Import Geant4 0.0.0 source tree
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// This code implementation is the intellectual property of
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// neutron_hp -- header 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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// By copying, distributing or modifying the Program (or any work
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// based on the Program) you indicate your acceptance of this statement,
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// and all its terms.
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//
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// $Id: G4NeutronHPFissionSpectrum.hh,v 2.4 1998/11/07 11:21:16 hpw Exp $
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// GEANT4 tag $Name: geant4-00 $
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//
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#ifndef G4NeutronHPFissionSpectrum_h
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#define G4NeutronHPFissionSpectrum_h 1
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#include "globals.hh"
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#include "G4NeutronHPVector.hh"
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#include "Randomize.hh"
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#include "G4ios.hh"
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#include <fstream.h>
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#include "G4VNeutronHPEDis.hh"
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// we will need a List of these .... one per term.
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class G4NeutronHPFissionSpectrum : public G4VNeutronHPEDis
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{
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public:
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G4NeutronHPFissionSpectrum()
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{
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expm1 = exp(-1.);
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}
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~G4NeutronHPFissionSpectrum()
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{
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}
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inline void Init(ifstream & aDataFile)
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{
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theFractionalProb.Init(aDataFile, eV);
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theThetaDist.Init(aDataFile, eV);
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}
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inline G4double GetFractionalProbability(G4double anEnergy)
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{
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return theFractionalProb.GetY(anEnergy);
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}
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inline G4double Sample(G4double anEnergy)
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{
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G4double theta = theThetaDist.GetY(anEnergy);
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// here we need to sample Maxwells distribution, if
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// need be.
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G4double result, cut;
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G4double range =50*MeV;
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G4double max = Maxwell((theta*eV)/2., theta);
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G4double value;
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do
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{
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result = range*G4UniformRand();
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value = Maxwell(result, theta);
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cut = G4UniformRand();
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}
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while(cut > value/max);
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return result;
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}
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private:
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// this is the function to sample from.
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inline G4double Maxwell(G4double anEnergy, G4double theta)
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{
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G4double result = sqrt(anEnergy/eV)*exp(-anEnergy/eV/theta);
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return result;
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}
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private:
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G4double expm1;
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G4NeutronHPVector theFractionalProb;
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G4NeutronHPVector theThetaDist;
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};
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#endif
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