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: G4Be9GEMProbability.cc,v 1.5 2006/06/29 20:21:33 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 "G4Be9GEMProbability.hh" |
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36 | |
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37 | G4Be9GEMProbability::G4Be9GEMProbability() : |
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38 | G4GEMProbability(9,4,3.0/2.0) // A,Z,Spin |
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39 | { |
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40 | ExcitEnergies.push_back(1685.0*keV); |
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41 | ExcitSpins.push_back(1.0/2.0); |
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42 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(150.0*keV)); |
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43 | |
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44 | ExcitEnergies.push_back(2429.4*keV); |
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45 | ExcitSpins.push_back(5.0/2.0); |
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46 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.77*keV)); |
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47 | |
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48 | ExcitEnergies.push_back(2.78e3*keV); |
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49 | ExcitSpins.push_back(1.0/2.0); |
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50 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1080.0*keV)); |
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51 | |
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52 | ExcitEnergies.push_back(3049.0*keV); |
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53 | ExcitSpins.push_back(5.0/2.0); |
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54 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(282.0*keV)); |
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55 | |
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56 | ExcitEnergies.push_back(4704.0*keV); |
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57 | ExcitSpins.push_back(3.0/2.0); |
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58 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(743.0*keV)); |
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59 | |
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60 | ExcitEnergies.push_back(6760.0*keV); |
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61 | ExcitSpins.push_back(7.0/2.0); |
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62 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1540.0*keV)); |
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63 | |
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64 | ExcitEnergies.push_back(7940.0*keV); |
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65 | ExcitSpins.push_back(1.0/2.0); |
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66 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV)); |
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67 | |
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68 | ExcitEnergies.push_back(11283.0*keV); |
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69 | ExcitSpins.push_back(3.0/2.0); |
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70 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(575.0*keV)); |
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71 | |
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72 | ExcitEnergies.push_back(11810.0*keV); |
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73 | ExcitSpins.push_back(0.0); |
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74 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400.0*keV)); |
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75 | |
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76 | ExcitEnergies.push_back(13790.0*keV); |
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77 | ExcitSpins.push_back(0.0); |
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78 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(590.0*keV)); |
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79 | |
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80 | ExcitEnergies.push_back(14392.9*keV); |
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81 | ExcitSpins.push_back(3.0/2.0); |
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82 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.381*keV)); |
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83 | |
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84 | ExcitEnergies.push_back(14.4e3*keV); |
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85 | ExcitSpins.push_back(0.0); |
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86 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800*keV)); |
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87 | |
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88 | ExcitEnergies.push_back(15970.0*keV); |
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89 | ExcitSpins.push_back(0.0); |
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90 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV)); |
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91 | |
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92 | ExcitEnergies.push_back(16671.0*keV); |
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93 | ExcitSpins.push_back(0.0); |
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94 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(41.0*keV)); |
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95 | |
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96 | ExcitEnergies.push_back(16975.0*keV); |
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97 | ExcitSpins.push_back(1.0/2.0); |
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98 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.47*keV)); |
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99 | |
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100 | ExcitEnergies.push_back(17298.0*keV); |
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101 | ExcitSpins.push_back(5.0/2.0); |
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102 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200.0*keV)); |
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103 | |
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104 | ExcitEnergies.push_back(17493.0*keV); |
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105 | ExcitSpins.push_back(7.0/2.0); |
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106 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(47.0*keV)); |
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107 | |
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108 | ExcitEnergies.push_back(19200.0*keV); |
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109 | ExcitSpins.push_back(0.0); |
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110 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(310.0*keV)); |
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111 | |
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112 | ExcitEnergies.push_back(20740.0*keV); |
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113 | ExcitSpins.push_back(0.0); |
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114 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV)); |
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115 | |
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116 | SetExcitationEnergiesPtr(&ExcitEnergies); |
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117 | SetExcitationSpinsPtr(&ExcitSpins); |
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118 | SetExcitationLifetimesPtr(&ExcitLifetimes); |
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119 | } |
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120 | |
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121 | |
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122 | G4Be9GEMProbability::G4Be9GEMProbability(const G4Be9GEMProbability &) : G4GEMProbability() |
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123 | { |
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124 | throw G4HadronicException(__FILE__, __LINE__, "G4Be9GEMProbability::copy_constructor meant to not be accessable"); |
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125 | } |
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126 | |
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127 | |
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128 | |
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129 | |
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130 | const G4Be9GEMProbability & G4Be9GEMProbability:: |
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131 | operator=(const G4Be9GEMProbability &) |
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132 | { |
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133 | throw G4HadronicException(__FILE__, __LINE__, "G4Be9GEMProbability::operator= meant to not be accessable"); |
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134 | return *this; |
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135 | } |
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136 | |
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137 | |
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138 | G4bool G4Be9GEMProbability::operator==(const G4Be9GEMProbability &) const |
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139 | { |
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140 | return false; |
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141 | } |
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142 | |
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143 | G4bool G4Be9GEMProbability::operator!=(const G4Be9GEMProbability &) const |
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144 | { |
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145 | return true; |
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146 | } |
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147 | |
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148 | |
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149 | |
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