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G4LivermoreBremsstrahlungModel.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: G4LivermoreBremsstrahlungModel
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//
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// Author: Andreas Schaelicke & Vladimir Ivantchenko
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//
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// Creation date: 04.10.2011
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//
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// Modifications:
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//
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//
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// Class Description:
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//
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// Implementation of the bremssrahlung energy spectrum using
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// 1. S.M. Seltzer and M.J. Berger Nucl. Instr. Meth. B12 (1985) 95
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// 2. S.M. Seltzer and M.J. Berger Atomic data and Nuclear Data
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// Tables 35 (1986) 345
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// Cross section computation in the base class G4eBremsstrahlungRelModel
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// -------------------------------------------------------------------
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//
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#ifndef G4LivermoreBremsstrahlungModel_h
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#define G4LivermoreBremsstrahlungModel_h 1
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#include "
G4eBremsstrahlungRelModel.hh
"
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#include "
globals.hh
"
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class
G4Physics2DVector
;
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class
G4LivermoreBremsstrahlungModel
:
public
G4eBremsstrahlungRelModel
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{
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public
:
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G4LivermoreBremsstrahlungModel
(
const
G4ParticleDefinition
*
p
= 0,
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const
G4String
& nam =
"LowEnBrem"
);
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virtual
~G4LivermoreBremsstrahlungModel
();
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virtual
void
Initialise
(
const
G4ParticleDefinition
*,
const
G4DataVector
&);
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virtual
void
InitialiseForElement
(
const
G4ParticleDefinition
*,
G4int
Z
);
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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
cutEnergy,
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G4double
maxEnergy);
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inline
void
SetBicubicInterpolationFlag
(
G4bool
);
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protected
:
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virtual
G4double
ComputeDXSectionPerAtom
(
G4double
gammaEnergy);
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virtual
G4String
DirectoryPath
()
const
;
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private
:
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void
ReadData
(
G4int
Z,
const
char
* path = 0);
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// hide assignment operator
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G4LivermoreBremsstrahlungModel
&
operator=
(
const
G4LivermoreBremsstrahlungModel
&
right
);
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G4LivermoreBremsstrahlungModel
(
const
G4LivermoreBremsstrahlungModel
&);
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static
G4Physics2DVector
*
dataSB
[101];
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static
G4double
ylimit
[101];
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static
G4double
expnumlim
;
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G4int
nwarn
;
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size_t
idx
;
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size_t
idy
;
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G4bool
useBicubicInterpolation
;
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};
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inline
void
G4LivermoreBremsstrahlungModel::SetBicubicInterpolationFlag
(
G4bool
val)
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{
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useBicubicInterpolation
= val;
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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
lowenergy
include
G4LivermoreBremsstrahlungModel.hh
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Jin Huang
. updated:
Wed Jun 29 2022 17:25:31
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