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25 // 25 //
>> 26 // $Id$
26 // 27 //
27 // 28 //
28 // G4PAIySection.cc -- class implementation fi 29 // G4PAIySection.cc -- class implementation file
29 // 30 //
30 // GEANT 4 class implementation file 31 // GEANT 4 class implementation file
31 // 32 //
32 // For information related to this code, pleas 33 // For information related to this code, please, contact
33 // the Geant4 Collaboration. 34 // the Geant4 Collaboration.
34 // 35 //
35 // R&D: Vladimir.Grichine@cern.ch 36 // R&D: Vladimir.Grichine@cern.ch
36 // 37 //
37 // History: 38 // History:
38 // 39 //
39 // 01.10.07, V.Ivanchenko create using V.Grich 40 // 01.10.07, V.Ivanchenko create using V.Grichine G4PAIxSection class
40 // 26.07.09, V.Ivanchenko added protection for 41 // 26.07.09, V.Ivanchenko added protection for mumerical exceptions for
41 // low-density materials 42 // low-density materials
42 // 21.11.10 V. Grichine bug fixed in Initialis 43 // 21.11.10 V. Grichine bug fixed in Initialise for reading sandia table from
43 // material. Warning: the table is 44 // material. Warning: the table is tuned for photo-effect not PAI model.
44 // 23.06.13 V.Grichine arrays->G4DataVectors <<
45 // 45 //
46 46
47 #include "G4PAIySection.hh" 47 #include "G4PAIySection.hh"
48 48
49 #include "globals.hh" 49 #include "globals.hh"
50 #include "G4PhysicalConstants.hh" 50 #include "G4PhysicalConstants.hh"
51 #include "G4SystemOfUnits.hh" 51 #include "G4SystemOfUnits.hh"
52 #include "G4ios.hh" 52 #include "G4ios.hh"
53 #include "G4Poisson.hh" 53 #include "G4Poisson.hh"
54 #include "G4Material.hh" 54 #include "G4Material.hh"
55 #include "G4MaterialCutsCouple.hh" 55 #include "G4MaterialCutsCouple.hh"
56 #include "G4SandiaTable.hh" 56 #include "G4SandiaTable.hh"
57 #include "G4Exp.hh" <<
58 #include "G4Log.hh" <<
59 57
60 using namespace std; 58 using namespace std;
61 59
62 // Local class constants 60 // Local class constants
63 61
64 const G4double G4PAIySection::fDelta = 0.005; 62 const G4double G4PAIySection::fDelta = 0.005; // energy shift from interval border
65 const G4double G4PAIySection::fError = 0.005; 63 const G4double G4PAIySection::fError = 0.005; // error in lin-log approximation
66 64
67 const G4int G4PAIySection::fMaxSplineSize = 50 65 const G4int G4PAIySection::fMaxSplineSize = 500; // Max size of output spline
68 << 66 // arrays
69 67
70 ////////////////////////////////////////////// 68 //////////////////////////////////////////////////////////////////
71 // 69 //
72 // Constructor 70 // Constructor
73 // 71 //
74 72
75 G4PAIySection::G4PAIySection() 73 G4PAIySection::G4PAIySection()
76 { 74 {
77 fSandia = nullptr; << 75 fSandia = 0;
78 fDensity = fElectronDensity = fNormalization 76 fDensity = fElectronDensity = fNormalizationCof = fLowEnergyCof = 0.0;
79 fIntervalNumber = fSplineNumber = 0; 77 fIntervalNumber = fSplineNumber = 0;
80 fVerbose = 0; 78 fVerbose = 0;
81 << 79 for(G4int i=0; i<500; ++i) {
82 betaBohr = fine_structure_const; << 80 fSplineEnergy[i] = 0.0;
83 G4double cofBetaBohr = 4.0; << 81 fRePartDielectricConst[i] = 0.0;
84 G4double betaBohr2 = fine_structure_const*fi << 82 fImPartDielectricConst[i] = 0.0;
85 betaBohr4 = betaBohr2*betaBohr2*cofBetaBohr; << 83 fIntegralTerm[i] = 0.0;
86 << 84 fDifPAIySection[i] = 0.0;
87 fSplineEnergy = G4DataVector(fMaxSp << 85 fdNdxCerenkov[i] = 0.0;
88 fRePartDielectricConst = G4DataVector(fMaxSp << 86 fdNdxPlasmon[i] = 0.0;
89 fImPartDielectricConst = G4DataVector(fMaxSp << 87 fIntegralPAIySection[i] = 0.0;
90 fIntegralTerm = G4DataVector(fMaxSp << 88 fIntegralPAIdEdx[i] = 0.0;
91 fDifPAIySection = G4DataVector(fMaxSp << 89 fIntegralCerenkov[i] = 0.0;
92 fdNdxCerenkov = G4DataVector(fMaxSp << 90 fIntegralPlasmon[i] = 0.0;
93 fdNdxPlasmon = G4DataVector(fMaxSp << 91 for(G4int j=0; j<112; ++j) { fPAItable[i][j] = 0.0; }
94 fIntegralPAIySection = G4DataVector(fMaxSp <<
95 fIntegralPAIdEdx = G4DataVector(fMaxSp <<
96 fIntegralCerenkov = G4DataVector(fMaxSp <<
97 fIntegralPlasmon = G4DataVector(fMaxSp <<
98 <<
99 for( G4int i = 0; i < 500; ++i ) <<
100 { <<
101 for( G4int j = 0; j < 112; ++j ) { fPAItab <<
102 } 92 }
103 } 93 }
104 94
105 ////////////////////////////////////////////// 95 ////////////////////////////////////////////////////////////////////////////
106 // 96 //
107 // << 97 // Destructor
108 98
109 G4double G4PAIySection::GetLorentzFactor(G4int << 99 G4PAIySection::~G4PAIySection()
110 { << 100 {}
111 return fLorentzFactor[j]; <<
112 } <<
113 101
114 ////////////////////////////////////////////// 102 ////////////////////////////////////////////////////////////////////////
115 // 103 //
116 // Constructor with beta*gamma square value ca << 104 // Test Constructor with beta*gamma square value
117 105
118 void G4PAIySection::Initialize( const G4Materi 106 void G4PAIySection::Initialize( const G4Material* material,
119 G4double maxEn << 107 G4double maxEnergyTransfer,
120 G4double betaG << 108 G4double betaGammaSq)
121 G4SandiaTable* <<
122 { 109 {
123 if(fVerbose > 0) <<
124 { <<
125 G4cout<<G4endl; <<
126 G4cout<<"G4PAIySection::Initialize(...,G4S <<
127 G4cout<<G4endl; <<
128 } <<
129 G4int i, j; 110 G4int i, j;
130 << 111 G4double energy;
131 fSandia = sandia; << 112 // fVerbose = 1;
132 fIntervalNumber = sandia->GetMaxInterval(); <<
133 fDensity = material->GetDensity(); 113 fDensity = material->GetDensity();
134 fElectronDensity = material->GetElectronDens 114 fElectronDensity = material->GetElectronDensity();
>> 115 //G4int numberOfElements = material->GetNumberOfElements();
135 116
136 // fIntervalNumber--; << 117 fSandia = material->GetSandiaTable();
137 118
138 if( fVerbose > 0 ) << 119 fIntervalNumber = fSandia->GetMaxInterval();
139 { << 120
140 G4cout<<"fDensity = "<<fDensity<<"\t"<<fEl << 121 fIntervalNumber--;
