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9.6.p02
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geant4_9_6_p02
source
processes
hadronic
models
neutron_hp
src
G4NeutronHPProduct.cc
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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// neutron_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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// 080718 As for secondary photons, if its mean value has a value of integer,
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// then a sampling of multiplicity that based on Poisson Distribution
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// is not carried out and the mean is used as a multiplicity.
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// modified by T. Koi.
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// 080721 Using ClearHistories() methodl for limiting the sum of secondary energies
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// modified by T. Koi.
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// 080901 bug fix of too many secnodaries production in nd reactinos by T. Koi
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//
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#include "
G4NeutronHPProduct.hh
"
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#include "
G4Poisson.hh
"
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#include "
G4Proton.hh
"
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G4ReactionProductVector
*
G4NeutronHPProduct::Sample
(
G4double
anEnergy)
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{
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if
(theDist == 0) {
return
0; }
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G4ReactionProductVector
* result =
new
G4ReactionProductVector
;
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G4double
mean = theYield.
GetY
(anEnergy);
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G4int
multi;
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multi =
G4int
(mean+0.0001);
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//if(theMassCode==0) multi = G4Poisson(mean); // @@@@gammas. please X-check this
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//080718
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if
( theMassCode == 0 )
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{
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if
(
G4int
( mean ) == mean )
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{
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multi = (
G4int
) mean;
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}
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else
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{
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multi =
G4Poisson
( mean );
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}
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}
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theDist->
SetTarget
(theTarget);
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theDist->
SetNeutron
(theNeutron);
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G4int
i;
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// G4double eMax = GetTarget()->GetMass()+GetNeutron()->GetMass()
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// - theActualStateQValue;
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theCurrentMultiplicity =
static_cast<
G4int
>
(mean);
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G4ReactionProduct
*
tmp
;
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theDist->
ClearHistories
();
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for
(i=0;i<multi;i++)
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{
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tmp = theDist->
Sample
(anEnergy, theMassCode, theMass);
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if
(tmp != 0) { result->push_back(tmp); }
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}
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if
(multi == 0)
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{
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tmp = theDist->
Sample
(anEnergy, theMassCode, theMass);
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delete
tmp
;
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}
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/*
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//080901 TK Comment out, too many secondaries are produced in deuteron reactions
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if(theTarget->GetMass()<2*GeV) // @@@ take care of residuals in all cases
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{
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tmp = theDist->Sample(anEnergy, theMassCode, theMass);
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tmp->SetDefinition(G4Proton::Proton());
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if(tmp != 0) { result->push_back(tmp); }
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}
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*/
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return
result;
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}
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