| 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: G4Mg23GEMProbability.cc,v 1.5 2009/09/15 12:54:17 vnivanch Exp $ |
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| 28 | // GEANT4 tag $Name: geant4-09-04-beta-01 $ |
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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 "G4Mg23GEMProbability.hh" |
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| 36 | |
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| 37 | G4Mg23GEMProbability::G4Mg23GEMProbability() : |
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| 38 | G4GEMProbability(23,12,3.0/2.0) // A,Z,Spin |
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| 39 | { |
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| 40 | |
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| 41 | ExcitEnergies.push_back(450.70*keV); |
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| 42 | ExcitSpins.push_back(5.0/2.0); |
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| 43 | ExcitLifetimes.push_back(1.25*picosecond); |
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| 44 | |
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| 45 | ExcitEnergies.push_back(2051.0*keV); |
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| 46 | ExcitSpins.push_back(7.0/2.0); |
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| 47 | ExcitLifetimes.push_back(55.0e-3*picosecond); |
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| 48 | |
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| 49 | ExcitEnergies.push_back(2359.0*keV); |
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| 50 | ExcitSpins.push_back(1.0/2.0); |
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| 51 | ExcitLifetimes.push_back(575.0e-3*picosecond); |
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| 52 | |
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| 53 | ExcitEnergies.push_back(2715.0*keV); |
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| 54 | ExcitSpins.push_back(9.0/2.0); |
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| 55 | ExcitLifetimes.push_back(97.0e-3*picosecond); |
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| 56 | |
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| 57 | ExcitEnergies.push_back(2771.0*keV); |
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| 58 | ExcitSpins.push_back(1.0/2.0); |
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| 59 | ExcitLifetimes.push_back(107.0e-3*picosecond); |
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| 60 | |
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| 61 | ExcitEnergies.push_back(2908.0*keV); |
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| 62 | ExcitSpins.push_back(3.0/2.0); |
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| 63 | ExcitLifetimes.push_back(17.0e-3*picosecond); |
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| 64 | |
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| 65 | ExcitEnergies.push_back(3795.0*keV); |
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| 66 | ExcitSpins.push_back(3.0/2.0); |
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| 67 | ExcitLifetimes.push_back(14.0*nanosecond); |
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| 68 | |
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| 69 | ExcitEnergies.push_back(4356.0*keV); |
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| 70 | ExcitSpins.push_back(1.0/2.0); |
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| 71 | ExcitLifetimes.push_back(14.0*nanosecond); |
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| 72 | |
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| 73 | } |
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| 74 | |
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| 75 | |
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| 76 | G4Mg23GEMProbability::G4Mg23GEMProbability(const G4Mg23GEMProbability &) : G4GEMProbability() |
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| 77 | { |
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| 78 | throw G4HadronicException(__FILE__, __LINE__, "G4Mg23GEMProbability::copy_constructor meant to not be accessable"); |
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| 79 | } |
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| 80 | |
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| 81 | |
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| 82 | |
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| 83 | |
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| 84 | const G4Mg23GEMProbability & G4Mg23GEMProbability:: |
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| 85 | operator=(const G4Mg23GEMProbability &) |
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| 86 | { |
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| 87 | throw G4HadronicException(__FILE__, __LINE__, "G4Mg23GEMProbability::operator= meant to not be accessable"); |
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| 88 | return *this; |
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| 89 | } |
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| 90 | |
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| 91 | |
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| 92 | G4bool G4Mg23GEMProbability::operator==(const G4Mg23GEMProbability &) const |
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| 93 | { |
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| 94 | return false; |
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| 95 | } |
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| 96 | |
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| 97 | G4bool G4Mg23GEMProbability::operator!=(const G4Mg23GEMProbability &) const |
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| 98 | { |
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| 99 | return true; |
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| 100 | } |
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| 101 | |
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| 102 | |
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| 103 | |
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