Gabriele Cosmo
237 lines
8.6 KiB
C++
237 lines
8.6 KiB
C++
//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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// Authors: Francesco Longo, franzlongo1969@gmail.com
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//
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// Code based on the hadrontherapy && radioprotection advanced example
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#include "GammaRayTelPhysicsList.hh"
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#include "GammaRayTelPhysicsListMessenger.hh"
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#include "G4PhysListFactory.hh"
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#include "G4VPhysicsConstructor.hh"
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// Physic lists (contained inside the Geant4 distribution)
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#include "G4EmStandardPhysics_option3.hh"
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#include "G4EmStandardPhysics_option4.hh" // to treat the new polarised process
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#include "G4EmLivermorePhysics.hh"
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#include "G4EmPenelopePhysics.hh"
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#include "G4EmLivermorePolarizedPhysics.hh" //
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#include "G4DecayPhysics.hh"
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#include "G4HadronElasticPhysics.hh"
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#include "G4HadronDElasticPhysics.hh"
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#include "G4HadronElasticPhysicsHP.hh"
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#include "G4IonBinaryCascadePhysics.hh"
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#include "G4Decay.hh"
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#include "G4StepLimiter.hh"
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#include "G4LossTableManager.hh"
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#include "G4UnitsTable.hh"
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#include "G4SystemOfUnits.hh"
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#include "G4ProcessManager.hh"
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#include "G4IonFluctuations.hh"
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#include "G4IonParametrisedLossModel.hh"
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#include "G4HadronPhysicsQGSP_BIC_HP.hh"
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#include "G4RadioactiveDecayPhysics.hh"
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/////////////////////////////////////////////////////////////////////////////
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GammaRayTelPhysicsList::GammaRayTelPhysicsList() : G4VModularPhysicsList()
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{
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G4LossTableManager::Instance();
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defaultCutValue = 100*micrometer;
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SetVerboseLevel(1);
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G4ProductionCutsTable::GetProductionCutsTable()->SetEnergyRange(250*eV, 1*GeV);
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SetDefaultCutValue(defaultCutValue);
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DumpCutValuesTable();
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helIsRegisted = false;
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bicIsRegisted = false;
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biciIsRegisted = false;
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locIonIonInelasticIsRegistered = false;
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radioactiveDecayIsRegisted = false;
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pMessenger = new GammaRayTelPhysicsListMessenger(this);
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SetVerboseLevel(1);
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// EM physics
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emPhysicsList = new G4EmStandardPhysics_option3(1);
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emName = G4String("emstandard_opt3");
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// Decay physics and all particles
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decPhysicsList = new G4DecayPhysics();
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}
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/////////////////////////////////////////////////////////////////////////////
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GammaRayTelPhysicsList::~GammaRayTelPhysicsList()
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{
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delete pMessenger;
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delete emPhysicsList;
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delete decPhysicsList;
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for(size_t i=0; i<hadronPhys.size(); i++) {delete hadronPhys[i];}
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}
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/////////////////////////////////////////////////////////////////////////////
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void GammaRayTelPhysicsList::AddPackage(const G4String& name)
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{
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G4PhysListFactory factory;
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G4VModularPhysicsList* phys =factory.GetReferencePhysList(name);
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G4int i=0;
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const G4VPhysicsConstructor* elem= phys->GetPhysics(i);
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G4VPhysicsConstructor* tmp = const_cast<G4VPhysicsConstructor*> (elem);
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while (elem !=0)
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{
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RegisterPhysics(tmp);
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elem= phys->GetPhysics(++i) ;
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tmp = const_cast<G4VPhysicsConstructor*> (elem);
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}
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}
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/////////////////////////////////////////////////////////////////////////////
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void GammaRayTelPhysicsList::ConstructParticle()
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{
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decPhysicsList->ConstructParticle();
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}
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/////////////////////////////////////////////////////////////////////////////
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void GammaRayTelPhysicsList::ConstructProcess()
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{
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// transportation
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//
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AddTransportation();
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// electromagnetic physics list
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//
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emPhysicsList->ConstructProcess();
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em_config.AddModels();
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// decay physics list
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//
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decPhysicsList->ConstructProcess();
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// hadronic physics lists
