// // ******************************************************************** // * 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: G4He3GEMProbability.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) // // J.M. Quesada (July 2009) C's and k's values according to Furihata's paper // (based on notes added on proof in Dostrovskii's paper) #include "G4He3GEMProbability.hh" G4He3GEMProbability::G4He3GEMProbability() : G4GEMProbability(3,2,1.0/2.0) // A,Z,Gamma { SetExcitationEnergiesPtr(&ExcitEnergies); SetExcitationSpinsPtr(&ExcitSpins); SetExcitationLifetimesPtr(&ExcitLifetimes); } G4He3GEMProbability::G4He3GEMProbability(const G4He3GEMProbability &) : G4GEMProbability() { throw G4HadronicException(__FILE__, __LINE__, "G4He3GEMProbability::copy_constructor meant to not be accessable"); } const G4He3GEMProbability & G4He3GEMProbability:: operator=(const G4He3GEMProbability &) { throw G4HadronicException(__FILE__, __LINE__, "G4He3GEMProbability::operator= meant to not be accessable"); return *this; } G4bool G4He3GEMProbability::operator==(const G4He3GEMProbability &) const { return false; } G4bool G4He3GEMProbability::operator!=(const G4He3GEMProbability &) const { return true; } //JMQ 190709 C's values from Furihata's paper //(notes added on proof in Dostrovskii's paper) G4double G4He3GEMProbability::CCoeficient(const G4double/* aZ*/) const { return 0.; } //G4double G4He3GEMProbability::CCoeficient(const G4double aZ) const //{ // Data comes from // Dostrovsky, Fraenkel and Friedlander // Physical Review, vol 116, num. 3 1959 // // const G4int size = 5; // G4double Zlist[5] = { 10.0, 20.0, 30.0, 50.0, 70.0}; // G4double Calpha[5] = { 0.10, 0.10, 0.10, 0.08, 0.06}; // C for He3 is equal to C for alpha times 4/3 // G4double C = 0.0; // if (aZ <= 30) { // C = 0.10; // } else if (aZ <= 50) { // C = 0.1 + -((aZ-50.)/20.)*0.02; // } else if (aZ < 70) { // C = 0.08 + -((aZ-70.)/20.)*0.02; // } else { // C = 0.06; // } // return C*(4.0/3.0); //}