source: trunk/source/processes/hadronic/models/de_excitation/photon_evaporation/src/G4ContinuumGammaTransition.cc @ 1347

Last change on this file since 1347 was 1347, checked in by garnier, 13 years ago

geant4 tag 9.4

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26// $Id: G4ContinuumGammaTransition.cc,v 1.5 2010/11/17 19:17:17 vnivanch Exp $
27// GEANT4 tag $Name: geant4-09-04-ref-00 $
28//
29// -------------------------------------------------------------------
30//      GEANT 4 class file
31//
32//      CERN, Geneva, Switzerland
33//
34//      File name:     G4ContinuumGammaTransition
35//
36//      Authors:       Carlo Dallapiccola (dallapiccola@umdhep.umd.edu)
37//                     Maria Grazia Pia (pia@genova.infn.it)
38//
39//      Creation date: 23 October 1998
40//
41//      Modifications:
42//     
43//        15 April 1999, Alessandro Brunengo (Alessandro.Brunengo@ge.infn.it)
44//              Added creation time evaluation for products of evaporation
45//        02 May 2003,   V. Ivanchenko change interface to G4NuclearlevelManager
46//        06 Oct 2010,   M. Kelsey -- follow changes to G4NuclearLevelManager
47//        17 Nov 2010,   V. Ivanchenko use exponential law for sampling of time
48//                                     and extra cleanup
49// ----------------------------------------------------------------------------
50//
51//  Class G4ContinuumGammaTransition.cc
52//
53
54#include "G4ContinuumGammaTransition.hh"
55#include "G4VLevelDensityParameter.hh"
56#include "G4ConstantLevelDensityParameter.hh"
57#include "G4RandGeneralTmp.hh"
58#include "Randomize.hh"
59#include "G4Pow.hh"
60
61//
62// Constructor
63//
64
65G4ContinuumGammaTransition::G4ContinuumGammaTransition(
66                            const G4NuclearLevelManager* levelManager,
67                            G4int Z, G4int A,
68                            G4double excitation,
69                            G4int verbose):
70  _nucleusA(A), _nucleusZ(Z), _excitation(excitation), _levelManager(levelManager) 
71{
72  G4double eTolerance = 0.;
73  G4int lastButOne = _levelManager->NumberOfLevels() - 2;
74  if (lastButOne >= 0)
75    {
76      eTolerance = (_levelManager->MaxLevelEnergy() -
77                    _levelManager->GetLevel(lastButOne)->Energy());
78      if (eTolerance < 0.) eTolerance = 0.;
79    }
80 
81
82  _verbose = verbose;
83  _eGamma = 0.;
84  _gammaCreationTime = 0.;
85
86  _maxLevelE = _levelManager->MaxLevelEnergy() + eTolerance;
87  _minLevelE = _levelManager->MinLevelEnergy();
88
89  // Energy range for photon generation; upper limit is defined 5*Gamma(GDR) from GDR peak
90  _eMin = 0.001 * MeV;
91  // Giant Dipole Resonance energy
92  G4double energyGDR = (40.3 / G4Pow::GetInstance()->powZ(_nucleusA,0.2) ) * MeV;
93  // Giant Dipole Resonance width
94  G4double widthGDR = 0.30 * energyGDR;
95  // Extend
96  G4double factor = 5;
97  _eMax = energyGDR + factor * widthGDR;
98  if (_eMax > excitation) _eMax = _excitation;
99
100}
101
102//
103// Destructor
104//
105
106G4ContinuumGammaTransition::~G4ContinuumGammaTransition() 
107{}
108
109void G4ContinuumGammaTransition::SelectGamma()
110{
111
112  _eGamma = 0.;
113
114  G4int nBins = 200;
115  G4double sampleArray[200];
116  G4int i;
117  for (i=0; i<nBins; i++)
118    {
119      G4double e = _eMin + ( (_eMax - _eMin) / nBins) * i;
120      sampleArray[i] = E1Pdf(e);
121
122      if(_verbose > 10)
123        G4cout << "*---* G4ContinuumTransition: e = " << e
124               << " pdf = " << sampleArray[i] << G4endl;
125    }
126  G4RandGeneralTmp randGeneral(sampleArray, nBins);
127  G4double random = randGeneral.shoot();
128 
129  _eGamma = _eMin + (_eMax - _eMin) * random;
130 
131  G4double finalExcitation = _excitation - _eGamma;
132 
133  if(_verbose > 10) {
134    G4cout << "*---*---* G4ContinuumTransition: eGamma = " << _eGamma
