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G4EvaporationProbability.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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//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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// V.Ivanchenko general clean-up since 2010
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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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class
G4VCoulombBarrier
;
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class
G4EvaporationProbability
:
public
G4VEmissionProbability
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{
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public
:
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explicit
G4EvaporationProbability
(
G4int
anA,
G4int
aZ,
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G4double
aGamma);
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~G4EvaporationProbability
()
override
;
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// general method used for evaporation
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virtual
G4double
TotalProbability
(
const
G4Fragment
& fragment,
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G4double
minKinEnergy,
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G4double
maxKinEnergy,
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G4double
CB,
G4double
exEnergy);
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/*
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virtual G4double TotalProbability(const G4Fragment& fragment,
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G4double minKinEnergy,
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G4double maxKinEnergy,
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G4double CB);
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*/
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// main method to compute full probability for OPTx > 2
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G4double
ComputeProbability
(
G4double
K,
G4double
CB)
override
;
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// Samples fragment kinetic energy and excitation energy
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// of the residual nucleaus
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G4double
SampleKineticEnergy
(
G4double
minKinEnergy,
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G4double
maxKinEnergy,
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G4double
CB);
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protected
:
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virtual
G4double
CalcAlphaParam
(
const
G4Fragment
& fragment);
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virtual
G4double
CalcBetaParam
(
const
G4Fragment
& fragment);
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private
:
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G4double
CrossSection
(
G4double
K,
G4double
CB);
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// Copy constructor
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G4EvaporationProbability
(
const
G4EvaporationProbability
&
right
);
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const
G4EvaporationProbability
&
operator
=
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(
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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//G4int fragA;
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//G4int fragZ;
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G4int
index
;
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G4double
resA13
;
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G4double
muu
;
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G4double
freeU
;
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G4double
a0
;
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G4double
delta1
;
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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
fGamma
;
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G4double
pcoeff
;
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};
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#endif
geant4
tree
geant4-10.6-release
source
processes
hadronic
models
de_excitation
evaporation
include
G4EvaporationProbability.hh
Built by
Jin Huang
. updated:
Wed Jun 29 2022 17:25:41
using
1.8.2 with
ECCE GitHub integration