source: trunk/source/processes/hadronic/models/neutron_hp/include/G4NeutronHPEnergyDistribution.hh @ 1340

Last change on this file since 1340 was 1340, checked in by garnier, 14 years ago

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27// $Id: G4NeutronHPEnergyDistribution.hh,v 1.11 2007/06/06 12:45:13 ahoward Exp $
28// GEANT4 tag $Name: geant4-09-03-ref-09 $
29//
30#ifndef G4NeutronHPEnergyDistribution_h
31#define G4NeutronHPEnergyDistribution_h 1
32
33#include "globals.hh"
34#include "G4ios.hh"
35#include <fstream>
36#include "G4NeutronHPArbitaryTab.hh"
37#include "G4NeutronHPEvapSpectrum.hh"
38#include "G4NeutronHPSimpleEvapSpectrum.hh"
39#include "G4NeutronHPFissionSpectrum.hh"
40#include "G4NeutronHPWattSpectrum.hh"
41#include "G4NeutronHPMadlandNixSpectrum.hh"
42#include "G4VNeutronHPEDis.hh"
43#include "Randomize.hh"
44
45// we will need a List of these .... one per term.
46
47class G4NeutronHPEnergyDistribution
48{
49  public:
50  G4NeutronHPEnergyDistribution()
51  {
52    theEnergyDistribution = 0;
53    theNumberOfPartials = 0;
54    theRepresentationType = 0;
55  }
56  ~G4NeutronHPEnergyDistribution()
57  {
58    if(theEnergyDistribution != 0)
59    {
60      for(G4int i=0; i<theNumberOfPartials; i++) 
61      {
62        delete theEnergyDistribution[i];
63      }
64      delete [] theEnergyDistribution;
65    }
66  }
67 
68  inline void Init(std::ifstream & theData)
69  {
70    G4double dummy;
71    theData >> dummy >> theNumberOfPartials;
72    theEnergyDistribution = new G4VNeutronHPEDis * [theNumberOfPartials];
73    for(G4int i=0; i<theNumberOfPartials; i++) 
74    {
75      theData >> theRepresentationType;
76      switch(theRepresentationType)
77      {
78        case 1:
79          theEnergyDistribution[i] = new G4NeutronHPArbitaryTab;
80          break;
81        case 5:       
82          theEnergyDistribution[i] = new G4NeutronHPEvapSpectrum;
83          break;
84        case 7:
85          theEnergyDistribution[i] = new G4NeutronHPFissionSpectrum;
86          break;
87        case 9:
88          theEnergyDistribution[i] = new G4NeutronHPSimpleEvapSpectrum;
89          break;
90        case 11:
91          theEnergyDistribution[i] = new G4NeutronHPWattSpectrum;
92          break;
93        case 12:
94          theEnergyDistribution[i] = new G4NeutronHPMadlandNixSpectrum;
95          break;
96      }
97      theEnergyDistribution[i]->Init(theData);
98    }
99  }
100 
101  inline G4double Sample(G4double anEnergy, G4int & it) 
102  {
103    G4double result = 0;
104    it = 0;
105    if (theNumberOfPartials != 0)
106    {
107      G4double sum=0;
108      G4double * running = new G4double[theNumberOfPartials];
109      running[0] = 0;
110      G4int i;
111      for (i=0; i<theNumberOfPartials; i++)
112      { 
113        if (i!=0) running[i]=running[i-1];
114        running[i]+=theEnergyDistribution[i]->GetFractionalProbability(anEnergy);
115      }
116      sum = running[theNumberOfPartials-1];
117      G4double random = G4UniformRand();
118      for(i=0; i<theNumberOfPartials; i++)
119      {
120        it = i;
121        if(running[i]/sum>random) break;
122      }
123      delete [] running;
124      if(it==theNumberOfPartials) it--;
125      result = theEnergyDistribution[it]->Sample(anEnergy);
126    }
127    return result;
128  }
129 
130  private:
131 
132  G4int theNumberOfPartials;
133  G4int theRepresentationType;
134  G4VNeutronHPEDis ** theEnergyDistribution;
135};
136
137#endif
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