source: trunk/source/processes/electromagnetic/lowenergy/src/G4CrossSectionExcitationMillerGreenPartial.cc@ 992

Last change on this file since 992 was 991, checked in by garnier, 17 years ago

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[819]1//
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[991]26// $Id: G4CrossSectionExcitationMillerGreenPartial.cc,v 1.2 2008/07/14 20:47:34 sincerti Exp $
27// GEANT4 tag $Name: geant4-09-02 $
[819]28
29#include "G4CrossSectionExcitationMillerGreenPartial.hh"
30
[961]31//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
[819]32
33G4CrossSectionExcitationMillerGreenPartial::G4CrossSectionExcitationMillerGreenPartial()
34{
35 nLevels = waterExcitation.NumberOfLevels();
36
37 //PROTON
38 kineticEnergyCorrection[0] = 1.;
39 slaterEffectiveCharge[0][0] = 0.;
40 slaterEffectiveCharge[1][0] = 0.;
41 slaterEffectiveCharge[2][0] = 0.;
42 sCoefficient[0][0] = 0.;
43 sCoefficient[1][0] = 0.;
44 sCoefficient[2][0] = 0.;
45
46 //ALPHA++
47 kineticEnergyCorrection[1] = 0.9382723/3.727417;
48 slaterEffectiveCharge[0][1]=0.;
49 slaterEffectiveCharge[1][1]=0.;
50 slaterEffectiveCharge[2][1]=0.;
51 sCoefficient[0][1]=0.;
52 sCoefficient[1][1]=0.;
53 sCoefficient[2][1]=0.;
54
55 // ALPHA+
56 kineticEnergyCorrection[2] = 0.9382723/3.727417;
57 slaterEffectiveCharge[0][2]=2.0;
58 slaterEffectiveCharge[1][2]=1.15;
59 slaterEffectiveCharge[2][2]=1.15;
60 sCoefficient[0][2]=0.7;
61 sCoefficient[1][2]=0.15;
62 sCoefficient[2][2]=0.15;
63
64 // HELIUM
65 kineticEnergyCorrection[3] = 0.9382723/3.727417;
66 slaterEffectiveCharge[0][3]=1.7;
67 slaterEffectiveCharge[1][3]=1.15;
68 slaterEffectiveCharge[2][3]=1.15;
69 sCoefficient[0][3]=0.5;
70 sCoefficient[1][3]=0.25;
71 sCoefficient[2][3]=0.25;
72
73}
74
[961]75//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
76
[819]77G4CrossSectionExcitationMillerGreenPartial::~G4CrossSectionExcitationMillerGreenPartial()
[961]78{}
[819]79
[961]80//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
81
[819]82G4double G4CrossSectionExcitationMillerGreenPartial::CrossSection(G4double k, G4int excitationLevel,
83 const G4ParticleDefinition* particleDefinition)
84{
85 // ( ( z * aj ) ^ omegaj ) * ( t - ej ) ^ nu
86 // sigma(t) = zEff^2 * sigma0 * --------------------------------------------
87 // jj ^ ( omegaj + nu ) + t ^ ( omegaj + nu )
88 //
89 // where t is the kinetic energy corrected by Helium mass over proton mass for Helium ions
90 //
91 // zEff is:
92 // 1 for protons
93 // 2 for alpha++
94 // and 2 - c1 S_1s - c2 S_2s - c3 S_2p for alpha+ and He
95 //
96 // Dingfelder et al., RPC 59, 255-275, 2000 from Miller and Green (1973)
97 // Formula (34) and Table 2
98
99 const G4double sigma0(1.E+8 * barn);
100 const G4double nu(1.);
101 const G4double aj[]={876.*eV, 2084.* eV, 1373.*eV, 692.*eV, 900.*eV};
102 const G4double jj[]={19820.*eV, 23490.*eV, 27770.*eV, 30830.*eV, 33080.*eV};
103 const G4double omegaj[]={0.85, 0.88, 0.88, 0.78, 0.78};
104
105 G4int particleTypeIndex = 0;
106 G4DNAGenericIonsManager* instance;
107 instance = G4DNAGenericIonsManager::Instance();
108
109 if (particleDefinition == G4Proton::ProtonDefinition()) particleTypeIndex=0;