141 <<fIntervalNumber<< " (beta*gamma)^2 <<
142 } <<
143 fEnergyInterval = G4DataVector(fIntervalNumb <<
144 fA1 = G4DataVector(fIntervalNumb <<
145 fA2 = G4DataVector(fIntervalNumb <<
146 fA3 = G4DataVector(fIntervalNumb <<
147 fA4 = G4DataVector(fIntervalNumb <<
148 122
149 for( i = 1; i <= fIntervalNumber; ++i ) << 123 for( i = 1; i <= fIntervalNumber; i++ )
150 { 124 {
151 if ( sandia->GetSandiaMatTablePAI(i-1,0) < << 125 energy = fSandia->GetSandiaMatTablePAI(i-1,0); //vmg 20.11.10
152 { << 126
153 fIntervalNumber--; << 127 if( energy >= maxEnergyTransfer || i > fIntervalNumber )
154 continue; <<
155 } <<
156 if( ( sandia->GetSandiaMatTablePAI(i-1,0) <<
157 || i >= fIntervalNumber ) <<
158 { 128 {
159 fEnergyInterval[i] = maxEnergyTransfer; 129 fEnergyInterval[i] = maxEnergyTransfer;
160 fIntervalNumber = i; 130 fIntervalNumber = i;
161 break; 131 break;
162 } 132 }
163 fEnergyInterval[i] = sandia->GetSandiaMatT << 133 fEnergyInterval[i] = energy;
164 fA1[i] = sandia->GetSandiaMatT << 134 fA1[i] = fSandia->GetSandiaMatTablePAI(i-1,1);
165 fA2[i] = sandia->GetSandiaMatT << 135 fA2[i] = fSandia->GetSandiaMatTablePAI(i-1,2);
166 fA3[i] = sandia->GetSandiaMatT << 136 fA3[i] = fSandia->GetSandiaMatTablePAI(i-1,3);
167 fA4[i] = sandia->GetSandiaMatT << 137 fA4[i] = fSandia->GetSandiaMatTablePAI(i-1,4);
168 << 138
169 if( fVerbose > 0 ) { << 139 if( fVerbose > 0 && std::fabs( betaGammaSq - 8. ) < 0.4 )
170 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV< << 140 {
171 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4en << 141 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV<<" keV \t"<<fA1[i]<<"\t"<<fA2[i] <<"\t"<<fA3[i] <<"\t"<<fA4[i]<<G4endl;
172 } 142 }
173 } << 143 }
174 if( fVerbose > 0 ) { << 144
175 G4cout<<"last i = "<<i<<"; "<<"fIntervalNu << 145
176 <<fIntervalNumber<<G4endl; <<
177 } <<
178 if( fEnergyInterval[fIntervalNumber] != maxE 146 if( fEnergyInterval[fIntervalNumber] != maxEnergyTransfer )
179 { 147 {
180 fIntervalNumber++; << 148 fIntervalNumber++;
181 fEnergyInterval[fIntervalNumber] = maxEn << 149 fEnergyInterval[fIntervalNumber] = maxEnergyTransfer;
182 } << 150 fA1[fIntervalNumber] = fA1[fIntervalNumber-1];
183 if( fVerbose > 0 ) << 151 fA2[fIntervalNumber] = fA2[fIntervalNumber-1];
184 { << 152 fA3[fIntervalNumber] = fA3[fIntervalNumber-1];
185 for( i = 1; i <= fIntervalNumber; ++i ) << 153 fA4[fIntervalNumber] = fA4[fIntervalNumber-1];
186 { <<
187 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV< <<
188 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl; <<
189 } <<
190 } <<
191 if( fVerbose > 0 ) { <<
192 G4cout<<"Now checking, if two borders are <<
193 } 154 }
194 for( i = 1; i < fIntervalNumber; ++i ) << 155
>> 156 // Now checking, if two borders are too close together
>> 157 for( i = 1; i < fIntervalNumber; i++ )
195 { 158 {
196 if( fEnergyInterval[i+1]-fEnergyInterval[i << 159 // G4cout<<fEnergyInterval[i]<<"\t"<<fA1[i]<<"\t"<<fA2[i]<<"\t"
197 1.5*fDelta*(fEnergyInterval[i+1]+fEne << 160 // <<fA3[i]<<"\t"<<fA4[i]<<G4endl;
198 else << 161 if(fEnergyInterval[i+1]-fEnergyInterval[i] <
>> 162 1.5*fDelta*(fEnergyInterval[i+1]+fEnergyInterval[i]))
199 { 163 {
200 for( j = i; j < fIntervalNumber; j++ ) 164 for( j = i; j < fIntervalNumber; j++ )
201 { 165 {
202 fEnergyInterval[j] = fEnergyInte << 166 fEnergyInterval[j] = fEnergyInterval[j+1];
203 fA1[j] = fA1[j+1]; << 167 fA1[j] = fA1[j+1];
204 fA2[j] = fA2[j+1]; << 168 fA2[j] = fA2[j+1];
205 fA3[j] = fA3[j+1]; << 169 fA3[j] = fA3[j+1];
206 fA4[j] = fA4[j+1]; << 170 fA4[j] = fA4[j+1];
207 } 171 }
208 fIntervalNumber--; 172 fIntervalNumber--;
>> 173 i--;
209 } 174 }
210 } 175 }
211 if( fVerbose > 0 ) << 176 if( fVerbose > 0 && std::fabs( betaGammaSq - 8. ) < 0.4 )
212 { 177 {
213 for( i = 1; i <= fIntervalNumber; ++i ) << 178 G4cout<<"Sandia cofs in G4PAIySection::Initialize(), mat = "<<material->GetName()<<G4endl;
214 { << 179 G4cout<<"for bg2 = "<<betaGammaSq<<", Tmax = "<< maxEnergyTransfer/keV<<" keV"<<G4endl;
215 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV< << 180 G4cout<<"energy \t"<<"a1 \t"<<"a2 \t"<<"a3 \t"<<"a4 \t"<<G4endl;
216 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl; << 181
217 } << 182 for( j = 1; j < fIntervalNumber; j++ )
>> 183 {
>> 184 G4cout<<j<<"\t"<<fEnergyInterval[j]/keV<<" keV \t"<<fA1[j]<<"\t"<<fA2[j] <<"\t"<<fA3[j] <<"\t"<<fA4[j]<<G4endl;
>> 185 }
218 } 186 }
219 // Preparation of fSplineEnergy array corres <<
220 187
221 ComputeLowEnergyCof(material); << 188 // Preparation of fSplineEnergy array corresponding to min ionisation, G~4
222 << 189
223 G4double betaGammaSqRef = 190 G4double betaGammaSqRef =
224 fLorentzFactor[fRefGammaNumber]*fLorentzFa << 191 fLorentzFactor[fRefGammaNumber]*fLorentzFactor[fRefGammaNumber] - 1;
225 << 192
>> 193 ComputeLowEnergyCof(material);
226 NormShift(betaGammaSqRef); 194 NormShift(betaGammaSqRef);
227 SplainPAI(betaGammaSqRef); 195 SplainPAI(betaGammaSqRef);
228 196
229 // Preparation of integral PAI cross section << 197 // Preparation of integral PAI cross section for input betaGammaSq
230 198
231 for( i = 1; i <= fSplineNumber; ++i ) << 199 for( i = 1; i <= fSplineNumber; i++ )
232 { 200 {
233 fDifPAIySection[i] = DifPAIySection(i,bet << 201 fDifPAIySection[i] = DifPAIySection(i,betaGammaSq);
234 << 202 fdNdxCerenkov[i] = PAIdNdxCerenkov(i,betaGammaSq);
235 if( fVerbose > 0 ) G4cout<<i<<"; dNdxPAI << 203 fdNdxPlasmon[i] = PAIdNdxPlasmon(i,betaGammaSq);
236 } 204 }
237 IntegralPAIySection(); << 205 IntegralPAIySection();
>> 206 IntegralCerenkov();
>> 207 IntegralPlasmon();
238 } 208 }
239 209
240 ////////////////////////////////////////////// 210 /////////////////////////////////////////////////////////////////////////
241 // 211 //
242 // Compute low energy cof. It reduces PAI xsc 212 // Compute low energy cof. It reduces PAI xsc for Lorentz factors less than 4.
