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9.6.p02
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geant4_9_6_p02
source
processes
hadronic
models
de_excitation
evaporation
include
G4EvaporationProbability.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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//J.M. Quesada (August2008). Based on:
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//
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// Hadronic Process: Nuclear De-excitations
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// by V. Lara (Oct 1998)
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//
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#ifndef G4EvaporationProbability_h
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#define G4EvaporationProbability_h 1
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#include "
G4VEmissionProbability.hh
"
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#include "
G4VLevelDensityParameter.hh
"
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#include "
G4EvaporationLevelDensityParameter.hh
"
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#include "
G4VCoulombBarrier.hh
"
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#include "
G4CoulombBarrier.hh
"
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class
G4EvaporationProbability
:
public
G4VEmissionProbability
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{
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public
:
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// Only available constructor
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G4EvaporationProbability
(
G4int
anA,
G4int
aZ,
G4double
aGamma,
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G4VCoulombBarrier
* aCoulombBarrier);
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virtual
~G4EvaporationProbability
();
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inline
G4int
GetZ
(
void
)
const
{
return
theZ; }
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inline
G4int
GetA
(
void
)
const
{
return
theA;}
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protected
:
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// Default constructor
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G4EvaporationProbability
();
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private
:
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// Copy constructor
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G4EvaporationProbability
(
const
G4EvaporationProbability
&
right
);
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const
G4EvaporationProbability
& operator=(
const
G4EvaporationProbability
&
right
);
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G4bool
operator==(
const
G4EvaporationProbability
&
right
)
const
;
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G4bool
operator!=(
const
G4EvaporationProbability
&
right
)
const
;
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public
:
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G4double
ProbabilityDistributionFunction
(
const
G4Fragment
& aFragment,
G4double
K);
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G4double
EmissionProbability
(
const
G4Fragment
& fragment,
G4double
anEnergy);
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private
:
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G4double
CalculateProbability(
const
G4Fragment
& fragment,
G4double
MaximalKineticEnergy );
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G4double
IntegrateEmissionProbability(
const
G4Fragment
& aFragment,
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const
G4double
& Low,
const
G4double
& Up );
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protected
:
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virtual
G4double
CrossSection
(
const
G4Fragment
& fragment,
G4double
K )= 0;
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virtual
G4double
CalcAlphaParam
(
const
G4Fragment
& fragment)=0 ;
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virtual
G4double
CalcBetaParam
(
const
G4Fragment
& fragment)=0 ;
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private
:
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// Data Members
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G4int
theA;
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G4int
theZ;
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// Gamma is A_f(2S_f+1) factor, where A_f is fragment atomic
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// number and S_f is fragment spin
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G4double
Gamma;
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//The Coulomb Barrier
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G4VCoulombBarrier
* theCoulombBarrierptr;
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};
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#endif
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