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for(size_t i=0; i<hadronPhys.size(); i++) {
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hadronPhys[i]->ConstructProcess();
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}
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// step limitation (as a full process)
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//
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// AddStepMax();
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}
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/////////////////////////////////////////////////////////////////////////////
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void GammaRayTelPhysicsList::AddPhysicsList(const G4String& name)
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{
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if (verboseLevel>1) {
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G4cout << "PhysicsList::AddPhysicsList: <" << name << ">" << G4endl;
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}
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if (name == emName) return;
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/////////////////////////////////////////////////////////////////////////////
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// ELECTROMAGNETIC MODELS
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/////////////////////////////////////////////////////////////////////////////
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if (name == "standard_opt3") {
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emName = name;
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delete emPhysicsList;
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emPhysicsList = new G4EmStandardPhysics_option3();
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G4cout << "THE FOLLOWING ELECTROMAGNETIC PHYSICS LIST HAS BEEN ACTIVATED: G4EmStandardPhysics_option3" << G4endl;
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} else if (name == "LowE_Livermore") {
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emName = name;
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delete emPhysicsList;
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emPhysicsList = new G4EmLivermorePhysics();
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G4cout << "THE FOLLOWING ELECTROMAGNETIC PHYSICS LIST HAS BEEN ACTIVATED: G4EmLivermorePhysics" << G4endl;
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} else if (name == "LowE_Penelope") {
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emName = name;
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delete emPhysicsList;
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emPhysicsList = new G4EmPenelopePhysics();
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G4cout << "THE FOLLOWING ELECTROMAGNETIC PHYSICS LIST HAS BEEN ACTIVATED: G4EmLivermorePhysics" << G4endl;
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} else if (name == "LowE_Polarized") {
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emName = name;
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delete emPhysicsList;
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emPhysicsList = new G4EmLivermorePolarizedPhysics();
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G4cout << "THE FOLLOWING ELECTROMAGNETIC PHYSICS LIST HAS BEEN ACTIVATED: G4EmLivermorePhysics" << G4endl;
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} else if (name == "standard_opt4") {
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emName = name;
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delete emPhysicsList;
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emPhysicsList = new G4EmStandardPhysics_option4();
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G4cout << "THE FOLLOWING ELECTROMAGNETIC PHYSICS LIST HAS BEEN ACTIVATED: G4EmStandardOption_4" << G4endl;
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/////////////////////////////////////////////////////////////////////////////
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// HADRONIC MODELS
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/////////////////////////////////////////////////////////////////////////////
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} else if (name == "elastic" && !helIsRegisted) {
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G4cout << "THE FOLLOWING HADRONIC ELASTIC PHYSICS LIST HAS BEEN ACTIVATED: G4HadronElasticPhysics()" << G4endl;
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hadronPhys.push_back( new G4HadronElasticPhysics());
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helIsRegisted = true;
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} else if (name == "DElastic" && !helIsRegisted) {
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hadronPhys.push_back( new G4HadronDElasticPhysics());
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helIsRegisted = true;
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} else if (name == "HPElastic" && !helIsRegisted) {
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hadronPhys.push_back( new G4HadronElasticPhysicsHP());
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helIsRegisted = true;
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} else if (name == "binary" && !bicIsRegisted) {
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hadronPhys.push_back(new G4HadronPhysicsQGSP_BIC_HP());
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bicIsRegisted = true;
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G4cout << "THE FOLLOWING HADRONIC INELASTIC PHYSICS LIST HAS BEEN ACTIVATED: HadronPhysicsQGSP_BIC_HP()" << G4endl;
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} else if (name == "binary_ion" && !biciIsRegisted) {
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hadronPhys.push_back(new G4IonBinaryCascadePhysics());
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biciIsRegisted = true;
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G4cout << "THE FOLLOWING HADRONIC INELASTIC PHYSICS LIST HAS BEEN ACTIVATED: G4IonBinaryCascadePhysics()" << G4endl;
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} else if (name == "radioactive_decay" && !radioactiveDecayIsRegisted ) {
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hadronPhys.push_back(new G4RadioactiveDecayPhysics());
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radioactiveDecayIsRegisted = true;
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G4cout << "THE FOLLOWING HADRONIC INELASTIC PHYSICS LIST HAS BEEN ACTIVATED: G4RadioactiveDecayPhysics()" << G4endl;
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} else {
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G4cout << "PhysicsList::AddPhysicsList: <" << name << ">"
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<< " is not defined"
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<< G4endl;
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}
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}
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void GammaRayTelPhysicsList::SetCutForGamma(G4double cut)
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{
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SetParticleCuts(cut, G4Gamma::Gamma());
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}
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void GammaRayTelPhysicsList::SetCutForElectron(G4double cut)
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{
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SetParticleCuts(cut, G4Electron::Electron());
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}
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void GammaRayTelPhysicsList::SetCutForPositron(G4double cut)
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{
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SetParticleCuts(cut, G4Positron::Positron());
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}
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