243 // 213 //
244 214
245 void G4PAIySection::ComputeLowEnergyCof(const 215 void G4PAIySection::ComputeLowEnergyCof(const G4Material* material)
246 { 216 {
247 G4int i, numberOfElements = (G4int)material- << 217 G4int i, numberOfElements = material->GetNumberOfElements();
248 G4double sumZ = 0., sumCof = 0.; 218 G4double sumZ = 0., sumCof = 0.;
249 219
250 static const G4double p0 = 1.20923e+00; << 220 const G4double p0 = 1.20923e+00;
251 static const G4double p1 = 3.53256e-01; << 221 const G4double p1 = 3.53256e-01;
252 static const G4double p2 = -1.45052e-03; << 222 const G4double p2 = -1.45052e-03;
253 223
254 G4double* thisMaterialZ = new G4double[num 224 G4double* thisMaterialZ = new G4double[numberOfElements];
255 G4double* thisMaterialCof = new G4double[num 225 G4double* thisMaterialCof = new G4double[numberOfElements];
256 226
257 for( i = 0; i < numberOfElements; ++i ) << 227 for( i = 0; i < numberOfElements; i++ )
258 { 228 {
259 thisMaterialZ[i] = material->GetElement(i) 229 thisMaterialZ[i] = material->GetElement(i)->GetZ();
260 sumZ += thisMaterialZ[i]; 230 sumZ += thisMaterialZ[i];
261 thisMaterialCof[i] = p0+p1*thisMaterialZ[i 231 thisMaterialCof[i] = p0+p1*thisMaterialZ[i]+p2*thisMaterialZ[i]*thisMaterialZ[i];
262 } 232 }
263 for( i = 0; i < numberOfElements; ++i ) << 233 for( i = 0; i < numberOfElements; i++ )
264 { 234 {
265 sumCof += thisMaterialCof[i]*thisMaterialZ 235 sumCof += thisMaterialCof[i]*thisMaterialZ[i]/sumZ;
266 } 236 }
267 fLowEnergyCof = sumCof; 237 fLowEnergyCof = sumCof;
268 delete [] thisMaterialZ; 238 delete [] thisMaterialZ;
269 delete [] thisMaterialCof; 239 delete [] thisMaterialCof;
270 // G4cout<<"fLowEnergyCof = "<<fLowEnergyCof 240 // G4cout<<"fLowEnergyCof = "<<fLowEnergyCof<<G4endl;
271 } 241 }
272 242
>> 243
>> 244
>> 245
273 ////////////////////////////////////////////// 246 /////////////////////////////////////////////////////////////////////////
274 // 247 //
275 // General control function for class G4PAIySe 248 // General control function for class G4PAIySection
276 // 249 //
277 250
278 void G4PAIySection::InitPAI() 251 void G4PAIySection::InitPAI()
279 { 252 {
280 G4int i; 253 G4int i;
281 G4double betaGammaSq = fLorentzFactor[fRefG 254 G4double betaGammaSq = fLorentzFactor[fRefGammaNumber]*
282 fLorentzFactor[fRefG 255 fLorentzFactor[fRefGammaNumber] - 1;
283 256
284 // Preparation of integral PAI cross sectio 257 // Preparation of integral PAI cross section for reference gamma
285 258
286 NormShift(betaGammaSq); 259 NormShift(betaGammaSq);
287 SplainPAI(betaGammaSq); 260 SplainPAI(betaGammaSq);
288 261
289 IntegralPAIySection(); 262 IntegralPAIySection();
290 IntegralCerenkov(); 263 IntegralCerenkov();
291 IntegralPlasmon(); 264 IntegralPlasmon();
292 265
293 for( i = 0; i<= fSplineNumber; ++i) << 266 for(i = 0; i<=fSplineNumber; i++)
294 { 267 {
295 fPAItable[i][fRefGammaNumber] = fIntegral << 268 fPAItable[i][fRefGammaNumber] = fIntegralPAIySection[i];
296 << 269 if(i != 0)
297 if(i != 0) fPAItable[i][0] = fSplineEner << 270 {
>> 271 fPAItable[i][0] = fSplineEnergy[i];
>> 272 }
298 } 273 }
299 fPAItable[0][0] = fSplineNumber; 274 fPAItable[0][0] = fSplineNumber;
300 275
301 for( G4int j = 1; j < 112; ++j) // fo << 276 for(G4int j = 1; j < 112; j++) // for other gammas
302 { 277 {
303 if( j == fRefGammaNumber ) continue; 278 if( j == fRefGammaNumber ) continue;
304 279
305 betaGammaSq = fLorentzFactor[j]*fLorentz 280 betaGammaSq = fLorentzFactor[j]*fLorentzFactor[j] - 1;
306 281
307 for(i = 1; i <= fSplineNumber; ++i) << 282 for(i = 1; i <= fSplineNumber; i++)
308 { 283 {
309 fDifPAIySection[i] = DifPAIySection(i 284 fDifPAIySection[i] = DifPAIySection(i,betaGammaSq);
310 fdNdxCerenkov[i] = PAIdNdxCerenkov( 285 fdNdxCerenkov[i] = PAIdNdxCerenkov(i,betaGammaSq);
311 fdNdxPlasmon[i] = PAIdNdxPlasmon(i 286 fdNdxPlasmon[i] = PAIdNdxPlasmon(i,betaGammaSq);
312 } 287 }
313 IntegralPAIySection(); 288 IntegralPAIySection();
314 IntegralCerenkov(); 289 IntegralCerenkov();
315 IntegralPlasmon(); 290 IntegralPlasmon();
316 291
317 for(i = 0; i <= fSplineNumber; ++i) << 292 for(i = 0; i <= fSplineNumber; i++)
318 { 293 {
319 fPAItable[i][j] = fIntegralPAIySection << 294 fPAItable[i][j] = fIntegralPAIySection[i];
320 } 295 }
321 } 296 }
>> 297
322 } 298 }
323 299
324 ////////////////////////////////////////////// 300 ///////////////////////////////////////////////////////////////////////
325 // 301 //
326 // Shifting from borders to intervals Creation 302 // Shifting from borders to intervals Creation of first energy points
327 // 303 //
328 304
329 void G4PAIySection::NormShift(G4double betaGam 305 void G4PAIySection::NormShift(G4double betaGammaSq)
330 { 306 {
331 G4int i, j; 307 G4int i, j;
332 308
333 for( i = 1; i <= fIntervalNumber-1; ++i) << 309 for( i = 1; i <= fIntervalNumber-1; i++ )
334 { 310 {
335 for( j = 1; j <= 2; ++j) << 311 for( j = 1; j <= 2; j++ )
336 { 312 {
337 fSplineNumber = (i-1)*2 + j; 313 fSplineNumber = (i-1)*2 + j;
338 314
339 if( j == 1 ) fSplineEnergy[fSplineNumber 315 if( j == 1 ) fSplineEnergy[fSplineNumber] = fEnergyInterval[i ]*(1+fDelta);
340 else fSplineEnergy[fSplineNumber 316 else fSplineEnergy[fSplineNumber] = fEnergyInterval[i+1]*(1-fDelta);
341 // G4cout<<"cn = "<<fSplineNumber<<"; 317 // G4cout<<"cn = "<<fSplineNumber<<"; "<<"energy = "
342 // <<fSplineEnergy[fSplineNumber]<<G4en 318 // <<fSplineEnergy[fSplineNumber]<<G4endl;
343 } 319 }
344 } 320 }
345 fIntegralTerm[1]=RutherfordIntegral(1,fEnerg 321 fIntegralTerm[1]=RutherfordIntegral(1,fEnergyInterval[1],fSplineEnergy[1]);
346 322
347 j = 1; 323 j = 1;
348 324
349 for(i=2;i<=fSplineNumber;++i) << 325 for(i=2;i<=fSplineNumber;i++)
350 { 326 {
351 if(fSplineEnergy[i]<fEnergyInterval[j+1]) 327 if(fSplineEnergy[i]<fEnergyInterval[j+1])
352 { 328 {
353 fIntegralTerm[i] = fIntegralTerm[i-1] 329 fIntegralTerm[i] = fIntegralTerm[i-1] +
354 RutherfordIntegral << 330 RutherfordIntegral(j,fSplineEnergy[i-1],
355 331 fSplineEnergy[i] );
356 } 332 }
357 else 333 else
358 { 334 {
359 G4double x = RutherfordIntegral(j,fSpli 335 G4double x = RutherfordIntegral(j,fSplineEnergy[i-1],
360 fEn 336 fEnergyInterval[j+1] );
361 j++; 337 j++;
362 fIntegralTerm[i] = fIntegralTerm[i-1] 338 fIntegralTerm[i] = fIntegralTerm[i-1] + x +
363 RutherfordIntegral << 339 RutherfordIntegral(j,fEnergyInterval[j],
364 340 fSplineEnergy[i] );
365 } 341 }
366 // G4cout<<i<<"\t"<<fSplineEnergy[i]<<"\t" 342 // G4cout<<i<<"\t"<<fSplineEnergy[i]<<"\t"<<fIntegralTerm[i]<<"\n"<<G4endl;
367 } 343 }
368 static const G4double nfactor = << 344 fNormalizationCof = 2*pi*pi*hbarc*hbarc*fine_structure_const/electron_mass_c2;
369 2*pi*pi*hbarc*hbarc*fine_structure_const/e << 345 fNormalizationCof *= fElectronDensity/fIntegralTerm[fSplineNumber];
370 fNormalizationCof = nfactor*fElectronDensity <<
371 346
372 // G4cout<<"fNormalizationCof = "<<fNormaliz 347 // G4cout<<"fNormalizationCof = "<<fNormalizationCof<<G4endl;
373 348
374 // Calculation of PAI differrential cross-se << 349 // Calculation of PAI differrential cross-section (1/(keV*cm))
375 // in the energy points near borders of ener << 350 // in the energy points near borders of energy intervals
