2.0); |
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87 | ExcitLifetimes.push_back(0.25e-3*picosecond); |
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88 | |
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89 | ExcitEnergies.push_back(5533.0*keV); |
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90 | ExcitSpins.push_back(11.0/2.0); |
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91 | ExcitLifetimes.push_back(8.0e-3*picosecond); |
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92 | |
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93 | ExcitEnergies.push_back(6117.0*keV); |
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94 | ExcitSpins.push_back(5.0/2.0); |
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95 | ExcitLifetimes.push_back(52.0e-3*picosecond); |
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96 | |
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97 | ExcitEnergies.push_back(6237.0*keV); |
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98 | ExcitSpins.push_back(9.0/2.0); |
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99 | ExcitLifetimes.push_back(17.0e-3*picosecond); |
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100 | |
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101 | ExcitEnergies.push_back(6348.0*keV); |
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102 | ExcitSpins.push_back(9.0/2.0); |
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103 | ExcitLifetimes.push_back(26e-3*picosecond); |
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104 | |
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105 | ExcitEnergies.push_back(7080.0*keV); |
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106 | ExcitSpins.push_back(3.0/2.0); |
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107 | ExcitLifetimes.push_back(0.24e-3*picosecond); |
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108 | |
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109 | ExcitEnergies.push_back(7132.0*keV); |
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110 | ExcitSpins.push_back(5.0/2.0); |
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111 | ExcitLifetimes.push_back(0.21e-3*picosecond); |
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112 | |
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113 | ExcitEnergies.push_back(7888.0*keV); |
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114 | ExcitSpins.push_back(5.0/2.0); |
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115 | ExcitLifetimes.push_back(0.17e-3*picosecond); |
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116 | |
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117 | ExcitEnergies.push_back(8663.0*keV); |
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118 | ExcitSpins.push_back(1.0/2.0); |
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119 | ExcitLifetimes.push_back(0.10e-3*picosecond); |
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120 | |
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121 | ExcitEnergies.push_back(8945.0*keV); |
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122 | ExcitSpins.push_back(7.0/2.0); |
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123 | ExcitLifetimes.push_back(21.0e-3*picosecond); |
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124 | |
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125 | ExcitEnergies.push_back(9209.6*keV); |
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126 | ExcitSpins.push_back(3.0/2.0); |
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127 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.11*keV)); |
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128 | |
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129 | ExcitEnergies.push_back(9250.8*keV); |
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130 | ExcitSpins.push_back(1.0/2.0); |
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131 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.6*keV)); |
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132 | |
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133 | ExcitEnergies.push_back(9395.4*keV); |
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134 | ExcitSpins.push_back(5.0/2.0); |
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135 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.03*keV)); |
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136 | |
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137 | ExcitEnergies.push_back(9404.4*keV); |
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138 | ExcitSpins.push_back(1.0/2.0); |
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139 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(65.0*keV)); |
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140 | |
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141 | ExcitEnergies.push_back(9425.6*keV); |
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142 | ExcitSpins.push_back(3.0/2.0); |
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143 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.6*keV)); |
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144 | |
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145 | ExcitEnergies.push_back(9485.9*keV); |
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146 | ExcitSpins.push_back(3.0/2.0); |
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147 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.22*keV)); |
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148 | |
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149 | ExcitEnergies.push_back(9606.6*keV); |
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150 | ExcitSpins.push_back(3.0/2.0); |
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151 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(6.0*keV)); |
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152 | |
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153 | ExcitEnergies.push_back(9650.0*keV); |
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154 | ExcitSpins.push_back(5.0/2.0); |
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155 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.1*keV)); |
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156 | |
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157 | ExcitEnergies.push_back(9653.7*keV); |
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158 | ExcitSpins.push_back(1.0/2.0); |
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159 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(105.0*keV)); |
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160 | |
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161 | ExcitEnergies.push_back(9679.5*keV); |
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162 | ExcitSpins.push_back(3.0/2.0); |
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163 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.6*keV)); |
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164 | |
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165 | ExcitEnergies.push_back(9698.9*keV); |
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166 | ExcitSpins.push_back(3.0/2.0); |
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167 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(29.0*keV)); |
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168 | |
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169 | ExcitEnergies.push_back(9730.8*keV); |
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170 | ExcitSpins.push_back(7.0/2.0); |
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171 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.35*keV)); |
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172 | |
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173 | ExcitEnergies.push_back(9753.5*keV); |
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174 | ExcitSpins.push_back(3.0/2.0); |
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175 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4.0*keV)); |
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176 | |
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177 | ExcitEnergies.push_back(9813.8*keV); |
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178 | ExcitSpins.push_back(5.0/2.0); |
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179 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.0*keV)); |
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180 | |
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181 | ExcitEnergies.push_back(9833.4*keV); |
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182 | ExcitSpins.push_back(3.0/2.0); |
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183 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(47.0*keV)); |
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184 | |
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185 | ExcitEnergies.push_back(9849.1*keV); |
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186 | ExcitSpins.push_back(1.0/2.0); |
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187 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(150.0*keV)); |
