// // ******************************************************************** // * 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: G4Be11GEMProbability.cc,v 1.5 2006/06/29 20:21:25 gunter Exp $ // GEANT4 tag $Name: geant4-09-02-ref-02 $ // // Hadronic Process: Nuclear De-excitations // by V. Lara (Nov 1999) // #include "G4Be11GEMProbability.hh" G4Be11GEMProbability::G4Be11GEMProbability() : G4GEMProbability(11,4,1.0/2.0) // A,Z,Spin { ExcitEnergies.push_back(320.04*keV); ExcitSpins.push_back(1.0/2); ExcitLifetimes.push_back(115.0e-15*s); ExcitEnergies.push_back(1778.0*keV); ExcitSpins.push_back(5.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV)); ExcitEnergies.push_back(2.69e3*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200.0*keV)); ExcitEnergies.push_back(3.41e3*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(125.0*keV)); ExcitEnergies.push_back(3887.0*keV); ExcitSpins.push_back(7.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(10.0*keV)); ExcitEnergies.push_back(3956.0*keV); ExcitSpins.push_back(3.0/2.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(15.0*keV)); ExcitEnergies.push_back(5240.0*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(45.0*keV)); ExcitEnergies.push_back(5.86e3*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV)); ExcitEnergies.push_back(6.51e3*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(120.0*keV)); ExcitEnergies.push_back(6705.0*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40.0*keV)); ExcitEnergies.push_back(7.03e3*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV)); ExcitEnergies.push_back(8816.0*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV)); ExcitEnergies.push_back(10.59e3*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(210.0*keV)); SetExcitationEnergiesPtr(&ExcitEnergies); SetExcitationSpinsPtr(&ExcitSpins); SetExcitationLifetimesPtr(&ExcitLifetimes); } G4Be11GEMProbability::G4Be11GEMProbability(const G4Be11GEMProbability &) : G4GEMProbability() { throw G4HadronicException(__FILE__, __LINE__, "G4Be11GEMProbability::copy_constructor meant to not be accessable"); } const G4Be11GEMProbability & G4Be11GEMProbability:: operator=(const G4Be11GEMProbability &) { throw G4HadronicException(__FILE__, __LINE__, "G4Be11GEMProbability::operator= meant to not be accessable"); return *this; } G4bool G4Be11GEMProbability::operator==(const G4Be11GEMProbability &) const { return false; } G4bool G4Be11GEMProbability::operator!=(const G4Be11GEMProbability &) const { return true; }