// // ******************************************************************** // * License and Disclaimer * // * * // * The Geant4 software is copyright of the Copyright Holders of * // * the Geant4 Collaboration. It is provided under the terms and * // * conditions of the Geant4 Software License, included in the file * // * LICENSE and available at http://cern.ch/geant4/license . These * // * include a list of copyright holders. * // * * // * Neither the authors of this software system, nor their employing * // * institutes,nor the agencies providing financial support for this * // * work make any representation or warranty, express or implied, * // * regarding this software system or assume any liability for its * // * use. Please see the license in the file LICENSE and URL above * // * for the full disclaimer and the limitation of liability. * // * * // * This code implementation is the result of the scientific and * // * technical work of the GEANT4 collaboration. * // * By using, copying, modifying or distributing the software (or * // * any work based on the software) you agree to acknowledge its * // * use in resulting scientific publications, and indicate your * // * acceptance of all terms of the Geant4 Software license. * // ******************************************************************** // // // $Id: G4C13GEMProbability.cc,v 1.6 2009/09/15 12:54:16 vnivanch Exp $ // GEANT4 tag $Name: geant4-09-04-beta-01 $ // // Hadronic Process: Nuclear De-excitations // by V. Lara (Nov 1999) // #include "G4C13GEMProbability.hh" G4C13GEMProbability::G4C13GEMProbability() : G4GEMProbability(13,6,1.0/2.0) // A,Z,Spin { ExcitEnergies.push_back(3088.4*keV); ExcitSpins.push_back(1.0/2.0); ExcitLifetimes.push_back(1.04e-15*s); ExcitEnergies.push_back(3684.37*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(1.04e-15*s); ExcitEnergies.push_back( 3853.62*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(7.5e-12*s); ExcitEnergies.push_back(6864*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(6*keV)); ExcitEnergies.push_back(7492*keV); ExcitSpins.push_back(7.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5*keV)); ExcitEnergies.push_back(7547*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.2*keV)); ExcitEnergies.push_back(7677*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(70*keV)); ExcitEnergies.push_back(8.2E3*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000*keV)); ExcitEnergies.push_back(8860*keV); ExcitSpins.push_back(1.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(150*keV)); ExcitEnergies.push_back(9498*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5*keV)); ExcitEnergies.push_back(9897*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(26*keV)); ExcitEnergies.push_back(10753*keV); ExcitSpins.push_back(7.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(55*keV)); ExcitEnergies.push_back(10818*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(24*keV)); ExcitEnergies.push_back(10996*keV); ExcitSpins.push_back(1.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(37*keV)); ExcitEnergies.push_back(11080*keV); ExcitSpins.push_back(1.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4*keV)); ExcitEnergies.push_back(11851*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(68*keV)); ExcitEnergies.push_back(11970*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200*keV)); ExcitEnergies.push_back(12106*keV); ExcitSpins.push_back(9.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(81*keV)); ExcitEnergies.push_back(12400*keV); ExcitSpins.push_back(7.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(150*keV)); ExcitEnergies.push_back(13280*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(340*keV)); ExcitEnergies.push_back(13410*keV); ExcitSpins.push_back(9.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(35*keV)); ExcitEnergies.push_back(13560*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500*keV)); ExcitEnergies.push_back(13760*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); ExcitEnergies.push_back(14120*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200*keV)); ExcitEnergies.push_back(14.39E3*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(260*keV)); ExcitEnergies.push_back(14940*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(380*keV)); ExcitEnergies.push_back(15106*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5*keV)); ExcitEnergies.push_back(19500*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(450*keV)); SetExcitationEnergiesPtr(&ExcitEnergies); SetExcitationSpinsPtr(&ExcitSpins); SetExcitationLifetimesPtr(&ExcitLifetimes); } G4C13GEMProbability::G4C13GEMProbability(const G4C13GEMProbability &) : G4GEMProbability() { throw G4HadronicException(__FILE__, __LINE__, "G4C13GEMProbability::copy_constructor meant to not be accessable"); } const G4C13GEMProbability & G4C13GEMProbability:: operator=(const G4C13GEMProbability &) { throw G4HadronicException(__FILE__, __LINE__, "G4C13GEMProbability::operator= meant to not be accessable"); return *this; } G4bool G4C13GEMProbability::operator==(const G4C13GEMProbability &) const { return false; } G4bool G4C13GEMProbability::operator!=(const G4C13GEMProbability &) const { return true; }