// // ******************************************************************** // * 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: G4FissionParameters.cc,v 1.7 2009/11/19 10:30:49 vnivanch Exp $ // GEANT4 tag $Name: geant4-09-03-ref-09 $ // // Hadronic Process: Nuclear De-excitations // by V. Lara (Oct 1998) // //J. M. Quesada (May 2009): sigma_sym (SigmaS) tuned for spallation data. //J. M. Quesada (30.10.09): retuning for IAEA spallation data #include "G4FissionParameters.hh" #include "G4HadronicException.hh" const G4double G4FissionParameters::A1 = 134.0; const G4double G4FissionParameters::A2 = 141.0; G4FissionParameters::G4FissionParameters(const G4int A, const G4int Z, const G4double ExEnergy, const G4double FissionBarrier) { G4double U = ExEnergy; As = A/2.0; if (A <= 235) Sigma2 = 5.6; // MeV else Sigma2 = 5.6 + 0.096*(A-235); // MeV Sigma1 = 0.5*Sigma2; // MeV SigmaS = std::exp(0.00553*U/MeV + 2.1386); // MeV //JMQ 310509 // if (SigmaS > 20.0) SigmaS = 20.0; // SigmaS*=1.3; //JMQ 301009: retuning (after CEM transition prob.have been chosen as default) SigmaS*=0.8; // G4double FasymAsym = 2.0*std::exp(-((A2-As)*(A2-As))/(2.0*Sigma2*Sigma2)) + std::exp(-((A1-As)*(A1-As))/(2.0*Sigma1*Sigma1)); G4double FsymA1A2 = std::exp(-((As-(A1+A2)/2.0)*(As-(A1+A2)/2.0))/(2.0*SigmaS*SigmaS)); G4double wa = 0.0; w = 0.0; if (Z >= 90) { // Z >= 90 if (U <= 16.25) wa = std::exp(0.5385*U/MeV-9.9564); // U <= 16.25 MeV else wa = std::exp(0.09197*U/MeV-2.7003); // U > 16.25 MeV } else if (Z == 89) { // Z == 89 wa = std::exp(0.09197*U-1.0808); } else if (Z >= 82) { // 82 <= Z <= 88 G4double X = FissionBarrier - 7.5*MeV; if (X < 0.0) X = 0.0; wa = std::exp(0.09197*(U-X)/MeV-1.0808); } else { // Z < 82 w = 1001.0; } if (w == 0.0) { G4double w1 = std::max(1.03*wa - FasymAsym, 0.0001); G4double w2 = std::max(1.0 - FsymA1A2*wa, 0.0001); w = w1/w2; if (82 <= Z && Z < 89 && A < 227) w *= std::exp(0.3*(227-A)); } } G4FissionParameters::G4FissionParameters(const G4FissionParameters &) { throw G4HadronicException(__FILE__, __LINE__, "G4FissionParameters::copy_constructor meant to not be accessable"); } const G4FissionParameters & G4FissionParameters::operator=(const G4FissionParameters &) { throw G4HadronicException(__FILE__, __LINE__, "G4FissionParameters::operator= meant to not be accessable"); return *this; } G4bool G4FissionParameters::operator==(const G4FissionParameters &) const { return false; } G4bool G4FissionParameters::operator!=(const G4FissionParameters &) const { return true; }