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G4LivermorePolarizedPhotoElectricModel.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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// Author: Sebastien Incerti
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// 30 October 2008
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// on base of G4LowEnergyPhotoElectric developed by A.Forti and M.G.Pia
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//
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// 15 Mar 2010 L. Pandola, removed methods to set explicitely fluorescence cuts.
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// Main cuts from G4ProductionCutsTable are always used
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// 30 May 2011 A Mantero & V Ivanchenko Migration to model design for deexcitation
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// 22 Oct 2012 A & V Ivanchenko Migration data structure to G4PhysicsVector
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//
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#ifndef G4LivermorePolarizedPhotoElectricModel_h
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#define G4LivermorePolarizedPhotoElectricModel_h 1
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#include "
G4VEmModel.hh
"
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#include "
G4ElementData.hh
"
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#include <vector>
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class
G4ParticleChangeForGamma
;
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class
G4VAtomDeexcitation
;
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class
G4LPhysicsFreeVector
;
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class
G4LivermorePolarizedPhotoElectricModel
:
public
G4VEmModel
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{
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public
:
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G4LivermorePolarizedPhotoElectricModel
(
const
G4String
& nam =
"LivermorePolarizedPhotoElectric"
);
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virtual
~G4LivermorePolarizedPhotoElectricModel
();
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virtual
void
Initialise
(
const
G4ParticleDefinition
*,
const
G4DataVector
&);
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virtual
G4double
CrossSectionPerVolume
(
const
G4Material
*,
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const
G4ParticleDefinition
*,
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G4double
energy
,
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G4double
cutEnergy = 0.0,
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G4double
maxEnergy =
DBL_MAX
);
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virtual
G4double
ComputeCrossSectionPerAtom
(
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const
G4ParticleDefinition
*,
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G4double
energy,
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G4double
Z
,
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G4double
A
=0,
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G4double
cut=0,
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G4double
emax
=
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,
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G4double
maxEnergy);
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virtual
void
InitialiseForElement
(
const
G4ParticleDefinition
*,
G4int
Z);
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inline
void
SetLimitNumberOfShells
(
G4int
);
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protected
:
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G4ParticleChangeForGamma
*
fParticleChange
;
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private
:
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void
ReadData
(
G4int
Z,
const
char
* path = 0);
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G4LivermorePolarizedPhotoElectricModel
&
operator=
(
const
G4LivermorePolarizedPhotoElectricModel
&
right
);
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G4LivermorePolarizedPhotoElectricModel
(
const
G4LivermorePolarizedPhotoElectricModel
&);
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G4ParticleDefinition
*
theGamma
;
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G4ParticleDefinition
*
theElectron
;
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G4int
verboseLevel
;
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G4int
maxZ
;
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G4int
nShellLimit
;
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G4bool
fDeexcitationActive
;
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G4bool
isInitialised
;
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static
G4LPhysicsFreeVector
*
fCrossSection
[99];
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static
G4LPhysicsFreeVector
*
fCrossSectionLE
[99];
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static
std::vector<G4double>*
fParam
[99];
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static
G4int
fNShells
[99];
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static
G4int
fNShellsUsed
[99];
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static
G4ElementData
*
fShellCrossSection
;
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static
G4Material
*
fWater
;
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static
G4double
fWaterEnergyLimit
;
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G4VAtomDeexcitation
*
fAtomDeexcitation
;
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G4double
fCurrSection
;
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std::vector<G4double>
fSandiaCof
;
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};
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inline
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void
G4LivermorePolarizedPhotoElectricModel::SetLimitNumberOfShells
(
G4int
n
)
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{
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nShellLimit
=
n
;
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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#endif
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geant4-10.6-release
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electromagnetic
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include
G4LivermorePolarizedPhotoElectricModel.hh
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