376 351
377 for(G4int k=1; k<=fIntervalNumber-1; ++k) << 352 for(G4int k=1;k<=fIntervalNumber-1;k++)
378 { 353 {
379 for(j=1; j<=2; ++j) << 354 for(j=1;j<=2;j++)
380 { 355 {
381 i = (k-1)*2 + j; 356 i = (k-1)*2 + j;
382 fImPartDielectricConst[i] = fNormaliz 357 fImPartDielectricConst[i] = fNormalizationCof*
383 ImPartDie << 358 ImPartDielectricConst(k,fSplineEnergy[i]);
384 fRePartDielectricConst[i] = fNormaliz 359 fRePartDielectricConst[i] = fNormalizationCof*
385 RePartDie << 360 RePartDielectricConst(fSplineEnergy[i]);
386 fIntegralTerm[i] *= fNormalizationCof 361 fIntegralTerm[i] *= fNormalizationCof;
387 362
388 fDifPAIySection[i] = DifPAIySection(i 363 fDifPAIySection[i] = DifPAIySection(i,betaGammaSq);
389 fdNdxCerenkov[i] = PAIdNdxCerenkov( 364 fdNdxCerenkov[i] = PAIdNdxCerenkov(i,betaGammaSq);
390 fdNdxPlasmon[i] = PAIdNdxPlasmon(i 365 fdNdxPlasmon[i] = PAIdNdxPlasmon(i,betaGammaSq);
391 } 366 }
392 } 367 }
393 368
394 } // end of NormShift 369 } // end of NormShift
395 370
396 ////////////////////////////////////////////// 371 /////////////////////////////////////////////////////////////////////////
397 // 372 //
398 // Creation of new energy points as geometrica 373 // Creation of new energy points as geometrical mean of existing
399 // one, calculation PAI_cs for them, while the 374 // one, calculation PAI_cs for them, while the error of logarithmic
400 // linear approximation would be smaller than 375 // linear approximation would be smaller than 'fError'
401 376
402 void G4PAIySection::SplainPAI(G4double betaGam 377 void G4PAIySection::SplainPAI(G4double betaGammaSq)
403 { 378 {
404 G4int k = 1; 379 G4int k = 1;
405 G4int i = 1; 380 G4int i = 1;
406 381
407 while ( (i < fSplineNumber) && (fSplineNumb 382 while ( (i < fSplineNumber) && (fSplineNumber < fMaxSplineSize-1) )
408 { 383 {
409 if(fSplineEnergy[i+1] > fEnergyInterval[ 384 if(fSplineEnergy[i+1] > fEnergyInterval[k+1])
410 { 385 {
411 k++; // Here next energy point is 386 k++; // Here next energy point is in next energy interval
412 ++i; << 387 i++;
413 continue; 388 continue;
414 } 389 }
415 // Shifting of arrayes for inserting the << 390 // Shifting of arrayes for inserting the geometrical
416 // average of 'i' and 'i+1' energy point << 391 // average of 'i' and 'i+1' energy points to 'i+1' place
417 fSplineNumber++; 392 fSplineNumber++;
418 393
419 for(G4int j = fSplineNumber; j >= i+2; j 394 for(G4int j = fSplineNumber; j >= i+2; j-- )
420 { 395 {
421 fSplineEnergy[j] = fSplineEn 396 fSplineEnergy[j] = fSplineEnergy[j-1];
422 fImPartDielectricConst[j] = fImPartDi 397 fImPartDielectricConst[j] = fImPartDielectricConst[j-1];
423 fRePartDielectricConst[j] = fRePartDi << 398 fRePartDielectricConst[j] = fRePartDielectricConst[j-1];
424 fIntegralTerm[j] = fIntegral << 399 fIntegralTerm[j] = fIntegralTerm[j-1];
425 400
426 fDifPAIySection[j] = fDifPAIySection[ << 401 fDifPAIySection[j] = fDifPAIySection[j-1];
427 fdNdxCerenkov[j] = fdNdxCerenkov[j- 402 fdNdxCerenkov[j] = fdNdxCerenkov[j-1];
428 fdNdxPlasmon[j] = fdNdxPlasmon[j-1 403 fdNdxPlasmon[j] = fdNdxPlasmon[j-1];
429 } 404 }
430 G4double x1 = fSplineEnergy[i]; 405 G4double x1 = fSplineEnergy[i];
431 G4double x2 = fSplineEnergy[i+1]; 406 G4double x2 = fSplineEnergy[i+1];
432 G4double yy1 = fDifPAIySection[i]; 407 G4double yy1 = fDifPAIySection[i];
433 G4double y2 = fDifPAIySection[i+1]; 408 G4double y2 = fDifPAIySection[i+1];
434 409
435 G4double en1 = sqrt(x1*x2); 410 G4double en1 = sqrt(x1*x2);
436 fSplineEnergy[i+1] = en1; 411 fSplineEnergy[i+1] = en1;
437 412
438 // Calculation of logarithmic linear app << 413 // Calculation of logarithmic linear approximation
439 // in this (enr) energy point, which num << 414 // in this (enr) energy point, which number is 'i+1' now
440 415
441 G4double a = log10(y2/yy1)/log10(x2/x1); 416 G4double a = log10(y2/yy1)/log10(x2/x1);
442 G4double b = log10(yy1) - a*log10(x1); 417 G4double b = log10(yy1) - a*log10(x1);
443 G4double y = a*log10(en1) + b; 418 G4double y = a*log10(en1) + b;
444 y = pow(10.,y); 419 y = pow(10.,y);
445 420
446 // Calculation of the PAI dif. cross-sec << 421 // Calculation of the PAI dif. cross-section at this point
447 422
448 fImPartDielectricConst[i+1] = fNormaliza 423 fImPartDielectricConst[i+1] = fNormalizationCof*
449 ImPartDiel << 424 ImPartDielectricConst(k,fSplineEnergy[i+1]);
450 fRePartDielectricConst[i+1] = fNormaliza 425 fRePartDielectricConst[i+1] = fNormalizationCof*
451 RePartDiel << 426 RePartDielectricConst(fSplineEnergy[i+1]);
452 fIntegralTerm[i+1] = fIntegralTerm[i] + 427 fIntegralTerm[i+1] = fIntegralTerm[i] + fNormalizationCof*
453 RutherfordIntegral( << 428 RutherfordIntegral(k,fSplineEnergy[i],
454 429 fSplineEnergy[i+1]);
455 430
456 fDifPAIySection[i+1] = DifPAIySection(i+ 431 fDifPAIySection[i+1] = DifPAIySection(i+1,betaGammaSq);
457 fdNdxCerenkov[i+1] = PAIdNdxCerenkov(i 432 fdNdxCerenkov[i+1] = PAIdNdxCerenkov(i+1,betaGammaSq);
458 fdNdxPlasmon[i+1] = PAIdNdxPlasmon(i+ 433 fdNdxPlasmon[i+1] = PAIdNdxPlasmon(i+1,betaGammaSq);
459 434
460 // Condition for next divisi << 435 // Condition for next division of this segment or to pass
461 // to higher energies << 436 // to higher energies
462 437
463 G4double x = 2*(fDifPAIySection[i+1] - y 438 G4double x = 2*(fDifPAIySection[i+1] - y)/(fDifPAIySection[i+1] + y);
464 439
465 G4double delta = 2.*(fSplineEnergy[i+1]- <<
466 /(fSplineEnergy[i+1]+fSplineEnergy[i]) <<
467 <<
468 if( x < 0 ) 440 if( x < 0 )
469 { 441 {
470 x = -x; << 442 x = -x;
471 } 443 }
472 if( x > fError && fSplineNumber < fMaxSp << 444 if( x > fError && fSplineNumber < fMaxSplineSize-1 )
473 { 445 {
474 continue; // next division << 446 continue; // next division
475 } 447 }
476 i += 2; // pass to next segment 448 i += 2; // pass to next segment
477 449
478 // Loop checking, 03-Aug-2015, Vladimir <<
479 } // close 'while' 450 } // close 'while'
480 451
481 } // end of SplainPAI 452 } // end of SplainPAI
482 453
483 454
484 ////////////////////////////////////////////// 455 ////////////////////////////////////////////////////////////////////
485 // 456 //
486 // Integration over electrons that could be co 457 // Integration over electrons that could be considered
487 // quasi-free at energy transfer of interest 458 // quasi-free at energy transfer of interest
488 459
489 G4double G4PAIySection::RutherfordIntegral( G4 460 G4double G4PAIySection::RutherfordIntegral( G4int k,
490 G4 << 461 G4double x1,
491 << 462 G4double x2 )
492 { 463 {
493 G4double c1, c2, c3; 464 G4double c1, c2, c3;
494 // G4cout<<"RI: x1 = "<<x1<<"; "<<"x2 = "<< << 465 // G4cout<<"RI: x1 = "<<x1<<"; "<<"x2 = "<<x2<<G4endl;
495 G4double x12 = x1*x2; << 466 c1 = (x2 - x1)/x1/x2;
496 c1 = (x2 - x1)/x12; << 467 c2 = (x2 - x1)*(x2 + x1)/x1/x1/x2/x2;
497 c2 = (x2 - x1)*(x2 + x1)/(x12*x12); << 468 c3 = (x2 - x1)*(x1*x1 + x1*x2 + x2*x2)/x1/x1/x1/x2/x2/x2;
498 c3 = (x2 - x1)*(x1*x1 + x1*x2 + x2*x2)/(x12 <<
499 // G4cout<<" RI: c1 = "<<c1<<"; "<<"c2 = "< 469 // G4cout<<" RI: c1 = "<<c1<<"; "<<"c2 = "<<c2<<"; "<<"c3 = "<<c3<<G4endl;
500 470
