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: G4C12GEMProbability.cc,v 1.6 2009/09/15 12:54:16 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 "G4C12GEMProbability.hh" |
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36 | |
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37 | G4C12GEMProbability::G4C12GEMProbability() : |
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38 | G4GEMProbability(12,6,0.0) // A,Z,Spin |
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39 | { |
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40 | |
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41 | ExcitEnergies.push_back(4438.91*keV); |
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42 | ExcitSpins.push_back(2.0); |
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43 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(10.8e-3*eV)); |
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44 | |
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45 | ExcitEnergies.push_back(7654.2*keV); |
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46 | ExcitSpins.push_back(0.0); |
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47 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(8.5*keV)); |
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48 | |
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49 | ExcitEnergies.push_back(9641*keV); |
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50 | ExcitSpins.push_back(3.0); |
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51 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(34*keV)); |
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52 | |
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53 | ExcitEnergies.push_back(1.03E+4*keV); |
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54 | ExcitSpins.push_back(0.0); |
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55 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.0e3*keV)); |
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56 | |
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57 | ExcitEnergies.push_back(10844*keV); |
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58 | ExcitSpins.push_back(1.0); |
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59 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(315*keV)); |
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60 | |
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61 | ExcitEnergies.push_back(1.116E+4*keV); |
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62 | ExcitSpins.push_back(2.0); |
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63 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(430*keV)); |
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64 | |
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65 | ExcitEnergies.push_back(1.1828E+4*keV); |
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66 | ExcitSpins.push_back(2.0); |
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67 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(260*keV)); |
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68 | |
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69 | ExcitEnergies.push_back(12710*keV); |
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70 | ExcitSpins.push_back(1.0); |
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71 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(18.1*eV)); |
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72 | |
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73 | ExcitEnergies.push_back(13352*keV); |
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74 | ExcitSpins.push_back(2.0); |
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75 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(375*keV)); |
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76 | |
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77 | ExcitEnergies.push_back(14083*keV); |
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78 | ExcitSpins.push_back(4.0); |
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79 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(258*keV)); |
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80 | |
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81 | ExcitEnergies.push_back(15110*keV); |
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82 | ExcitSpins.push_back(1.0); |
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83 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(42*eV)); |
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84 | |
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85 | ExcitEnergies.push_back(16106.7*keV); |
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86 | ExcitSpins.push_back(2.0); |
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87 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5.2*keV)); |
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88 | |
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89 | ExcitEnergies.push_back(16.57E+3*keV); |
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90 | ExcitSpins.push_back(2.0); |
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91 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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92 | |
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93 | ExcitEnergies.push_back(17.23E+3*keV); |
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94 | ExcitSpins.push_back(1.0); |
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95 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1150*keV)); |
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96 | |
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97 | ExcitEnergies.push_back(17.76E+3*keV); |
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98 | ExcitSpins.push_back(0.0); |
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99 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(80*keV)); |
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100 | |
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101 | ExcitEnergies.push_back(18.13E+3*keV); |
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102 | ExcitSpins.push_back(1.0); |
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103 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600*keV)); |
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104 | |
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105 | ExcitEnergies.push_back(18.27E+3*keV); |
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106 | ExcitSpins.push_back(4.0); |
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107 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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108 | |
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109 | ExcitEnergies.push_back(18.38E+3*keV); |
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110 | ExcitSpins.push_back(3.0); |
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111 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(220*keV)); |
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112 | |
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113 | ExcitEnergies.push_back(18.39E+3*keV); |
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114 | ExcitSpins.push_back(2.0); |
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115 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(43*keV)); |
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116 | |
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117 | ExcitEnergies.push_back(18.6E+3*keV); |
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118 | ExcitSpins.push_back(3.0); |
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119 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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120 | |
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121 | ExcitEnergies.push_back(18.80E+3*keV); |
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122 | ExcitSpins.push_back(2.0); |
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123 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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124 | |
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125 | ExcitEnergies.push_back(19.2E+3*keV); |
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126 | ExcitSpins.push_back(1.0); |
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127 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1100*keV)); |
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128 | |
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129 | ExcitEnergies.push_back(19.39E+3*keV); |
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130 | ExcitSpins.push_back(2.0); |
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131 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800*keV)); |
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132 | |
