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G4GEMProbabilityVI.hh
Go to the documentation of this file.
Or view
the newest version in sPHENIX GitHub for file G4GEMProbabilityVI.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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// GEM de-excitation model
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// by V. Ivanchenko (July 2019)
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//
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#ifndef G4GEMProbabilityVI_h
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#define G4GEMProbabilityVI_h 1
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#include "
G4VEmissionProbability.hh
"
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//const G4int NPOINTSGEM = 10;
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class
G4LevelManager
;
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class
G4GEMProbabilityVI
:
public
G4VEmissionProbability
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{
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public
:
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explicit
G4GEMProbabilityVI
(
G4int
anA,
G4int
aZ,
const
G4LevelManager
*);
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~G4GEMProbabilityVI
()
final
;
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G4double
ComputeTotalProbability
(
const
G4Fragment
&,
G4double
CB);
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// compute probability for evaporated fragment in ground state
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G4double
ComputeProbability
(
G4double
ekin,
G4double
CB)
override
;
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G4Fragment
*
SampleEvaporationFragment
();
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private
:
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// compute probability for evaporated fragment may be excited
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G4double
Integrated2DProbability
();
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// probability as a function of excitations
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G4double
ProbabilityDistributionFunction
(
G4double
exc,
G4double
resExc);
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G4Fragment
*
Sample2DDistribution
();
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G4double
I0
(
G4double
t
);
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G4double
I1
(
G4double
t,
G4double
tx);
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G4double
I2
(
G4double
s0
,
G4double
sx);
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G4double
I3
(
G4double
s0,
G4double
sx);
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// Copy constructor
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G4GEMProbabilityVI
(
const
G4GEMProbabilityVI
&
right
);
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const
G4GEMProbabilityVI
&
operator=
(
const
G4GEMProbabilityVI
&right);
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G4bool
operator==
(
const
G4GEMProbabilityVI
&right)
const
;
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G4bool
operator!=
(
const
G4GEMProbabilityVI
&right)
const
;
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const
G4LevelManager
*
lManager
;
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G4int
fragA
;
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G4int
fragZ
;
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G4double
bCoulomb
;
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G4double
resA13
;
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G4double
U
,
delta0
,
delta1
,
a0
,
a1
;
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G4double
alphaP
,
betaP
;
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G4double
Umax
,
A13
;
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// G4double levelDensity, levelDensity1;
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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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G4double
coeff
;
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G4double
pcoeff
;
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G4double
probmax
;
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G4bool
isExcited
;
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//static const G4double ws[NPOINTSGEM];
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//static const G4double xs[NPOINTSGEM];
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};
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#endif
geant4
tree
geant4-10.6-release
source
processes
hadronic
models
de_excitation
gem_evaporation
include
G4GEMProbabilityVI.hh
Built by
Jin Huang
. updated:
Wed Jun 29 2022 17:25:41
using
1.8.2 with
ECCE GitHub integration