501 return fA1[k]*log(x2/x1) + fA2[k]*c1 + fA3 471 return fA1[k]*log(x2/x1) + fA2[k]*c1 + fA3[k]*c2/2 + fA4[k]*c3/3;
502 472
503 } // end of RutherfordIntegral 473 } // end of RutherfordIntegral
504 474
505 475
506 ////////////////////////////////////////////// 476 /////////////////////////////////////////////////////////////////
507 // 477 //
508 // Imaginary part of dielectric constant 478 // Imaginary part of dielectric constant
509 // (G4int k - interval number, G4double en1 - 479 // (G4int k - interval number, G4double en1 - energy point)
510 480
511 G4double G4PAIySection::ImPartDielectricConst( << 481 G4double G4PAIySection::ImPartDielectricConst( G4int k ,
>> 482 G4double energy1 )
512 { 483 {
513 G4double energy2,energy3,energy4,result; 484 G4double energy2,energy3,energy4,result;
514 485
515 energy2 = energy1*energy1; 486 energy2 = energy1*energy1;
516 energy3 = energy2*energy1; 487 energy3 = energy2*energy1;
517 energy4 = energy3*energy1; 488 energy4 = energy3*energy1;
518 489
519 result = fA1[k]/energy1+fA2[k]/energy2+fA3[ 490 result = fA1[k]/energy1+fA2[k]/energy2+fA3[k]/energy3+fA4[k]/energy4;
520 result *=hbarc/energy1; 491 result *=hbarc/energy1;
521 492
522 return result; 493 return result;
523 494
524 } // end of ImPartDielectricConst 495 } // end of ImPartDielectricConst
525 496
526 497
527 ////////////////////////////////////////////// 498 //////////////////////////////////////////////////////////////////////////////
528 // 499 //
529 // Real part of dielectric constant minus unit 500 // Real part of dielectric constant minus unit: epsilon_1 - 1
530 // (G4double enb - energy point) 501 // (G4double enb - energy point)
531 // 502 //
532 503
533 G4double G4PAIySection::RePartDielectricConst( 504 G4double G4PAIySection::RePartDielectricConst(G4double enb)
534 { 505 {
535 G4double x0, x02, x03, x04, x05, x1, x2, xx 506 G4double x0, x02, x03, x04, x05, x1, x2, xx1 ,xx2 , xx12,
536 c1, c2, c3, cof1, cof2, xln1, xln2 507 c1, c2, c3, cof1, cof2, xln1, xln2, xln3, result;
537 508
538 x0 = enb; 509 x0 = enb;
539 result = 0; 510 result = 0;
540 511
541 for(G4int i=1;i<=fIntervalNumber-1;++i) << 512 for(G4int i=1;i<=fIntervalNumber-1;i++)
542 { 513 {
543 x1 = fEnergyInterval[i]; 514 x1 = fEnergyInterval[i];
544 x2 = fEnergyInterval[i+1]; 515 x2 = fEnergyInterval[i+1];
545 xx1 = x1 - x0; 516 xx1 = x1 - x0;
546 xx2 = x2 - x0; 517 xx2 = x2 - x0;
547 xx12 = xx2/xx1; 518 xx12 = xx2/xx1;
548 519
549 if(xx12<0.) << 520 if(xx12<0)
550 { 521 {
551 xx12 = -xx12; << 522 xx12 = -xx12;
552 } 523 }
553 xln1 = log(x2/x1); 524 xln1 = log(x2/x1);
554 xln2 = log(xx12); 525 xln2 = log(xx12);
555 xln3 = log((x2 + x0)/(x1 + x0)); 526 xln3 = log((x2 + x0)/(x1 + x0));
556 x02 = x0*x0; 527 x02 = x0*x0;
557 x03 = x02*x0; 528 x03 = x02*x0;
558 x04 = x03*x0; 529 x04 = x03*x0;
559 x05 = x04*x0; 530 x05 = x04*x0;
560 G4double x12 = x1*x2; << 531 c1 = (x2 - x1)/x1/x2;
561 c1 = (x2 - x1)/x12; << 532 c2 = (x2 - x1)*(x2 +x1)/x1/x1/x2/x2;
562 c2 = (x2 - x1)*(x2 +x1)/(x12*x12); << 533 c3 = (x2 -x1)*(x1*x1 + x1*x2 + x2*x2)/x1/x1/x1/x2/x2/x2;
563 c3 = (x2 -x1)*(x1*x1 + x1*x2 + x2*x2)/( <<
564 534
565 result -= (fA1[i]/x02 + fA3[i]/x04)*xln1 535 result -= (fA1[i]/x02 + fA3[i]/x04)*xln1;
566 result -= (fA2[i]/x02 + fA4[i]/x04)*c1; 536 result -= (fA2[i]/x02 + fA4[i]/x04)*c1;
567 result -= fA3[i]*c2/2/x02; 537 result -= fA3[i]*c2/2/x02;
568 result -= fA4[i]*c3/3/x02; 538 result -= fA4[i]*c3/3/x02;
569 539
570 cof1 = fA1[i]/x02 + fA3[i]/x04; 540 cof1 = fA1[i]/x02 + fA3[i]/x04;
571 cof2 = fA2[i]/x03 + fA4[i]/x05; 541 cof2 = fA2[i]/x03 + fA4[i]/x05;
572 542
573 result += 0.5*(cof1 +cof2)*xln2; 543 result += 0.5*(cof1 +cof2)*xln2;
574 result += 0.5*(cof1 - cof2)*xln3; 544 result += 0.5*(cof1 - cof2)*xln3;
575 } 545 }
576 result *= 2*hbarc/pi; 546 result *= 2*hbarc/pi;
577 547
578 return result; 548 return result;
579 549
580 } // end of RePartDielectricConst 550 } // end of RePartDielectricConst
581 551
582 ////////////////////////////////////////////// 552 //////////////////////////////////////////////////////////////////////
583 // 553 //
584 // PAI differential cross-section in terms of 554 // PAI differential cross-section in terms of
585 // simplified Allison's equation 555 // simplified Allison's equation
586 // 556 //
587 557
588 G4double G4PAIySection::DifPAIySection( G4int 558 G4double G4PAIySection::DifPAIySection( G4int i ,
589 G4doub 559 G4double betaGammaSq )
590 { 560 {
591 G4double beta, be2,cof,x1,x2,x3,x4,x5,x6,x7 << 561 G4double beta, be2,cof,x1,x2,x3,x4,x5,x6,x7,x8,result;
>> 562 //G4double beta, be4;
>> 563 //G4double be4;
>> 564 G4double betaBohr = fine_structure_const;
>> 565 // G4double betaBohr2 = fine_structure_const*fine_structure_const;
>> 566 // G4double betaBohr4 = betaBohr2*betaBohr2*4.0;
592 be2 = betaGammaSq/(1 + betaGammaSq); 567 be2 = betaGammaSq/(1 + betaGammaSq);
593 beta = std::sqrt(be2); << 568 //be4 = be2*be2;
>> 569 beta = sqrt(be2);
594 cof = 1; 570 cof = 1;
595 x1 = log(2*electron_mass_c2/fSplineEnergy[i 571 x1 = log(2*electron_mass_c2/fSplineEnergy[i]);
596 572
597 if( betaGammaSq < 0.01 ) x2 = log(be2); 573 if( betaGammaSq < 0.01 ) x2 = log(be2);
598 else 574 else
599 { 575 {
600 x2 = -log( (1/betaGammaSq - fRePartDielec 576 x2 = -log( (1/betaGammaSq - fRePartDielectricConst[i])*
601 (1/betaGammaSq - fRePartDielec << 577 (1/betaGammaSq - fRePartDielectricConst[i]) +
602 fImPartDielectricConst[i]*fImP << 578 fImPartDielectricConst[i]*fImPartDielectricConst[i] )/2;
603 } 579 }
604 if( fImPartDielectricConst[i] == 0.0 ||beta 580 if( fImPartDielectricConst[i] == 0.0 ||betaGammaSq < 0.01 )
605 { 581 {
606 x6=0; 582 x6=0;
607 } 583 }
608 else 584 else
609 { 585 {
610 x3 = -fRePartDielectricConst[i] + 1/betaG 586 x3 = -fRePartDielectricConst[i] + 1/betaGammaSq;
611 x5 = -1 - fRePartDielectricConst[i] + 587 x5 = -1 - fRePartDielectricConst[i] +
612 be2*((1 +fRePartDielectricConst[i])* 588 be2*((1 +fRePartDielectricConst[i])*(1 + fRePartDielectricConst[i]) +
613 fImPartDielectricConst[i]*fImPartDie << 589 fImPartDielectricConst[i]*fImPartDielectricConst[i]);
614 590
615 x7 = std::atan2(fImPartDielectricConst[i] << 591 x7 = atan2(fImPartDielectricConst[i],x3);
616 x6 = x5 * x7; 592 x6 = x5 * x7;
617 } 593 }
>> 594 // if(fImPartDielectricConst[i] == 0) x6 = 0;
>> 595
618 x4 = ((x1 + x2)*fImPartDielectricConst[i] + 596 x4 = ((x1 + x2)*fImPartDielectricConst[i] + x6)/hbarc;
>> 597 // if( x4 < 0.0 ) x4 = 0.0;
619 x8 = (1 + fRePartDielectricConst[i])*(1 + f 598 x8 = (1 + fRePartDielectricConst[i])*(1 + fRePartDielectricConst[i]) +
620 fImPartDielectricConst[i]*fImPartDiele 599 fImPartDielectricConst[i]*fImPartDielectricConst[i];
621 600
622 result = (x4 + cof*fIntegralTerm[i]/fSpline 601 result = (x4 + cof*fIntegralTerm[i]/fSplineEnergy[i]/fSplineEnergy[i]);
623 result = std::max(result, 1.0e-8); << 602 if(result < 1.0e-8) result = 1.0e-8;
624 result *= fine_structure_const/(be2*pi); << 603 result *= fine_structure_const/be2/pi;
625 // low energy correction 604 // low energy correction
626 605
627 G4double lowCof = fLowEnergyCof; // 6.0 ; / 606 G4double lowCof = fLowEnergyCof; // 6.0 ; // Ar ~ 4.; -> fLowCof as f(Z1,Z2)?