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188 | |
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189 | ExcitEnergies.push_back(9998.0*keV); |
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190 | ExcitSpins.push_back(1.0/2.0); |
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191 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(475.0*keV)); |
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192 | |
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193 | ExcitEnergies.push_back(10014.0*keV); |
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194 | ExcitSpins.push_back(5.0/2.0); |
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195 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(69.0*keV)); |
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196 | |
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197 | ExcitEnergies.push_back(10083.0*keV); |
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198 | ExcitSpins.push_back(1.0/2.0); |
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199 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1270.0*keV)); |
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200 | |
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201 | ExcitEnergies.push_back(10110.0*keV); |
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202 | ExcitSpins.push_back(1.0/2.0); |
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203 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4200.0*keV)); |
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204 | |
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205 | ExcitEnergies.push_back(10167.0*keV); |
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206 | ExcitSpins.push_back(5.0/2.0); |
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207 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(65.0*keV)); |
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208 | |
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209 | ExcitEnergies.push_back(10229.0*keV); |
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210 | ExcitSpins.push_back(3.0/2.0); |
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211 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5.0*keV)); |
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212 | |
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213 | ExcitEnergies.push_back(10239.0*keV); |
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214 | ExcitSpins.push_back(1.0/2.0); |
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215 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2450.0*keV)); |
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216 | |
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217 | ExcitEnergies.push_back(10313.0*keV); |
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218 | ExcitSpins.push_back(3.0/2.0); |
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219 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2000.0*keV)); |
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220 | |
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221 | ExcitEnergies.push_back(10334.0*keV); |
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222 | ExcitSpins.push_back(1.0/2.0); |
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223 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(190.0*keV)); |
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224 | |
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225 | ExcitEnergies.push_back(10341.0*keV); |
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226 | ExcitSpins.push_back(5.0/2.0); |
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227 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(11.0*keV)); |
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228 | |
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229 | ExcitEnergies.push_back(10348.0*keV); |
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230 | ExcitSpins.push_back(3.0/2.0); |
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231 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(210.0*keV)); |
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232 | |
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233 | ExcitEnergies.push_back(10436.0*keV); |
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234 | ExcitSpins.push_back(5.0/2.0); |
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235 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(25.0*keV)); |
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236 | |
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237 | ExcitEnergies.push_back(10476.0*keV); |
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238 | ExcitSpins.push_back(3.0/2.0); |
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239 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(470.0*keV)); |
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240 | |
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241 | ExcitEnergies.push_back(10499.0*keV); |
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242 | ExcitSpins.push_back(3.0/2.0); |
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243 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(920.0*keV)); |
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244 | |
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245 | ExcitEnergies.push_back(10505.0*keV); |
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246 | ExcitSpins.push_back(1.0/2.0); |
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247 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(560.0*keV)); |
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248 | |
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249 | ExcitEnergies.push_back(10516.0*keV); |
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250 | ExcitSpins.push_back(5.0/2.0); |
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251 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV)); |
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252 | |
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253 | ExcitEnergies.push_back(10546.0*keV); |
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254 | ExcitSpins.push_back(5.0/2.0); |
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255 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(540.0*keV)); |
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256 | |
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257 | ExcitEnergies.push_back(10570.0*keV); |
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258 | ExcitSpins.push_back(3.0/2.0); |
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259 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1100.0*keV)); |
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260 | |
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261 | ExcitEnergies.push_back(10615.0*keV); |
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262 | ExcitSpins.push_back(5.0/2.0); |
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263 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(425.0*keV)); |
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264 | |
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265 | ExcitEnergies.push_back(10673.0*keV); |
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266 | ExcitSpins.push_back(3.0/2.0); |
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267 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(23000.0*keV)); |
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268 | |
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269 | ExcitEnergies.push_back(10702.0*keV); |
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270 | ExcitSpins.push_back(3.0/2.0); |
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271 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400.0*keV)); |
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272 | |
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273 | ExcitEnergies.push_back(10769.0*keV); |
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274 | ExcitSpins.push_back(3.0/2.0); |
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275 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5.0*keV)); |
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276 | |
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277 | ExcitEnergies.push_back(10822.0*keV); |
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278 | ExcitSpins.push_back(3.0/2.0); |
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279 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1700.0*keV)); |
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280 | |
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281 | ExcitEnergies.push_back(10823.0*keV); |
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282 | ExcitSpins.push_back(3.0/2.0); |
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283 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(26000.0*keV)); |
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284 | |
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285 | ExcitEnergies.push_back(10837.0*keV); |
