[819] | 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 1.5 2006/06/29 20:22:59 gunter Exp $ |
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[1007] | 28 | // GEANT4 tag $Name: geant4-09-02 $ |
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[819] | 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 | |
---|
| 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 | |
---|
| 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 | |
---|
| 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 | |
---|
| 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 | |
---|
| 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 | |
---|
| 309 | ExcitEnergies.push_back(10931.0*keV); |
---|
| 310 | ExcitSpins.push_back(3.0/2.0); |
---|
| 311 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3500.0*keV)); |
---|
| 312 | |
---|
| 313 | ExcitEnergies.push_back(10949.0*keV); |
---|
| 314 | ExcitSpins.push_back(1.0/2.0); |
---|
| 315 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5200.0*keV)); |
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| 316 | |
---|
| 317 | ExcitEnergies.push_back(10954.0*keV); |
---|
| 318 | ExcitSpins.push_back(7.0/2.0); |
---|
| 319 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(65.0*keV)); |
---|
| 320 | |
---|
| 321 | ExcitEnergies.push_back(10972.0*keV); |
---|
| 322 | ExcitSpins.push_back(5.0/2.0); |
---|
| 323 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400.0*keV)); |
---|
| 324 | |
---|
| 325 | ExcitEnergies.push_back(10975.0*keV); |
---|
| 326 | ExcitSpins.push_back(3.0/2.0); |
---|
| 327 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(18.0*keV)); |
---|
| 328 | |
---|
| 329 | ExcitEnergies.push_back(10979.0*keV); |
---|
| 330 | ExcitSpins.push_back(3.0/2.0); |
---|
| 331 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(6000.0*keV)); |
---|
| 332 | |
---|
| 333 | ExcitEnergies.push_back(10993.0*keV); |
---|
| 334 | ExcitSpins.push_back(1.0/2.0); |
---|
| 335 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20600.0*keV)); |
---|
| 336 | |
---|
| 337 | ExcitEnergies.push_back(10994.0*keV); |
---|
| 338 | ExcitSpins.push_back(3.0/2.0); |
---|
| 339 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(60.0*keV)); |
---|
| 340 | |
---|
| 341 | ExcitEnergies.push_back(11039.0*keV); |
---|
| 342 | ExcitSpins.push_back(1.0/2.0); |
---|
| 343 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500.0*keV)); |
---|
| 344 | |
---|
| 345 | ExcitEnergies.push_back(11087.0*keV); |
---|
| 346 | ExcitSpins.push_back(3.0/2.0); |
---|
| 347 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800.0*keV)); |
---|
| 348 | |
---|
| 349 | ExcitEnergies.push_back(11109.0*keV); |
---|
| 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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