// // ******************************************************************** // * 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: G4B11GEMProbability.cc,v 1.5 2006/06/29 20:20:25 gunter Exp $ // GEANT4 tag $Name: geant4-09-02 $ // // Hadronic Process: Nuclear De-excitations // by V. Lara (Nov 1999) // #include "G4B11GEMProbability.hh" G4B11GEMProbability::G4B11GEMProbability() : G4GEMProbability(11,5,3.0/2.0) // A,Z,Spin { ExcitEnergies.push_back(2124.693*keV); ExcitSpins.push_back(1.0/2.0); ExcitLifetimes.push_back(3.8e-15*s); ExcitEnergies.push_back(4444.89*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(0.82e-15*s); ExcitEnergies.push_back(5020.31*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(0.236e-15*s); ExcitEnergies.push_back(6742.9*keV); ExcitSpins.push_back(7.0/2.0); ExcitLifetimes.push_back(15.0e-15*s); ExcitEnergies.push_back(6791.8*keV); ExcitSpins.push_back(1.0/2.0); ExcitLifetimes.push_back(1.18e-15*s); ExcitEnergies.push_back(7285.51*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(0.4e-15*s); ExcitEnergies.push_back(7977.84*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(0.4e-15*s); ExcitEnergies.push_back(8560.3*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(0.49e-15*s); ExcitEnergies.push_back(8920.2*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(4.4e-15*s); ExcitEnergies.push_back(9185.0*keV); ExcitSpins.push_back(7.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.9*eV)); ExcitEnergies.push_back(9274.4*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4.0*keV)); ExcitEnergies.push_back(9876.0*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(110.0*keV)); ExcitEnergies.push_back(10260.0*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(165.0*keV)); ExcitEnergies.push_back(10330.0*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(110.0*keV)); ExcitEnergies.push_back(10597.0*keV); ExcitSpins.push_back(7.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV)); ExcitEnergies.push_back(10960.0*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4500.0*keV)); ExcitEnergies.push_back(11265.0*keV); ExcitSpins.push_back(9.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(110.0*keV)); ExcitEnergies.push_back(11444.0*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(103.0*keV)); ExcitEnergies.push_back(11886.0*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200.0*keV)); ExcitEnergies.push_back(12.0e3*keV); ExcitSpins.push_back(7.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV)); ExcitEnergies.push_back(12557.0*keV); ExcitSpins.push_back(1.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(210.0*keV)); ExcitEnergies.push_back(12916.0*keV); ExcitSpins.push_back(1.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(155.0*keV)); ExcitEnergies.push_back(13137.0*keV); ExcitSpins.push_back(9.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(426.0*keV)); ExcitEnergies.push_back(13.16e3*keV); ExcitSpins.push_back(7.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(430.0*keV)); ExcitEnergies.push_back(14.04e3*keV); ExcitSpins.push_back(11.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500.0*keV)); ExcitEnergies.push_back(14.34e3*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(254.0*keV)); ExcitEnergies.push_back(14565.0*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30.0*keV)); ExcitEnergies.push_back(15.32e3*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(635.0*keV)); ExcitEnergies.push_back(16437.0*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30.0*keV)); SetExcitationEnergiesPtr(&ExcitEnergies); SetExcitationSpinsPtr(&ExcitSpins); SetExcitationLifetimesPtr(&ExcitLifetimes); } G4B11GEMProbability::G4B11GEMProbability(const G4B11GEMProbability &): G4GEMProbability() { throw G4HadronicException(__FILE__, __LINE__, "G4B11GEMProbability::copy_constructor meant to not be accessable");} const G4B11GEMProbability & G4B11GEMProbability:: operator=(const G4B11GEMProbability &) { throw G4HadronicException(__FILE__, __LINE__, "G4B11GEMProbability::operator= meant to not be accessable"); return *this; } G4bool G4B11GEMProbability::operator==(const G4B11GEMProbability &) const { return false; } G4bool G4B11GEMProbability::operator!=(const G4B11GEMProbability &) const { return true; }