110 if (particleDefinition == instance->GetIon("alpha++")) particleTypeIndex=1;
111 if (particleDefinition == instance->GetIon("alpha+")) particleTypeIndex=2;
112 if (particleDefinition == instance->GetIon("helium")) particleTypeIndex=3;
113
114 G4double tCorrected;
115 tCorrected = k * kineticEnergyCorrection[particleTypeIndex];
116
117 G4int z = 10;
118
119 G4double numerator;
120 numerator = std::pow(z * aj[excitationLevel], omegaj[excitationLevel]) *
121 std::pow(tCorrected - waterExcitation.ExcitationEnergy(excitationLevel), nu);
122
123 G4double power;
124 power = omegaj[excitationLevel] + nu;
125
126 G4double denominator;
127 denominator = std::pow(jj[excitationLevel], power) + std::pow(tCorrected, power);
128
129 G4double zEff = particleDefinition->GetPDGCharge() / eplus + particleDefinition->GetLeptonNumber();
130
131 zEff -= ( sCoefficient[0][particleTypeIndex] * S_1s(k, waterExcitation.ExcitationEnergy(excitationLevel), slaterEffectiveCharge[0][particleTypeIndex], 1.) +
132 sCoefficient[1][particleTypeIndex] * S_2s(k, waterExcitation.ExcitationEnergy(excitationLevel), slaterEffectiveCharge[1][particleTypeIndex], 2.) +
133 sCoefficient[2][particleTypeIndex] * S_2p(k, waterExcitation.ExcitationEnergy(excitationLevel), slaterEffectiveCharge[2][particleTypeIndex], 2.) );
134
135 G4double cross = sigma0 * zEff * zEff * numerator / denominator;
136
137 return cross;
138}
139
[961]140//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
141
[819]142G4int G4CrossSectionExcitationMillerGreenPartial::RandomSelect(G4double k,
143 const G4ParticleDefinition* particle)
144{
145 G4int i = nLevels;
146 G4double value = 0.;
147 std::deque<double> values;
148
[961]149 // ---- MGP ---- The following algorithm is wrong: it works if the cross section
[819]150 // is a monotone increasing function.
151 // The algorithm should be corrected by building the cumulative function
152 // of the cross section and comparing a random number in the range 0-1 against
153 // the cumulative value at each bin
154
155 G4DNAGenericIonsManager *instance;
156 instance = G4DNAGenericIonsManager::Instance();
157
158 // ELECTRON CORRECTION
159
[991]160 if ( particle == instance->GetIon("alpha++"))
[961]161 { while (i > 0)
162 {
[819]163 i--;
164 G4double partial = CrossSection(k,i,particle);
165 values.push_front(partial);
166 value += partial;
[961]167 }
[819]168
[961]169 value *= G4UniformRand();
[819]170
[961]171 i = nLevels;
[819]172
[961]173 while (i > 0)
174 {
[819]175 i--;
176 if (values[i] > value) return i;
177 value -= values[i];
[961]178 }
179 }
[819]180
181 // add ONE or TWO electron-water excitation for alpha+ and helium
182
183 if ( particle == instance->GetIon("alpha+")
184 ||
185 particle == instance->GetIon("helium")
[961]186 )
187 {
188 while (i>0)
[819]189 {
190 i--;
191
192 G4CrossSectionExcitationEmfietzoglouPartial* excitationXS =
193 new G4CrossSectionExcitationEmfietzoglouPartial();
194
195 G4double sigmaExcitation=0;
196 if (k*0.511/3728 > 7.4*eV && k*0.511/3728 < 10*keV) sigmaExcitation = excitationXS->CrossSection(k*0.511/3728,i);
197
198 G4double partial = CrossSection(k,i,particle);