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133 | ExcitEnergies.push_back(19.55E+3*keV); |
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134 | ExcitSpins.push_back(4.0); |
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135 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(490*keV)); |
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136 | |
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137 | ExcitEnergies.push_back(19.69E+3*keV); |
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138 | ExcitSpins.push_back(1.0); |
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139 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(230*keV)); |
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140 | |
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141 | ExcitEnergies.push_back(20.0E+3*keV); |
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142 | ExcitSpins.push_back(2.0); |
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143 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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144 | |
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145 | ExcitEnergies.push_back(20.27E+3*keV); |
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146 | ExcitSpins.push_back(1.0); |
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147 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(140*keV)); |
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148 | |
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149 | ExcitEnergies.push_back(20.5E+3*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)/(180*keV)); |
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152 | |
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153 | ExcitEnergies.push_back(20.62E+3*keV); |
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154 | ExcitSpins.push_back(3.0); |
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155 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200*keV)); |
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156 | |
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157 | ExcitEnergies.push_back(21.60E+3*keV); |
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158 | ExcitSpins.push_back(2.0); |
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159 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1200*keV)); |
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160 | |
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161 | ExcitEnergies.push_back(22.0E+3*keV); |
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162 | ExcitSpins.push_back(1.0); |
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163 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800*keV)); |
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164 | |
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165 | ExcitEnergies.push_back(22.40E+3*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)/(275*keV)); |
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168 | |
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169 | ExcitEnergies.push_back(22.65E+3*keV); |
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170 | ExcitSpins.push_back(1.0); |
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171 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3200*keV)); |
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172 | |
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173 | ExcitEnergies.push_back(23.04E+3 *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)/(60*keV)); |
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176 | |
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177 | ExcitEnergies.push_back(23.52E+3*keV); |
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178 | ExcitSpins.push_back(1.0); |
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179 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(230*keV)); |
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180 | |
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181 | ExcitEnergies.push_back(23.92E+3*keV); |
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182 | ExcitSpins.push_back(1.0); |
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183 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400*keV)); |
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184 | |
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185 | ExcitEnergies.push_back(25.30E+3*keV); |
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186 | ExcitSpins.push_back(1.0); |
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187 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(510*keV)); |
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188 | |
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189 | ExcitEnergies.push_back(25.4E+3*keV); |
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190 | ExcitSpins.push_back(1.0); |
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191 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2000*keV)); |
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192 | |
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193 | ExcitEnergies.push_back(27.0E+3*keV); |
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194 | ExcitSpins.push_back(1.0); |
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195 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1400*keV)); |
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196 | |
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197 | ExcitEnergies.push_back(27595.0*keV); |
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198 | ExcitSpins.push_back(0.0); |
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199 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30*keV)); |
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200 | |
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201 | ExcitEnergies.push_back(28.2E+3*keV); |
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202 | ExcitSpins.push_back(1.0); |
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203 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1600*keV)); |
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204 | |
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205 | SetExcitationEnergiesPtr(&ExcitEnergies); |
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206 | SetExcitationSpinsPtr(&ExcitSpins); |
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207 | SetExcitationLifetimesPtr(&ExcitLifetimes); |
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208 | } |
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209 | |
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210 | |
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211 | G4C12GEMProbability::G4C12GEMProbability(const G4C12GEMProbability &) : G4GEMProbability() |
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212 | { |
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213 | throw G4HadronicException(__FILE__, __LINE__, "G4C12GEMProbability::copy_constructor meant to not be accessable"); |
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214 | } |
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215 | |
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216 | |
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217 | |
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218 | |
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219 | const G4C12GEMProbability & G4C12GEMProbability:: |
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220 | operator=(const G4C12GEMProbability &) |
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221 | { |
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222 | throw G4HadronicException(__FILE__, __LINE__, "G4C12GEMProbability::operator= meant to not be accessable"); |
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223 | return *this; |
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224 | } |
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225 | |
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226 | |
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227 | G4bool G4C12GEMProbability::operator==(const G4C12GEMProbability &) const |
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228 | { |
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229 | return false; |
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230 | } |
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231 | |
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232 | G4bool G4C12GEMProbability::operator!=(const G4C12GEMProbability &) const |
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233 | { |
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234 | return true; |
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235 | } |
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236 | |
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237 | |
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238 | |
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