// // ******************************************************************** // * 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: G4C12GEMProbability.cc,v 1.5 2006/06/29 20:21:39 gunter Exp $ // GEANT4 tag $Name: geant4-09-02-ref-02 $ // // Hadronic Process: Nuclear De-excitations // by V. Lara (Nov 1999) // #include "G4C12GEMProbability.hh" G4C12GEMProbability::G4C12GEMProbability() : G4GEMProbability(12,6,0.0) // A,Z,Spin { ExcitEnergies.push_back(4438.91*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(10.8e-3*eV)); ExcitEnergies.push_back(7654.2*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(8.5*keV)); ExcitEnergies.push_back(9641*keV); ExcitSpins.push_back(3.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(34*keV)); ExcitEnergies.push_back(1.03E+4*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.0e3*keV)); ExcitEnergies.push_back(10844*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(315*keV)); ExcitEnergies.push_back(1.116E+4*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(430*keV)); ExcitEnergies.push_back(1.1828E+4*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(260*keV)); ExcitEnergies.push_back(12710*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(18.1*eV)); ExcitEnergies.push_back(13352*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(375*keV)); ExcitEnergies.push_back(14083*keV); ExcitSpins.push_back(4.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(258*keV)); ExcitEnergies.push_back(15110*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(42*eV)); ExcitEnergies.push_back(16106.7*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5.2*keV)); ExcitEnergies.push_back(16.57E+3*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); ExcitEnergies.push_back(17.23E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1150*keV)); ExcitEnergies.push_back(17.76E+3*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(80*keV)); ExcitEnergies.push_back(18.13E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600*keV)); ExcitEnergies.push_back(18.27E+3*keV); ExcitSpins.push_back(4.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); ExcitEnergies.push_back(18.38E+3*keV); ExcitSpins.push_back(3.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(220*keV)); ExcitEnergies.push_back(18.39E+3*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(43*keV)); ExcitEnergies.push_back(18.6E+3*keV); ExcitSpins.push_back(3.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); ExcitEnergies.push_back(18.80E+3*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); ExcitEnergies.push_back(19.2E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1100*keV)); ExcitEnergies.push_back(19.39E+3*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800*keV)); ExcitEnergies.push_back(19.55E+3*keV); ExcitSpins.push_back(4.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(490*keV)); ExcitEnergies.push_back(19.69E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(230*keV)); ExcitEnergies.push_back(20.0E+3*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); ExcitEnergies.push_back(20.27E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(140*keV)); ExcitEnergies.push_back(20.5E+3*keV); ExcitSpins.push_back(3.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(180*keV)); ExcitEnergies.push_back(20.62E+3*keV); ExcitSpins.push_back(3.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200*keV)); ExcitEnergies.push_back(21.60E+3*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1200*keV)); ExcitEnergies.push_back(22.0E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800*keV)); ExcitEnergies.push_back(22.40E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(275*keV)); ExcitEnergies.push_back(22.65E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3200*keV)); ExcitEnergies.push_back(23.04E+3 *keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(60*keV)); ExcitEnergies.push_back(23.52E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(230*keV)); ExcitEnergies.push_back(23.92E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400*keV)); ExcitEnergies.push_back(25.30E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(510*keV)); ExcitEnergies.push_back(25.4E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2000*keV)); ExcitEnergies.push_back(27.0E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1400*keV)); ExcitEnergies.push_back(27595.0*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30*keV)); ExcitEnergies.push_back(28.2E+3*keV); ExcitSpins.push_back(1.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1600*keV)); SetExcitationEnergiesPtr(&ExcitEnergies); SetExcitationSpinsPtr(&ExcitSpins); SetExcitationLifetimesPtr(&ExcitLifetimes); } G4C12GEMProbability::G4C12GEMProbability(const G4C12GEMProbability &) : G4GEMProbability() { throw G4HadronicException(__FILE__, __LINE__, "G4C12GEMProbability::copy_constructor meant to not be accessable"); } const G4C12GEMProbability & G4C12GEMProbability:: operator=(const G4C12GEMProbability &) { throw G4HadronicException(__FILE__, __LINE__, "G4C12GEMProbability::operator= meant to not be accessable"); return *this; } G4bool G4C12GEMProbability::operator==(const G4C12GEMProbability &) const { return false; } G4bool G4C12GEMProbability::operator!=(const G4C12GEMProbability &) const { return true; }