Gabriele Cosmo
91 lines
3.5 KiB
C++
91 lines
3.5 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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/// \file hadronic/Hadr02/include/CRMC_FTFP_BERT.hh
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/// \brief Definition of the CRMC_FTFP_BERT class
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//
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//
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//---------------------------------------------------------------------------
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//
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// ClassName: CRMC_FTFP_BERT
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//
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// Author: 2018 Alberto Ribon
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//
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// This is a variant of the FTFP_BERT physics list, whereby CRMC is used
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// for modeling final-state pion- , kaon- , proton- , neutron- and
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// ion-nuclear inelastic interactions at very high energies (above a
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// threshold defined in HadronPhysicsCRMC_FTFP_BERT and IonCRMCPhysics).
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// For the remaining inelastic interactions (i.e. hyperon- , antihyperon- ,
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// antinucleon- and light anti-ion-nuclear interactions, as well as
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// for all elastic final-state interactions, and for all elastic and
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// inelastic hadronic cross sections, the usual Geant4 approach, as in
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// FTFP_BERT is used.
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//
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// Modified:
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//
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//----------------------------------------------------------------------------
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//
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#ifndef TCRMC_FTFP_BERT_h
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#define TCRMC_FTFP_BERT_h 1
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#include "G4VModularPhysicsList.hh"
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#include "globals.hh"
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#include "CompileTimeConstraints.hh"
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template<class T>
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class TCRMC_FTFP_BERT: public T {
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public:
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TCRMC_FTFP_BERT( G4int ver = 1 );
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virtual ~TCRMC_FTFP_BERT();
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virtual void SetCuts();
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private:
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enum { ok = CompileTimeConstraints::IsA< T, G4VModularPhysicsList >::ok };
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};
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#ifdef G4_USE_CRMC
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#include "CRMC_FTFP_BERT.icc"
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#else
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template<class T>
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TCRMC_FTFP_BERT<T>::TCRMC_FTFP_BERT( G4int ) : T() {
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G4ExceptionDescription de;
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de << "Support for CRMC_FTFP_BERT not enabled" << G4endl;
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G4Exception( __FILE__, "CRMC_FTFP_BERT-01", FatalException, de,
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"Code should be compiled with G4_USE_CRMC environment variable set.");
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}
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template<class T>
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TCRMC_FTFP_BERT<T>::~TCRMC_FTFP_BERT() { }
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template<class T>
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void TCRMC_FTFP_BERT<T>::SetCuts() {}
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#endif
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typedef TCRMC_FTFP_BERT< G4VModularPhysicsList > CRMC_FTFP_BERT;
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#endif //TCRMC_FTFP_BERT_h
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