// // ******************************************************************** // * 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. * // ******************************************************************** // // $Id$ // //--------------------------------------------------------------------------- // // 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 #include "globals.hh" #include "G4VModularPhysicsList.hh" #include "CompileTimeConstraints.hh" template class TQGSC_CHIPS: public T { public: TQGSC_CHIPS(G4int ver = 1); virtual ~TQGSC_CHIPS(); public: // SetCuts() virtual void SetCuts(); private: enum {ok = CompileTimeConstraints::IsA::ok }; }; #include "QGSC_CHIPS.icc" typedef TQGSC_CHIPS QGSC_CHIPS; #endif