199 if (particle == instance->GetIon("alpha+")) partial = CrossSection(k,i,particle) + sigmaExcitation;
200 if (particle == instance->GetIon("helium")) partial = CrossSection(k,i,particle) + 2*sigmaExcitation;
201 values.push_front(partial);
202 value += partial;
203 delete excitationXS;
[961]204 }
[819]205
[961]206 value*=G4UniformRand();
[819]207
[961]208 i=5;
209 while (i>0)
210 {
[819]211 i--;
212
213 if (values[i]>value) return i;
214
215 value-=values[i];
[961]216 }
217 }
[819]218 //
[961]219
[819]220 return 0;
221}
222
[961]223//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
224
[819]225G4double G4CrossSectionExcitationMillerGreenPartial::Sum(G4double k, const G4ParticleDefinition* particle)
226{
227 G4double totalCrossSection = 0.;
228
229 for (G4int i=0; i<nLevels; i++)
[961]230 {
231 totalCrossSection += CrossSection(k,i,particle);
232 }
[819]233 return totalCrossSection;
234}
235
[961]236//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
[819]237
238G4double G4CrossSectionExcitationMillerGreenPartial::S_1s(G4double t,
239 G4double energyTransferred,
240 G4double slaterEffectiveCharge,
241 G4double shellNumber)
242{
243 // 1 - e^(-2r) * ( 1 + 2 r + 2 r^2)
244 // Dingfelder, in Chattanooga 2005 proceedings, formula (7)
245
246 G4double r = R(t, energyTransferred, slaterEffectiveCharge, shellNumber);
247 G4double value = 1. - std::exp(-2 * r) * ( ( 2. * r + 2. ) * r + 1. );
248
249 return value;
250}
251
252
[961]253//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
254
[819]255G4double G4CrossSectionExcitationMillerGreenPartial::S_2s(G4double t,
256 G4double energyTransferred,
257 G4double slaterEffectiveCharge,
258 G4double shellNumber)
259{
260 // 1 - e^(-2 r) * ( 1 + 2 r + 2 r^2 + 2 r^4)
261 // Dingfelder, in Chattanooga 2005 proceedings, formula (8)
262
263 G4double r = R(t, energyTransferred, slaterEffectiveCharge, shellNumber);
264 G4double value = 1. - std::exp(-2 * r) * (((2. * r * r + 2.) * r + 2.) * r + 1.);
265
266 return value;
267
268}
269
[961]270//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
[819]271
272G4double G4CrossSectionExcitationMillerGreenPartial::S_2p(G4double t,
273 G4double energyTransferred,
274 G4double slaterEffectiveCharge,
275 G4double shellNumber)
276{
277 // 1 - e^(-2 r) * ( 1 + 2 r + 2 r^2 + 4/3 r^3 + 2/3 r^4)
278 // Dingfelder, in Chattanooga 2005 proceedings, formula (9)
279
280 G4double r = R(t, energyTransferred, slaterEffectiveCharge, shellNumber);
281 G4double value = 1. - std::exp(-2 * r) * (((( 2./3. * r + 4./3.) * r + 2.) * r + 2.) * r + 1.);
282
283 return value;
284}
285
[961]286//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
[819]287
288G4double G4CrossSectionExcitationMillerGreenPartial::R(G4double t,
289 G4double energyTransferred,
290 G4double slaterEffectiveCharge,
291 G4double shellNumber)
292{
293 // tElectron = m_electron / m_alpha * t
294 // Hardcoded in Riccardo's implementation; to be corrected
295 // Dingfelder, in Chattanooga 2005 proceedings, p 4
296
297 G4double tElectron = 0.511/3728. * t;
298 G4double value = 2. * tElectron * slaterEffectiveCharge / (energyTransferred * shellNumber);
299
300 return value;
301}
302
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