135           << "   finalExcitation = " << finalExcitation
136           << " random = " << random << G4endl;
137  }
138  //  if (finalExcitation < 0)
139  if(finalExcitation < _minLevelE/2.)
140    {
141      _eGamma = _excitation;
142      finalExcitation = 0.;
143    }
144 
145  if (finalExcitation < _maxLevelE && finalExcitation > 0.) 
146    {
147      G4double levelE = _levelManager->NearestLevel(finalExcitation)->Energy();
148      G4double diff = finalExcitation - levelE;
149      _eGamma = _eGamma + diff;
150    } 
151
152  _gammaCreationTime = GammaTime();
153
154  if(_verbose > 10) {
155    G4cout << "*---*---* G4ContinuumTransition: _gammaCreationTime = "
156           << _gammaCreationTime/second << G4endl;
157  }
158  return; 
159}
160
161G4double G4ContinuumGammaTransition::GetGammaEnergy()
162{
163  return _eGamma;
164}
165
166G4double G4ContinuumGammaTransition::GetGammaCreationTime()
167{
168  return _gammaCreationTime;
169}
170
171
172void G4ContinuumGammaTransition::SetEnergyFrom(G4double energy)
173{
174  if (energy > 0.) _excitation = energy;
175}
176
177
178G4double G4ContinuumGammaTransition::E1Pdf(G4double e)
179{
180  G4double theProb = 0.0;
181  G4double U = std::max(0.0, _excitation - e);
182
183  if(e < 0.0 || _excitation < 0.0) { return theProb; }
184
185  G4ConstantLevelDensityParameter ldPar;
186  G4double aLevelDensityParam = 
187    ldPar.LevelDensityParameter(_nucleusA,_nucleusZ,_excitation);
188
189  //G4double levelDensBef = std::exp(2.0*std::sqrt(aLevelDensityParam*_excitation));
190  //G4double levelDensAft = std::exp(2.0*std::sqrt(aLevelDensityParam*(_excitation - e)));
191  G4double coeff = std::exp(2.0*(std::sqrt(aLevelDensityParam*U) 
192                                 - std::sqrt(aLevelDensityParam*_excitation)));
193
194  //if(_verbose > 20)
195  //  G4cout << _nucleusA << " LevelDensityParameter = " <<  aLevelDensityParam
196  //       << " Bef Aft " << levelDensBef << " " << levelDensAft << G4endl;
197 
198  // Now form the probability density
199
200  // Define constants for the photoabsorption cross-section (the reverse
201  // process of our de-excitation)
202
203  //  G4double sigma0 = 2.5 * _nucleusA * millibarn; 
204  G4double sigma0 = 2.5 * _nucleusA; 
205
206  G4double Egdp = (40.3 /G4Pow::GetInstance()->powZ(_nucleusA,0.2) )*MeV;
207  G4double GammaR = 0.30 * Egdp;
208 
209  const G4double normC = 1.0 / (pi * hbarc)*(pi * hbarc);
210
211  G4double numerator = sigma0 * e*e * GammaR*GammaR;
212  G4double denominator = (e*e - Egdp*Egdp)* (e*e - Egdp*Egdp) + GammaR*GammaR*e*e;
213  //  if (denominator < 1.0e-9) denominator = 1.0e-9;
214
215  G4double sigmaAbs = numerator/denominator ; 
216
217  if(_verbose > 20) {
218    G4cout << ".. " << Egdp << " .. " << GammaR
219           << " .. " << normC << " .. " << sigmaAbs 
220           << " .. " << e*e << " .. " << coeff
221           << G4endl;
222  }
223
224  //  theProb = normC * sigmaAbs * e*e * levelDensAft/levelDensBef;
225  theProb =  sigmaAbs * e*e * coeff;
226
227  return theProb;
228}
229
230
231G4double G4ContinuumGammaTransition::GammaTime()
232{
233
234  G4double GammaR = 0.30 * (40.3 /G4Pow::GetInstance()->powZ(_nucleusA,0.2) )*MeV;
235  G4double tau = hbar_Planck/GammaR;
236  G4double creationTime = -tau*std::log(G4UniformRand());
237  /*
238  G4double tMin = 0;
239  G4double tMax = 10.0 * tau;
240  G4int nBins = 200;
241  G4double sampleArray[200];
242
243  for(G4int i = 0; i<nBins;i++)
244  {
245    G4double t = tMin + ((tMax-tMin)/nBins)*i;
246    sampleArray[i] = (std::exp(-t/tau))/tau;
247  }
248
249  G4RandGeneralTmp randGeneral(sampleArray, nBins);
250  G4double random = randGeneral.shoot();
251 
252  G4double creationTime = tMin + (tMax - tMin) * random;
253  */
254  return creationTime;
255}
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