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G4ParticleHPContEnergyAngular.cc
Go to the documentation of this file.
Or view
the newest version in sPHENIX GitHub for file G4ParticleHPContEnergyAngular.cc
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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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// particle_hp -- source file
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// J.P. Wellisch, Nov-1996
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// A prototype of the low energy neutron transport model.
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//
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// 080721 To be "ClearHistories" effective, the selection scheme of angular distribution is modified by T. Koi
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//
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// P. Arce, Dec-2014 Conversion neutron_hp to particle_hp
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//
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#include "
G4ParticleHPContEnergyAngular.hh
"
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G4ReactionProduct
*
G4ParticleHPContEnergyAngular::Sample
(
G4double
anEnergy,
G4double
massCode,
G4double
/*mass*/
)
37
{
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G4ReactionProduct
* result;
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G4int
i(0);
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G4int
it
(0);
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for
(i=0;i<
nEnergy
;i++)
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{
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it = i;
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#ifdef PHP_AS_HP
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if
(
theAngular
[i].GetEnergy()>anEnergy)
break
;
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#else
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if
(
theAngular
[i].GetEnergy()>=anEnergy)
break
;
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#endif
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}
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if
( std::getenv(
"G4PHPTEST"
) )
G4cout
<< i <<
" G4ParticleHPContEnergyAngular dataE "
<<
theAngular
[i].
GetEnergy
() <<
" > "
<< anEnergy <<
" it_theAngular "
<< it <<
" interpolation "
<<
theInterpolation
<<
G4endl
;
//GDEB
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G4double
targetMass =
GetTarget
()->
GetMass
();
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if
(it==0)
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{
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theAngular
[0].
SetTarget
(
GetTarget
());
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theAngular
[0].
SetTargetCode
(
theTargetCode
);
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theAngular
[0].
SetPrimary
(
GetProjectileRP
());
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result =
theAngular
[0].
Sample
(anEnergy, massCode, targetMass,
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theAngularRep
,
theInterpolation
);
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currentMeanEnergy
.
Put
(
theAngular
[0].
MeanEnergyOfThisInteraction
() );
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}
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else
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{
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// interpolation through alternating sampling. This needs improvement @@@
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// This is the cause of the He3 problem !!!!!!!!
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// See to it, if you can improve this.
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//080714 TK commnet Randomizing use angular distribution
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//080714 TK Always use the upper side distribution. enabling ClearHistories method.
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//G4double random = G4UniformRand();
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//G4double deltaE = theAngular[it].GetEnergy()-theAngular[it-1].GetEnergy();
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//G4double offset = theAngular[it].GetEnergy()-anEnergy;
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//if(random<offset/deltaE) it--;
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//--- create new
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// if( theManager.GetScheme(0) != LINLIN ) { // asserted in G4ParticleHPContEnergyAngular::init there is only one range
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#ifdef PHP_AS_HP
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theAngular
[
it
].
SetTarget
(
GetTarget
());
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theAngular
[
it
].
SetTargetCode
(
theTargetCode
);
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theAngular
[
it
].
SetPrimary
(
GetProjectileRP
());
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result =
theAngular
[
it
].
Sample
(anEnergy, massCode, targetMass,
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theAngularRep
,
theInterpolation
);
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currentMeanEnergy
.
Put
(
theAngular
[it].
MeanEnergyOfThisInteraction
() );
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#else
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if
( std::getenv(
"G4PHPTEST"
) )
G4cout
<< i <<
" G4ParticleHPContEnergyAngular To BUILDBYINTERPOLATION "
<< it <<
" : "
<<
theAngular
[
it
].
GetEnergy
()<<
" , "
<<
theAngular
[
it
].
GetNEnergies
() <<
" "
<< it-1 <<
" : "
<<
theAngular
[it-1].
GetEnergy
()<<
" : "
<<
theAngular
[it-1].
GetNEnergies
() <<
G4endl
;
//GDEB
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// G4ParticleHPContAngularPar * fAngular = new G4ParticleHPContAngularPar(theProjectile ); //fix start
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if
(
fCacheAngular
.
Get
() == NULL) {
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G4ParticleHPContAngularPar
* angpar =
new
G4ParticleHPContAngularPar
(
theProjectile
);
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fCacheAngular
.
Put
(angpar);
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}
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fCacheAngular
.
Get
()->
SetInterpolation
(
theInterpolation
);
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fCacheAngular
.
Get
()->
BuildByInterpolation
( anEnergy,
theManager
.
GetScheme
(0), (
theAngular
[it-1]), (
theAngular
[it]) );
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fCacheAngular
.
Get
()->
SetTarget
(
GetTarget
());
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fCacheAngular
.
Get
()->
SetTargetCode
(
theTargetCode
);
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fCacheAngular
.
Get
()->
SetPrimary
(
GetProjectileRP
());
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result =
fCacheAngular
.
Get
()->
Sample
(anEnergy, massCode, targetMass,
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theAngularRep
,
theInterpolation
);
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currentMeanEnergy
.
Put
(
fCacheAngular
.
Get
()->
MeanEnergyOfThisInteraction
() );
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fCacheAngular
.
Get
()->
ClearHistories
();
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// delete fAngular; //fix end
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#endif
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}
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// G4cout << " 0 0 @@@ G4ParticleHPContEnergyAngular::Sample " << result->GetDefinition()->GetParticleName() << " E= " << result->GetKineticEnergy() << G4endl;//GDEB
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return
result;
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}
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G4double
G4ParticleHPContEnergyAngular::
109
MeanEnergyOfThisInteraction
()
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{
111
G4double
result(0);
112
if
(
currentMeanEnergy
.
Get
()<-1)
113
{
114
throw
G4HadronicException
(__FILE__, __LINE__,
"G4ParticleHPContEnergyAngular: Logical error in Product class"
);
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}
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else
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{
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result =
currentMeanEnergy
.
Get
();
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}
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currentMeanEnergy
.
Put
( -2 );
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return
result;
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}
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void
G4ParticleHPContEnergyAngular::ClearHistories
()
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{
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if
(
theAngular
!= NULL )
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{
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for
(
G4int
i = 0 ; i<
nEnergy
; i++ )
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theAngular
[i].
ClearHistories
();
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}
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}
geant4
tree
geant4-10.6-release
source
processes
hadronic
models
particle_hp
src
G4ParticleHPContEnergyAngular.cc
Built by
Jin Huang
. updated:
Wed Jun 29 2022 17:25:48
using
1.8.2 with
ECCE GitHub integration