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/// \file CRMC_FTFP_BERT.hh
/// \brief Definition of the CRMC_FTFP_BERT class

//---------------------------------------------------------------------------
//
// ClassName: CRMC_FTFP_BERT
//
// Author:    2018 Alberto Ribon
//
// This is a variant of the FTFP_BERT physics list, whereby CRMC is used
// for modeling final-state pion- , kaon- , proton- , neutron- and
// ion-nuclear inelastic interactions at very high energies (above a
// threshold defined in HadronPhysicsCRMC_FTFP_BERT and IonCRMCPhysics).
// For the remaining inelastic interactions (i.e. hyperon- , antihyperon- ,
// antinucleon- and light anti-ion-nuclear interactions, as well as
// for all elastic final-state interactions, and for all elastic and
// inelastic hadronic cross sections), the usual Geant4 approach, as in
// FTFP_BERT is used.
//
// Modified:
// -  18-May-2021 Alberto Ribon : Migrated to non-templated physics list.
//
//----------------------------------------------------------------------------
//
#ifndef CRMC_FTFP_BERT_h
#define CRMC_FTFP_BERT_h 1

#include "G4VModularPhysicsList.hh"
#include "globals.hh"

class CRMC_FTFP_BERT : public G4VModularPhysicsList
{
  public:
    CRMC_FTFP_BERT(G4int ver = 1);
    virtual ~CRMC_FTFP_BERT() = default;

    CRMC_FTFP_BERT(const CRMC_FTFP_BERT&) = delete;
    CRMC_FTFP_BERT& operator=(const CRMC_FTFP_BERT&) = delete;
};

#endif