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: G4N16GEMProbability.cc,v 1.5 2006/06/29 20:22:51 gunter Exp $ |
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28 | // GEANT4 tag $Name: geant4-09-02-ref-02 $ |
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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 "G4N16GEMProbability.hh" |
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36 | |
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37 | G4N16GEMProbability::G4N16GEMProbability() : |
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38 | G4GEMProbability(16,7,2.0) // A,Z,Spin |
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39 | { |
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40 | ExcitEnergies.push_back(120.1*keV); |
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41 | ExcitSpins.push_back(0.0); |
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42 | ExcitLifetimes.push_back(5.25e-6*s); |
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43 | |
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44 | ExcitEnergies.push_back(397.5*keV); |
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45 | ExcitSpins.push_back(1.0); |
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46 | ExcitLifetimes.push_back(4.5e-12*s); |
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47 | |
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48 | ExcitEnergies.push_back( 3355*keV); |
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49 | ExcitSpins.push_back(1.0); |
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50 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(15*keV)); |
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51 | |
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52 | ExcitEnergies.push_back( 3519*keV); |
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53 | ExcitSpins.push_back(2.0); |
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54 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3*keV)); |
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55 | |
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56 | ExcitEnergies.push_back( 3960*keV); |
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57 | ExcitSpins.push_back(3.0); |
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58 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2*keV)); |
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59 | |
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60 | ExcitEnergies.push_back( 4319*keV); |
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61 | ExcitSpins.push_back(1.0); |
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62 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20*keV)); |
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63 | |
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64 | ExcitEnergies.push_back( 4387*keV); |
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65 | ExcitSpins.push_back(1.0); |
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66 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(82*keV)); |
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67 | |
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68 | ExcitEnergies.push_back( 4760*keV); |
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69 | ExcitSpins.push_back(1.0); |
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70 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(250*keV)); |
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71 | |
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72 | ExcitEnergies.push_back( 4776*keV); |
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73 | ExcitSpins.push_back(2.0); |
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74 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(59*keV)); |
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75 | |
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76 | ExcitEnergies.push_back( 5050*keV); |
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77 | ExcitSpins.push_back(2.0); |
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78 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(19*keV)); |
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79 | |
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80 | ExcitEnergies.push_back( 5130*keV); |
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81 | ExcitSpins.push_back(2.0); |
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82 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7*keV)); |
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83 | |
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84 | ExcitEnergies.push_back( 5150*keV); |
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85 | ExcitSpins.push_back(3.0); |
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86 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7*keV)); |
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87 | |
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88 | ExcitEnergies.push_back( 5232*keV); |
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89 | ExcitSpins.push_back(3.0); |
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90 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4*keV)); |
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91 | |
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92 | ExcitEnergies.push_back( 5240*keV); |
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93 | ExcitSpins.push_back(1.0); |
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94 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(260*keV)); |
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95 | |
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96 | ExcitEnergies.push_back( 5250*keV); |
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97 | ExcitSpins.push_back(2.0); |
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98 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(320*keV)); |
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99 | |
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100 | ExcitEnergies.push_back( 5518*keV); |
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101 | ExcitSpins.push_back(3.0); |
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102 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7*keV)); |
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103 | |
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104 | ExcitEnergies.push_back( 5730*keV); |
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105 | ExcitSpins.push_back(5.0); |
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106 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7*keV)); |
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107 | |
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108 | ExcitEnergies.push_back( 6009*keV); |
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109 | ExcitSpins.push_back(1.0); |
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110 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(270*keV)); |
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111 | |
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112 | ExcitEnergies.push_back( 6168*keV); |
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113 | ExcitSpins.push_back(4.0); |
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114 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7*keV)); |
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115 | |
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116 | ExcitEnergies.push_back( 6373*keV); |
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117 | ExcitSpins.push_back(3.0); |
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118 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30*keV)); |
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119 | |
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120 | ExcitEnergies.push_back( 6513*keV); |
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121 | ExcitSpins.push_back(2.0); |
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122 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(34*keV)); |
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123 | |
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124 | ExcitEnergies.push_back( 6840*keV); |
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125 | ExcitSpins.push_back(2.0); |
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126 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(140*keV)); |
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127 | |
