// // ******************************************************************** // * 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. * // ******************************************************************** // // GEANT4 tag $Name: geant4-09-04-beta-01 $ // //--------------------------------------------------------------------------- // // ClassName: G4QInelasticCHIPSBuilder // // Author: 2009 M. Kosov // //---------------------------------------------------------------------------- // // Short comment: This is a physics list of only one model G4QInelastic for // all hadron-nuclear interactions at all energies. There is no model- or // process-mixing, while it is possible to merge (G4QProcessMixer) the G4_HP // processes at low energies if the G4QInelastic, which includes all necessary // nA inelastic processes, is found to be not saficient for some applications. // In this particular builder the G4QInelastic process is attached to all // hadrons other than nucleons or pi and K-mesons. Previously it could be done // only using the LHEP parameterized package or in a temporary form by the // QGSC model conditionally extended (just not crashing) to low energies. // *** Important *** As the CHIPS treatment of all hadrons is the same, and // very simple, this builder with time can be not used in the CHIPS physics list // // ----------------------------------------------------------------------------- #include "G4QInelasticCHIPSBuilder.hh" G4QInelasticCHIPSBuilder::G4QInelasticCHIPSBuilder(G4int ver): verbose(ver), wasActivated(false) { // pointer to the particle table theParticleTable = G4ParticleTable::GetParticleTable(); theParticleIterator = theParticleTable->GetIterator(); } G4QInelasticCHIPSBuilder::~G4QInelasticCHIPSBuilder() { if(wasActivated) delete inelastic; } void G4QInelasticCHIPSBuilder::Build() { if(wasActivated) return; wasActivated = true; theParticleIterator->reset(); inelastic = new G4QInelastic(); while( (*theParticleIterator)() ) { G4ParticleDefinition* particle = theParticleIterator->value(); G4String pname = particle->GetParticleName(); if(pname == "kaon-" || pname == "kaon+" || pname == "kaon0S" || pname == "kaon0L" || pname == "pi-" || pname == "pi+" || pname == "neutron" || pname == "proton" || pname == "lambda" || pname == "sigma+" || pname == "sigma0" || pname == "sigma-" || pname == "xi0" || pname == "xi-" || pname == "omega-" || pname == "anti_proton" || pname == "anti_neutron" || pname == "anti_lambda" || pname == "anti_sigma+" || pname == "anti_sigma0" || pname == "anti_sigma-" || pname == "anti_xi0" || pname == "anti_xi-" || pname == "anti_omega-" ) { if(verbose>1)G4cout<< "__G4QInelCHIPSBuilder: "<< pname <<" is defined here"<GetProcessManager(); pmanager->AddDiscreteProcess(inelastic); if(verbose>1) G4cout<<"###> G4QInelasticCHIPSBuilder: "<GetProcessName() <<" is added for "<