628 607
629 result *= (1 - std::exp(-beta/(betaBohr*low << 608 result *= (1 - exp(-beta/betaBohr/lowCof));
>> 609
>> 610 // result *= (1-exp(-beta/betaBohr))*(1-exp(-beta/betaBohr));
>> 611 // result *= (1-exp(-be2/betaBohr2));
>> 612 // result *= (1-exp(-be4/betaBohr4));
>> 613 // if(fDensity >= 0.1)
630 if(x8 > 0.) 614 if(x8 > 0.)
631 { 615 {
632 result /= x8; << 616 result /= x8;
633 } 617 }
634 return result; 618 return result;
635 619
636 } // end of DifPAIySection 620 } // end of DifPAIySection
637 621
638 ////////////////////////////////////////////// 622 //////////////////////////////////////////////////////////////////////////
639 // 623 //
640 // Calculation od dN/dx of collisions with cre 624 // Calculation od dN/dx of collisions with creation of Cerenkov pseudo-photons
641 625
642 G4double G4PAIySection::PAIdNdxCerenkov( G4int << 626 G4double G4PAIySection::PAIdNdxCerenkov( G4int i ,
>> 627 G4double betaGammaSq )
643 { 628 {
644 G4double logarithm, x3, x5, argument, modul 629 G4double logarithm, x3, x5, argument, modul2, dNdxC;
645 G4double be2, be4; << 630 G4double be2, be4, betaBohr2,betaBohr4,cofBetaBohr;
>> 631
>> 632 //G4double cof = 1.0;
>> 633 cofBetaBohr = 4.0;
>> 634 betaBohr2 = fine_structure_const*fine_structure_const;
>> 635 betaBohr4 = betaBohr2*betaBohr2*cofBetaBohr;
646 636
647 be2 = betaGammaSq/(1 + betaGammaSq); 637 be2 = betaGammaSq/(1 + betaGammaSq);
648 be4 = be2*be2; 638 be4 = be2*be2;
649 639
650 if( betaGammaSq < 0.01 ) logarithm = log(1. 640 if( betaGammaSq < 0.01 ) logarithm = log(1.0+betaGammaSq); // 0.0;
651 else 641 else
652 { 642 {
653 logarithm = -std::log( (1/betaGammaSq - f << 643 logarithm = -log( (1/betaGammaSq - fRePartDielectricConst[i])*
654 (1/betaGammaSq - fRePa << 644 (1/betaGammaSq - fRePartDielectricConst[i]) +
655 fImPartDielectricConst << 645 fImPartDielectricConst[i]*fImPartDielectricConst[i] )*0.5;
656 logarithm += std::log(1+1.0/betaGammaSq); << 646 logarithm += log(1+1.0/betaGammaSq);
657 } 647 }
658 648
659 if( fImPartDielectricConst[i] == 0.0 || bet 649 if( fImPartDielectricConst[i] == 0.0 || betaGammaSq < 0.01 )
660 { 650 {
661 argument = 0.0; 651 argument = 0.0;
662 } 652 }
663 else 653 else
664 { 654 {
665 x3 = -fRePartDielectricConst[i] + 1.0/bet 655 x3 = -fRePartDielectricConst[i] + 1.0/betaGammaSq;
666 x5 = -1.0 - fRePartDielectricConst[i] + 656 x5 = -1.0 - fRePartDielectricConst[i] +
667 be2*((1.0 +fRePartDielectricConst[i] 657 be2*((1.0 +fRePartDielectricConst[i])*(1.0 + fRePartDielectricConst[i]) +
668 fImPartDielectricConst[i]*fImPartDie << 658 fImPartDielectricConst[i]*fImPartDielectricConst[i]);
669 if( x3 == 0.0 ) argument = 0.5*pi; 659 if( x3 == 0.0 ) argument = 0.5*pi;
670 else argument = std::atan2(fIm << 660 else argument = atan2(fImPartDielectricConst[i],x3);
671 argument *= x5 ; 661 argument *= x5 ;
672 } 662 }
673 dNdxC = ( logarithm*fImPartDielectricConst[ 663 dNdxC = ( logarithm*fImPartDielectricConst[i] + argument )/hbarc;
674 664
675 if(dNdxC < 1.0e-8) dNdxC = 1.0e-8; 665 if(dNdxC < 1.0e-8) dNdxC = 1.0e-8;
676 666
677 dNdxC *= fine_structure_const/be2/pi; 667 dNdxC *= fine_structure_const/be2/pi;
678 668
679 dNdxC *= (1 - std::exp(-be4/betaBohr4)); << 669 dNdxC *= (1-exp(-be4/betaBohr4));
680 670
>> 671 // if(fDensity >= 0.1)
>> 672 // {
681 modul2 = (1.0 + fRePartDielectricConst[i])* 673 modul2 = (1.0 + fRePartDielectricConst[i])*(1.0 + fRePartDielectricConst[i]) +
682 fImPartDielectricConst[i]* 674 fImPartDielectricConst[i]*fImPartDielectricConst[i];
683 if(modul2 > 0.) 675 if(modul2 > 0.)
684 { 676 {
685 dNdxC /= modul2; 677 dNdxC /= modul2;
686 } 678 }
687 return dNdxC; 679 return dNdxC;
688 680
689 } // end of PAIdNdxCerenkov 681 } // end of PAIdNdxCerenkov
690 682
691 ////////////////////////////////////////////// 683 //////////////////////////////////////////////////////////////////////////
692 // 684 //
693 // Calculation od dN/dx of collisions with cre 685 // Calculation od dN/dx of collisions with creation of longitudinal EM
694 // excitations (plasmons, delta-electrons) 686 // excitations (plasmons, delta-electrons)
695 687
696 G4double G4PAIySection::PAIdNdxPlasmon( G4int << 688 G4double G4PAIySection::PAIdNdxPlasmon( G4int i ,
>> 689 G4double betaGammaSq )
697 { 690 {
698 G4double cof, resonance, modul2, dNdxP; 691 G4double cof, resonance, modul2, dNdxP;
699 G4double be2, be4; << 692 G4double be2, be4, betaBohr2, betaBohr4, cofBetaBohr;
700 693
701 cof = 1; 694 cof = 1;
>> 695 cofBetaBohr = 4.0;
>> 696 betaBohr2 = fine_structure_const*fine_structure_const;
>> 697 betaBohr4 = betaBohr2*betaBohr2*cofBetaBohr;
702 698
703 be2 = betaGammaSq/(1 + betaGammaSq); 699 be2 = betaGammaSq/(1 + betaGammaSq);
704 be4 = be2*be2; 700 be4 = be2*be2;
705 701
706 resonance = std::log(2*electron_mass_c2*be2 << 702 resonance = log(2*electron_mass_c2*be2/fSplineEnergy[i]);
707 resonance *= fImPartDielectricConst[i]/hbar 703 resonance *= fImPartDielectricConst[i]/hbarc;
708 704
>> 705
709 dNdxP = ( resonance + cof*fIntegralTerm[i]/ 706 dNdxP = ( resonance + cof*fIntegralTerm[i]/fSplineEnergy[i]/fSplineEnergy[i] );
710 707
711 dNdxP = std::max(dNdxP, 1.0e-8); << 708 if( dNdxP < 1.0e-8 ) dNdxP = 1.0e-8;
712 709
713 dNdxP *= fine_structure_const/be2/pi; 710 dNdxP *= fine_structure_const/be2/pi;
714 dNdxP *= (1 - std::exp(-be4/betaBohr4)); << 711 dNdxP *= (1-exp(-be4/betaBohr4));
715 712
>> 713 // if( fDensity >= 0.1 )
>> 714 // {
716 modul2 = (1 + fRePartDielectricConst[i])*(1 715 modul2 = (1 + fRePartDielectricConst[i])*(1 + fRePartDielectricConst[i]) +
717 fImPartDielectricConst[i]*fImPartDielectr 716 fImPartDielectricConst[i]*fImPartDielectricConst[i];
718 if(modul2 > 0.) 717 if(modul2 > 0.)