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128 | ExcitEnergies.push_back( 7020*keV); |
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129 | ExcitSpins.push_back(1.0); |
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130 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(22*keV)); |
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131 | |
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132 | ExcitEnergies.push_back( 7250*keV); |
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133 | ExcitSpins.push_back(2.0); |
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134 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(17*keV)); |
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135 | |
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136 | ExcitEnergies.push_back( 7573*keV); |
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137 | ExcitSpins.push_back(3.0); |
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138 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7*keV)); |
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139 | |
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140 | ExcitEnergies.push_back( 7877*keV); |
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141 | ExcitSpins.push_back(4.0); |
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142 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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143 | |
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144 | ExcitEnergies.push_back( 8365*keV); |
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145 | ExcitSpins.push_back(1.0); |
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146 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(18*keV)); |
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147 | |
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148 | ExcitEnergies.push_back( 8490*keV); |
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149 | ExcitSpins.push_back(1.0); |
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150 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(50*keV)); |
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151 | |
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152 | ExcitEnergies.push_back( 8720*keV); |
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153 | ExcitSpins.push_back(1.0); |
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154 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40*keV)); |
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155 | |
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156 | ExcitEnergies.push_back( 9160*keV); |
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157 | ExcitSpins.push_back(2.0); |
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158 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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159 | |
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160 | ExcitEnergies.push_back( 9459*keV); |
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161 | ExcitSpins.push_back(2.0); |
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162 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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163 | |
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164 | ExcitEnergies.push_back( 9928*keV); |
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165 | ExcitSpins.push_back(0.0); |
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166 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(12*keV)); |
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167 | |
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168 | ExcitEnergies.push_back(10055*keV); |
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169 | ExcitSpins.push_back(3.0); |
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170 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30*keV)); |
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171 | |
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172 | ExcitEnergies.push_back(10270*keV); |
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173 | ExcitSpins.push_back(2.0); |
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174 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(165*keV)); |
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175 | |
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176 | ExcitEnergies.push_back(10710*keV); |
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177 | ExcitSpins.push_back(2.0); |
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178 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(120*keV)); |
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179 | |
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180 | ExcitEnergies.push_back(11620*keV); |
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181 | ExcitSpins.push_back(3.0); |
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182 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(220*keV)); |
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183 | |
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184 | ExcitEnergies.push_back(11701*keV); |
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185 | ExcitSpins.push_back(2.0); |
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186 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(12*keV)); |
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187 | |
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188 | ExcitEnergies.push_back(14410*keV); |
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189 | ExcitSpins.push_back(3.0); |
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190 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(180*keV)); |
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191 | |
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192 | SetExcitationEnergiesPtr(&ExcitEnergies); |
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193 | SetExcitationSpinsPtr(&ExcitSpins); |
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194 | SetExcitationLifetimesPtr(&ExcitLifetimes); |
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195 | } |
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196 | |
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197 | |
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198 | G4N16GEMProbability::G4N16GEMProbability(const G4N16GEMProbability &) : G4GEMProbability() |
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199 | { |
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200 | throw G4HadronicException(__FILE__, __LINE__, "G4N16GEMProbability::copy_constructor meant to not be accessable"); |
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201 | } |
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202 | |
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203 | |
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204 | |
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205 | |
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206 | const G4N16GEMProbability & G4N16GEMProbability:: |
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207 | operator=(const G4N16GEMProbability &) |
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208 | { |
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209 | throw G4HadronicException(__FILE__, __LINE__, "G4N16GEMProbability::operator= meant to not be accessable"); |
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210 | return *this; |
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211 | } |
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212 | |
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213 | |
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214 | G4bool G4N16GEMProbability::operator==(const G4N16GEMProbability &) const |
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215 | { |
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216 | return false; |
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217 | } |
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218 | |
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219 | G4bool G4N16GEMProbability::operator!=(const G4N16GEMProbability &) const |
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220 | { |
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221 | return true; |
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222 | } |
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223 | |
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224 | |
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225 | |
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