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286 | ExcitSpins.push_back(5.0/2.0); |
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287 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV)); |
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288 | |
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289 | ExcitEnergies.push_back(10869.0*keV); |
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290 | ExcitSpins.push_back(3.0/2.0); |
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291 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(21000.0*keV)); |
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292 | |
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293 | ExcitEnergies.push_back(10904.0*keV); |
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294 | ExcitSpins.push_back(1.0/2.0); |
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295 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(53.0*keV)); |
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296 | |
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297 | ExcitEnergies.push_back(10907.0*keV); |
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298 | ExcitSpins.push_back(1.0/2.0); |
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299 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2850.0*keV)); |
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300 | |
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301 | ExcitEnergies.push_back(10908.0*keV); |
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302 | ExcitSpins.push_back(5.0/2.0); |
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303 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(900.0*keV)); |
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304 | |
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305 | ExcitEnergies.push_back(10917.0*keV); |
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306 | ExcitSpins.push_back(1.0/2.0); |
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307 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(55.0*keV)); |
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308 | |
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309 | ExcitEnergies.push_back(10931.0*keV); |
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310 | ExcitSpins.push_back(3.0/2.0); |
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311 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3500.0*keV)); |
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312 | |
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313 | ExcitEnergies.push_back(10949.0*keV); |
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314 | ExcitSpins.push_back(1.0/2.0); |
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315 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5200.0*keV)); |
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316 | |
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317 | ExcitEnergies.push_back(10954.0*keV); |
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318 | ExcitSpins.push_back(7.0/2.0); |
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319 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(65.0*keV)); |
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320 | |
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321 | ExcitEnergies.push_back(10972.0*keV); |
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322 | ExcitSpins.push_back(5.0/2.0); |
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323 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400.0*keV)); |
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324 | |
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325 | ExcitEnergies.push_back(10975.0*keV); |
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326 | ExcitSpins.push_back(3.0/2.0); |
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327 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(18.0*keV)); |
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328 | |
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329 | ExcitEnergies.push_back(10979.0*keV); |
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330 | ExcitSpins.push_back(3.0/2.0); |
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331 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(6000.0*keV)); |
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332 | |
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333 | ExcitEnergies.push_back(10993.0*keV); |
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334 | ExcitSpins.push_back(1.0/2.0); |
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335 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20600.0*keV)); |
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336 | |
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337 | ExcitEnergies.push_back(10994.0*keV); |
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338 | ExcitSpins.push_back(3.0/2.0); |
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339 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(60.0*keV)); |
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340 | |
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341 | ExcitEnergies.push_back(11039.0*keV); |
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342 | ExcitSpins.push_back(1.0/2.0); |
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343 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500.0*keV)); |
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344 | |
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345 | ExcitEnergies.push_back(11087.0*keV); |
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346 | ExcitSpins.push_back(3.0/2.0); |
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347 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800.0*keV)); |
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348 | |
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349 | ExcitEnergies.push_back(11109.0*keV); |
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350 | ExcitSpins.push_back(5.0/2.0); |
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351 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(135.0*keV)); |
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352 | |
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353 | ExcitEnergies.push_back(11110.0*keV); |
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354 | ExcitSpins.push_back(3.0/2.0); |
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355 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4100.0*keV)); |
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356 | |
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357 | } |
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358 | |
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359 | |
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360 | G4Na23GEMProbability::G4Na23GEMProbability(const G4Na23GEMProbability &) : G4GEMProbability() |
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361 | { |
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362 | throw G4HadronicException(__FILE__, __LINE__, "G4Na23GEMProbability::copy_constructor meant to not be accessable"); |
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363 | } |
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364 | |
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365 | |
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366 | |
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367 | |
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368 | const G4Na23GEMProbability & G4Na23GEMProbability:: |
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369 | operator=(const G4Na23GEMProbability &) |
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370 | { |
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371 | throw G4HadronicException(__FILE__, __LINE__, "G4Na23GEMProbability::operator= meant to not be accessable"); |
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372 | return *this; |
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373 | } |
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374 | |
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375 | |
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376 | G4bool G4Na23GEMProbability::operator==(const G4Na23GEMProbability &) const |
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377 | { |
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378 | return false; |
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379 | } |
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380 | |
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381 | G4bool G4Na23GEMProbability::operator!=(const G4Na23GEMProbability &) const |
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382 | { |
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383 | return true; |
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384 | } |
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385 | |
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386 | |
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387 | |
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