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// $Id: QGSC_CHIPS.hh,v 1.3 2009/04/17 15:29:19 mkossov Exp $
// GEANT4 tag $Name: geant4-09-03 $
//
//---------------------------------------------------------------------------
//
// ClassName: QGSC_CHIPS
//
// Author: 2009 M.Kosov (Development of the QGSC_QGSC physics list)
//
// Modified:
//
//-------------------------------------------------------------------------------
//  Short description: In tis file the aim is to get rid of LHEP, use the
//  QGSC model with the Energy Flow interface for CHIPS from E=0 for all
//  hadrons and gradually substitute QGSC by the native CHIPS (G4QCollision)
//  process starting from low energies (first nucleons, then mesons, after that
//  hyperons and antibaryons). The present "QGSC" model at low energies is
//  jus a temporary (far from ideal) interface to the CHIPS model. The nuclear
//  fragmentation CHIPS algorithm is the same in both models, but the first
//  interaction is temporary taken from the QGSC algorithm, which is not expected
//  to work at low energies, but temporary can be used as an interface to CHIPS.
//-------------------------------------------------------------------------------
#ifndef TQGSC_CHIPS_h
#define TQGSC_CHIPS_h 1

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

template<class T>
class TQGSC_CHIPS: public T
{
public:
  TQGSC_CHIPS(G4int ver = 1);
  virtual ~TQGSC_CHIPS();
  
public:
  // SetCuts() 
  virtual void SetCuts();

private:
  enum {ok = CompileTimeConstraints::IsA<T, G4VModularPhysicsList>::ok };
};
#include "QGSC_CHIPS.icc"
typedef TQGSC_CHIPS<G4VModularPhysicsList> QGSC_CHIPS;

#endif
