// // ******************************************************************** // * 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: G4O19GEMProbability.cc,v 1.5 2006/06/29 20:23:33 gunter Exp $ // GEANT4 tag $Name: geant4-09-02 $ // // Hadronic Process: Nuclear De-excitations // by V. Lara (Nov 1999) // #include "G4O19GEMProbability.hh" G4O19GEMProbability::G4O19GEMProbability() : G4GEMProbability(19,8,5.0/2.0) // A,Z,Spin { ExcitEnergies.push_back(96.0*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(1.37e-3*picosecond); ExcitEnergies.push_back(1471.7*keV); ExcitSpins.push_back(1.0/2.0); ExcitLifetimes.push_back(0.78*picosecond); ExcitEnergies.push_back(3154.5*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(1.0*picosecond); ExcitEnergies.push_back(4583.0*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(53.0*keV)); ExcitEnergies.push_back(4707.0*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(15.0*keV)); ExcitEnergies.push_back(5086.0*keV); ExcitSpins.push_back(1.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(49.0*keV)); ExcitEnergies.push_back(5149.0*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.4*keV)); ExcitEnergies.push_back(5455.0*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(330.0*keV)); ExcitEnergies.push_back(5706.0*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7.8*keV)); ExcitEnergies.push_back(6130.0*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(150.0*keV)); ExcitEnergies.push_back(6200.0*keV); ExcitSpins.push_back(1.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(140.0*keV)); ExcitEnergies.push_back(6276.0*keV); ExcitSpins.push_back(7.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(19.2*keV)); } G4O19GEMProbability::G4O19GEMProbability(const G4O19GEMProbability &) : G4GEMProbability() { throw G4HadronicException(__FILE__, __LINE__, "G4O19GEMProbability::copy_constructor meant to not be accessable"); } const G4O19GEMProbability & G4O19GEMProbability:: operator=(const G4O19GEMProbability &) { throw G4HadronicException(__FILE__, __LINE__, "G4O19GEMProbability::operator= meant to not be accessable"); return *this; } G4bool G4O19GEMProbability::operator==(const G4O19GEMProbability &) const { return false; } G4bool G4O19GEMProbability::operator!=(const G4O19GEMProbability &) const { return true; }