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G4eeToHadronsModel.hh
Go to the documentation of this file.
Or view
the newest version in sPHENIX GitHub for file G4eeToHadronsModel.hh
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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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//
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// -------------------------------------------------------------------
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//
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// GEANT4 Class header file
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//
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//
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// File name: G4eeToHadronsModel
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//
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// Author: Vladimir Ivanchenko
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//
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// Creation date: 25.10.2003
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//
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// Modifications:
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// 08-04-05 Major optimisation of internal interfaces (V.Ivantchenko)
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// 18-05-05 Use optimized interfaces (V.Ivantchenko)
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//
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//
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// Class Description:
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//
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// -------------------------------------------------------------------
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//
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#ifndef G4eeToHadronsModel_h
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#define G4eeToHadronsModel_h 1
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#include "
G4VEmModel.hh
"
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class
G4PhysicsVector
;
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class
G4Vee2hadrons
;
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class
G4eeToHadronsModel
:
public
G4VEmModel
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{
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public
:
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explicit
G4eeToHadronsModel
(
G4Vee2hadrons
*,
G4int
ver=0,
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const
G4String
& nam =
"eeToHadrons"
);
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virtual
~G4eeToHadronsModel
();
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virtual
void
Initialise
(
const
G4ParticleDefinition
*,
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const
G4DataVector
&)
override
;
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virtual
G4double
CrossSectionPerVolume
(
const
G4Material
*,
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const
G4ParticleDefinition
*,
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G4double
kineticEnergy,
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G4double
cutEnergy,
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G4double
maxEnergy)
override
;
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virtual
G4double
ComputeCrossSectionPerAtom
(
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const
G4ParticleDefinition
*,
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G4double
kineticEnergy,
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G4double
Z
,
G4double
A
,
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G4double
cutEnergy = 0.0,
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G4double
maxEnergy =
DBL_MAX
)
override
;
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virtual
G4double
ComputeCrossSectionPerElectron
(
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const
G4ParticleDefinition
*,
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G4double
kineticEnergy,
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G4double
cutEnergy = 0.0,
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G4double
maxEnergy =
DBL_MAX
);
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virtual
void
SampleSecondaries
(std::vector<G4DynamicParticle*>*,
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const
G4MaterialCutsCouple
*,
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const
G4DynamicParticle
*,
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G4double
tmin = 0.0,
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G4double
maxEnergy =
DBL_MAX
)
override
;
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G4DynamicParticle
*
GenerateCMPhoton
(
G4double
);
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inline
G4double
PeakEnergy
()
const
;
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private
:
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void
ComputeCMCrossSectionPerElectron
();
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// hide assignment operator
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G4eeToHadronsModel
&
operator=
(
const
G4eeToHadronsModel
&
right
) =
delete
;
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G4eeToHadronsModel
(
const
G4eeToHadronsModel
&) =
delete
;
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G4Vee2hadrons
*
model
;
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G4ParticleDefinition
*
theGamma
;
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G4PhysicsVector
*
crossPerElectron
;
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G4PhysicsVector
*
crossBornPerElectron
;
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G4bool
isInitialised
;
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G4int
nbins
;
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G4int
verbose
;
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G4double
lowKinEnergy
;
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G4double
peakKinEnergy
;
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G4double
highKinEnergy
;
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G4double
emin
;
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G4double
epeak
;
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G4double
emax
;
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};
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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inline
G4double
G4eeToHadronsModel::PeakEnergy
()
const
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{
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return
peakKinEnergy
;
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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#endif
geant4
tree
geant4-10.6-release
source
processes
electromagnetic
highenergy
include
G4eeToHadronsModel.hh
Built by
Jin Huang
. updated:
Wed Jun 29 2022 17:25:31
using
1.8.2 with
ECCE GitHub integration