719 { 718 {
720 dNdxP /= modul2; 719 dNdxP /= modul2;
721 } 720 }
722 return dNdxP; 721 return dNdxP;
723 722
724 } // end of PAIdNdxPlasmon 723 } // end of PAIdNdxPlasmon
725 724
726 ////////////////////////////////////////////// 725 ////////////////////////////////////////////////////////////////////////
727 // 726 //
728 // Calculation of the PAI integral cross-secti 727 // Calculation of the PAI integral cross-section
729 // fIntegralPAIySection[1] = specific primary 728 // fIntegralPAIySection[1] = specific primary ionisation, 1/cm
730 // and fIntegralPAIySection[0] = mean energy l 729 // and fIntegralPAIySection[0] = mean energy loss per cm in keV/cm
731 730
732 void G4PAIySection::IntegralPAIySection() 731 void G4PAIySection::IntegralPAIySection()
733 { 732 {
734 fIntegralPAIySection[fSplineNumber] = 0; 733 fIntegralPAIySection[fSplineNumber] = 0;
735 fIntegralPAIdEdx[fSplineNumber] = 0; 734 fIntegralPAIdEdx[fSplineNumber] = 0;
736 fIntegralPAIySection[0] = 0; 735 fIntegralPAIySection[0] = 0;
737 G4int k = fIntervalNumber -1; 736 G4int k = fIntervalNumber -1;
738 737
739 for(G4int i = fSplineNumber-1; i >= 1; i--) 738 for(G4int i = fSplineNumber-1; i >= 1; i--)
740 { 739 {
741 if(fSplineEnergy[i] >= fEnergyInterval[k]) 740 if(fSplineEnergy[i] >= fEnergyInterval[k])
742 { 741 {
743 fIntegralPAIySection[i] = fIntegralPAIyS 742 fIntegralPAIySection[i] = fIntegralPAIySection[i+1] + SumOverInterval(i);
744 fIntegralPAIdEdx[i] = fIntegralPAIdEdx[i 743 fIntegralPAIdEdx[i] = fIntegralPAIdEdx[i+1] + SumOverIntervaldEdx(i);
745 } 744 }
746 else 745 else
747 { 746 {
748 fIntegralPAIySection[i] = fIntegralPAIyS 747 fIntegralPAIySection[i] = fIntegralPAIySection[i+1] +
749 SumOverBord << 748 SumOverBorder(i+1,fEnergyInterval[k]);
750 fIntegralPAIdEdx[i] = fIntegralPAIdEdx[i 749 fIntegralPAIdEdx[i] = fIntegralPAIdEdx[i+1] +
751 SumOverBord << 750 SumOverBorderdEdx(i+1,fEnergyInterval[k]);
752 k--; 751 k--;
753 } 752 }
754 } 753 }
755 } // end of IntegralPAIySection 754 } // end of IntegralPAIySection
756 755
757 ////////////////////////////////////////////// 756 ////////////////////////////////////////////////////////////////////////
758 // 757 //
759 // Calculation of the PAI Cerenkov integral cr 758 // Calculation of the PAI Cerenkov integral cross-section
760 // fIntegralCrenkov[1] = specific Crenkov ioni 759 // fIntegralCrenkov[1] = specific Crenkov ionisation, 1/cm
761 // and fIntegralCerenkov[0] = mean Cerenkov lo 760 // and fIntegralCerenkov[0] = mean Cerenkov loss per cm in keV/cm
762 761
763 void G4PAIySection::IntegralCerenkov() 762 void G4PAIySection::IntegralCerenkov()
764 { 763 {
765 G4int i, k; 764 G4int i, k;
766 fIntegralCerenkov[fSplineNumber] = 0; 765 fIntegralCerenkov[fSplineNumber] = 0;
767 fIntegralCerenkov[0] = 0; 766 fIntegralCerenkov[0] = 0;
768 k = fIntervalNumber -1; 767 k = fIntervalNumber -1;
769 768
770 for( i = fSplineNumber-1; i >= 1; i-- ) 769 for( i = fSplineNumber-1; i >= 1; i-- )
771 { 770 {
772 if(fSplineEnergy[i] >= fEnergyInterval[k 771 if(fSplineEnergy[i] >= fEnergyInterval[k])
773 { 772 {
774 fIntegralCerenkov[i] = fIntegralCerenk 773 fIntegralCerenkov[i] = fIntegralCerenkov[i+1] + SumOverInterCerenkov(i);
775 // G4cout<<"int: i = "<<i<<"; sumC = " << 774 // G4cout<<"int: i = "<<i<<"; sumC = "<<fIntegralCerenkov[i]<<G4endl;
776 } 775 }
777 else 776 else
778 { 777 {
779 fIntegralCerenkov[i] = fIntegralCerenk 778 fIntegralCerenkov[i] = fIntegralCerenkov[i+1] +
780 SumOverBord << 779 SumOverBordCerenkov(i+1,fEnergyInterval[k]);
781 k--; << 780 k--;
782 // G4cout<<"bord: i = "<<i<<"; sumC = << 781 // G4cout<<"bord: i = "<<i<<"; sumC = "<<fIntegralCerenkov[i]<<G4endl;
783 } 782 }
784 } 783 }
785 784
786 } // end of IntegralCerenkov 785 } // end of IntegralCerenkov
787 786
788 ////////////////////////////////////////////// 787 ////////////////////////////////////////////////////////////////////////
789 // 788 //
790 // Calculation of the PAI Plasmon integral cro 789 // Calculation of the PAI Plasmon integral cross-section
791 // fIntegralPlasmon[1] = splasmon primary ioni 790 // fIntegralPlasmon[1] = splasmon primary ionisation, 1/cm
792 // and fIntegralPlasmon[0] = mean plasmon loss 791 // and fIntegralPlasmon[0] = mean plasmon loss per cm in keV/cm
793 792
794 void G4PAIySection::IntegralPlasmon() 793 void G4PAIySection::IntegralPlasmon()
795 { 794 {
796 fIntegralPlasmon[fSplineNumber] = 0; 795 fIntegralPlasmon[fSplineNumber] = 0;
797 fIntegralPlasmon[0] = 0; 796 fIntegralPlasmon[0] = 0;
798 G4int k = fIntervalNumber -1; 797 G4int k = fIntervalNumber -1;
799 for(G4int i=fSplineNumber-1;i>=1;i--) 798 for(G4int i=fSplineNumber-1;i>=1;i--)
800 { 799 {
801 if(fSplineEnergy[i] >= fEnergyInterval[k 800 if(fSplineEnergy[i] >= fEnergyInterval[k])
802 { 801 {
803 fIntegralPlasmon[i] = fIntegralPlasmon 802 fIntegralPlasmon[i] = fIntegralPlasmon[i+1] + SumOverInterPlasmon(i);
804 } 803 }
805 else 804 else
806 { 805 {
807 fIntegralPlasmon[i] = fIntegralPlasmon 806 fIntegralPlasmon[i] = fIntegralPlasmon[i+1] +
808 SumOverBord << 807 SumOverBordPlasmon(i+1,fEnergyInterval[k]);
809 k--; << 808 k--;
810 } 809 }
811 } 810 }
>> 811
812 } // end of IntegralPlasmon 812 } // end of IntegralPlasmon
813 813
814 ////////////////////////////////////////////// 814 //////////////////////////////////////////////////////////////////////
815 // 815 //
816 // Calculation the PAI integral cross-section 816 // Calculation the PAI integral cross-section inside
817 // of interval of continuous values of photo-i 817 // of interval of continuous values of photo-ionisation
818 // cross-section. Parameter 'i' is the number 818 // cross-section. Parameter 'i' is the number of interval.
