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geant4_9_6_p02
source
physics_lists
lists
include
QGSC_CHIPS.hh
Go to the documentation of this file.
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//
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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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// $Id$
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//
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//---------------------------------------------------------------------------
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//
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// ClassName: QGSC_CHIPS
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//
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// Author: 2009 M.Kosov (Development of the QGSC_QGSC physics list)
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//
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// Modified:
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//
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//-------------------------------------------------------------------------------
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// Short description: In tis file the aim is to get rid of LHEP, use the
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// QGSC model with the Energy Flow interface for CHIPS from E=0 for all
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// hadrons and gradually substitute QGSC by the native CHIPS (G4QCollision)
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// process starting from low energies (first nucleons, then mesons, after that
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// hyperons and antibaryons). The present "QGSC" model at low energies is
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// jus a temporary (far from ideal) interface to the CHIPS model. The nuclear
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// fragmentation CHIPS algorithm is the same in both models, but the first
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// interaction is temporary taken from the QGSC algorithm, which is not expected
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// to work at low energies, but temporary can be used as an interface to CHIPS.
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//-------------------------------------------------------------------------------
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#ifndef TQGSC_CHIPS_h
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#define TQGSC_CHIPS_h 1
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#include <
CLHEP/Units/SystemOfUnits.h
>
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#include "
globals.hh
"
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#include "
G4VModularPhysicsList.hh
"
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#include "
CompileTimeConstraints.hh
"
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template
<
class
T>
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class
TQGSC_CHIPS
:
public
T
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{
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public
:
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TQGSC_CHIPS
(
G4int
ver = 1);
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virtual
~TQGSC_CHIPS
();
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public
:
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// SetCuts()
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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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#include "QGSC_CHIPS.icc"
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typedef
TQGSC_CHIPS<G4VModularPhysicsList>
QGSC_CHIPS
;
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#endif
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