// // ******************************************************************** // * 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: G4Mg22GEMProbability.cc,v 1.5 2009/09/15 12:54:17 vnivanch Exp $ // GEANT4 tag $Name: geant4-09-03-ref-09 $ // // Hadronic Process: Nuclear De-excitations // by V. Lara (Nov 1999) // #include "G4Mg22GEMProbability.hh" G4Mg22GEMProbability::G4Mg22GEMProbability() : G4GEMProbability(22,12,0.0) // A,Z,Spin { ExcitEnergies.push_back(1246.3*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(2.1*picosecond); ExcitEnergies.push_back(3308.2*keV); ExcitSpins.push_back(4.0); ExcitLifetimes.push_back(201.0e-3*picosecond); ExcitEnergies.push_back(4400.9*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(21.0e-3*picosecond); ExcitEnergies.push_back(5006.0*keV); ExcitSpins.push_back(0.0); ExcitLifetimes.push_back(17.0*nanosecond); ExcitEnergies.push_back(5037.0*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(69.0*picosecond); ExcitEnergies.push_back(5292.0*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(44.0e-3*picosecond); ExcitEnergies.push_back(5317.0*keV); ExcitSpins.push_back(3.0); ExcitLifetimes.push_back(17.0*nanosecond); ExcitEnergies.push_back(5464.0*keV); ExcitSpins.push_back(4.0); ExcitLifetimes.push_back(69.0*picosecond); ExcitEnergies.push_back(5713.9*keV); ExcitSpins.push_back(2.0); ExcitLifetimes.push_back(28.0e-3*picosecond); } G4Mg22GEMProbability::G4Mg22GEMProbability(const G4Mg22GEMProbability &) : G4GEMProbability() { throw G4HadronicException(__FILE__, __LINE__, "G4Mg22GEMProbability::copy_constructor meant to not be accessable"); } const G4Mg22GEMProbability & G4Mg22GEMProbability:: operator=(const G4Mg22GEMProbability &) { throw G4HadronicException(__FILE__, __LINE__, "G4Mg22GEMProbability::operator= meant to not be accessable"); return *this; } G4bool G4Mg22GEMProbability::operator==(const G4Mg22GEMProbability &) const { return false; } G4bool G4Mg22GEMProbability::operator!=(const G4Mg22GEMProbability &) const { return true; }