819 819
820 G4double G4PAIySection::SumOverInterval( G4int 820 G4double G4PAIySection::SumOverInterval( G4int i )
821 { 821 {
822 G4double x0,x1,y0,yy1,a,b,c,result; 822 G4double x0,x1,y0,yy1,a,b,c,result;
823 823
824 x0 = fSplineEnergy[i]; 824 x0 = fSplineEnergy[i];
825 x1 = fSplineEnergy[i+1]; 825 x1 = fSplineEnergy[i+1];
826 <<
827 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) <<
828 <<
829 y0 = fDifPAIySection[i]; 826 y0 = fDifPAIySection[i];
830 yy1 = fDifPAIySection[i+1]; 827 yy1 = fDifPAIySection[i+1];
831 //G4cout << "## x0= " << x0 << " x1= " << x <<
832 c = x1/x0; 828 c = x1/x0;
833 //G4cout << "c= " << c << " y0= " << y0 << <<
834 a = log10(yy1/y0)/log10(c); 829 a = log10(yy1/y0)/log10(c);
835 //G4cout << "a= " << a << G4endl; << 830 // b = log10(y0) - a*log10(x0);
836 << 831 b = y0/pow(x0,a);
837 b = 0.0; <<
838 if(a < 20.) b = y0/pow(x0,a); <<
839 <<
840 a += 1; 832 a += 1;
841 if(a == 0) 833 if(a == 0)
842 { 834 {
843 result = b*log(x1/x0); 835 result = b*log(x1/x0);
844 } 836 }
845 else 837 else
846 { 838 {
847 result = y0*(x1*pow(c,a-1) - x0)/a; 839 result = y0*(x1*pow(c,a-1) - x0)/a;
848 } 840 }
849 a++; 841 a++;
850 if(a == 0) 842 if(a == 0)
851 { 843 {
852 fIntegralPAIySection[0] += b*log(x1/x0); 844 fIntegralPAIySection[0] += b*log(x1/x0);
853 } 845 }
854 else 846 else
855 { 847 {
856 fIntegralPAIySection[0] += y0*(x1*x1*pow 848 fIntegralPAIySection[0] += y0*(x1*x1*pow(c,a-2) - x0*x0)/a;
857 } 849 }
858 return result; 850 return result;
859 851
860 } // end of SumOverInterval 852 } // end of SumOverInterval
861 853
862 ///////////////////////////////// 854 /////////////////////////////////
863 855
864 G4double G4PAIySection::SumOverIntervaldEdx( G 856 G4double G4PAIySection::SumOverIntervaldEdx( G4int i )
865 { 857 {
866 G4double x0,x1,y0,yy1,a,b,c,result; 858 G4double x0,x1,y0,yy1,a,b,c,result;
867 859
868 x0 = fSplineEnergy[i]; 860 x0 = fSplineEnergy[i];
869 x1 = fSplineEnergy[i+1]; 861 x1 = fSplineEnergy[i+1];
870 <<
871 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) <<
872 <<
873 y0 = fDifPAIySection[i]; 862 y0 = fDifPAIySection[i];
874 yy1 = fDifPAIySection[i+1]; 863 yy1 = fDifPAIySection[i+1];
875 c = x1/x0; 864 c = x1/x0;
876 a = log10(yy1/y0)/log10(c); 865 a = log10(yy1/y0)/log10(c);
877 << 866 // b = log10(y0) - a*log10(x0);
878 b = 0.0; << 867 b = y0/pow(x0,a);
879 if(a < 20.) b = y0/pow(x0,a); <<
880 <<
881 a += 2; 868 a += 2;
882 if(a == 0) 869 if(a == 0)
883 { 870 {
884 result = b*log(x1/x0); 871 result = b*log(x1/x0);
885 } 872 }
886 else 873 else
887 { 874 {
888 result = y0*(x1*x1*pow(c,a-2) - x0*x0)/a; 875 result = y0*(x1*x1*pow(c,a-2) - x0*x0)/a;
889 } 876 }
890 return result; 877 return result;
891 878
892 } // end of SumOverInterval 879 } // end of SumOverInterval
893 880
894 ////////////////////////////////////////////// 881 //////////////////////////////////////////////////////////////////////
895 // 882 //
896 // Calculation the PAI Cerenkov integral cross 883 // Calculation the PAI Cerenkov integral cross-section inside
897 // of interval of continuous values of photo-i 884 // of interval of continuous values of photo-ionisation Cerenkov
898 // cross-section. Parameter 'i' is the number 885 // cross-section. Parameter 'i' is the number of interval.
899 886
900 G4double G4PAIySection::SumOverInterCerenkov( 887 G4double G4PAIySection::SumOverInterCerenkov( G4int i )
901 { 888 {
902 G4double x0,x1,y0,yy1,a,c,result; 889 G4double x0,x1,y0,yy1,a,c,result;
903 890
904 x0 = fSplineEnergy[i]; 891 x0 = fSplineEnergy[i];
905 x1 = fSplineEnergy[i+1]; 892 x1 = fSplineEnergy[i+1];
906 <<
907 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) <<
908 <<
909 y0 = fdNdxCerenkov[i]; 893 y0 = fdNdxCerenkov[i];
910 yy1 = fdNdxCerenkov[i+1]; 894 yy1 = fdNdxCerenkov[i+1];
911 // G4cout<<"SumC, i = "<<i<<"; x0 ="<<x0<<" 895 // G4cout<<"SumC, i = "<<i<<"; x0 ="<<x0<<"; x1 = "<<x1
912 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4en 896 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4endl;
913 897
914 c = x1/x0; 898 c = x1/x0;
915 a = log10(yy1/y0)/log10(c); 899 a = log10(yy1/y0)/log10(c);
916 G4double b = 0.0; 900 G4double b = 0.0;
917 if(a < 20.) b = y0/pow(x0,a); 901 if(a < 20.) b = y0/pow(x0,a);
918 902
919 a += 1.0; 903 a += 1.0;
920 if(a == 0) result = b*log(c); 904 if(a == 0) result = b*log(c);
921 else result = y0*(x1*pow(c,a-1) - x0) 905 else result = y0*(x1*pow(c,a-1) - x0)/a;
922 a += 1.0; 906 a += 1.0;
923 907
924 if( a == 0 ) fIntegralCerenkov[0] += b*log( 908 if( a == 0 ) fIntegralCerenkov[0] += b*log(x1/x0);
925 else fIntegralCerenkov[0] += y0*(x1 909 else fIntegralCerenkov[0] += y0*(x1*x1*pow(c,a-2) - x0*x0)/a;
926 // G4cout<<"a = "<<a<<"; b = "<<b<<"; resu 910 // G4cout<<"a = "<<a<<"; b = "<<b<<"; result = "<<result<<G4endl;
927 return result; 911 return result;
928 912
929 } // end of SumOverInterCerenkov 913 } // end of SumOverInterCerenkov
930 914
931 ////////////////////////////////////////////// 915 //////////////////////////////////////////////////////////////////////
932 // 916 //
933 // Calculation the PAI Plasmon integral cross- 917 // Calculation the PAI Plasmon integral cross-section inside
934 // of interval of continuous values of photo-i 918 // of interval of continuous values of photo-ionisation Plasmon
935 // cross-section. Parameter 'i' is the number 919 // cross-section. Parameter 'i' is the number of interval.
936 920
937 G4double G4PAIySection::SumOverInterPlasmon( G 921 G4double G4PAIySection::SumOverInterPlasmon( G4int i )
938 { 922 {
939 G4double x0,x1,y0,yy1,a,c,result; 923 G4double x0,x1,y0,yy1,a,c,result;
940 924
941 x0 = fSplineEnergy[i]; 925 x0 = fSplineEnergy[i];
942 x1 = fSplineEnergy[i+1]; 926 x1 = fSplineEnergy[i+1];
943 <<
944 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) <<
945 <<
946 y0 = fdNdxPlasmon[i]; 927 y0 = fdNdxPlasmon[i];
947 yy1 = fdNdxPlasmon[i+1]; 928 yy1 = fdNdxPlasmon[i+1];
948 c = x1/x0; 929 c = x1/x0;
949 a = log10(yy1/y0)/log10(c); 930 a = log10(yy1/y0)/log10(c);
950 931
951 G4double b = 0.0; 932 G4double b = 0.0;
952 if(a < 20.) b = y0/pow(x0,a); 933 if(a < 20.) b = y0/pow(x0,a);
953 934
954 a += 1.0; 935 a += 1.0;
955 if(a == 0) result = b*log(x1/x0); 936 if(a == 0) result = b*log(x1/x0);
956 else result = y0*(x1*pow(c,a-1) - x0) 937 else result = y0*(x1*pow(c,a-1) - x0)/a;
957 a += 1.0; 938 a += 1.0;
958 939
959 if( a == 0 ) fIntegralPlasmon[0] += b*log(x 940 if( a == 0 ) fIntegralPlasmon[0] += b*log(x1/x0);
960 else fIntegralPlasmon[0] += y0*(x1* 941 else fIntegralPlasmon[0] += y0*(x1*x1*pow(c,a-2) - x0*x0)/a;
961 942
962 return result; 943 return result;
963 944
964 } // end of SumOverInterPlasmon 945 } // end of SumOverInterPlasmon
965 946
966 ////////////////////////////////////////////// 947 ///////////////////////////////////////////////////////////////////////////////
967 // 948 //
968 // Integration of PAI cross-section for the ca 949 // Integration of PAI cross-section for the case of
969 // passing across border between intervals 950 // passing across border between intervals
970 951
971 G4double G4PAIySection::SumOverBorder( G4int 952 G4double G4PAIySection::SumOverBorder( G4int i ,
972 G4doubl 953 G4double en0 )
973 { 954 {
974 G4double x0,x1,y0,yy1,a,d,e0,result; << 955 G4double x0,x1,y0,yy1,a,/*c,*/d,e0,result;
975 956
976 e0 = en0; 957 e0 = en0;
977 x0 = fSplineEnergy[i]; 958 x0 = fSplineEnergy[i];
978 x1 = fSplineEnergy[i+1]; 959 x1 = fSplineEnergy[i+1];
979 y0 = fDifPAIySection[i]; 960 y0 = fDifPAIySection[i];
980 yy1 = fDifPAIySection[i+1]; 961 yy1 = fDifPAIySection[i+1];
981 962
>> 963 //c = x1/x0;
982 d = e0/x0; 964 d = e0/x0;
983 a = log10(yy1/y0)/log10(x1/x0); 965 a = log10(yy1/y0)/log10(x1/x0);
984 966
985 G4double b = 0.0; 967 G4double b = 0.0;
986 if(a < 20.) b = y0/pow(x0,a); 968 if(a < 20.) b = y0/pow(x0,a);
987 969
988 a += 1; 970 a += 1;
989 if(a == 0) 971 if(a == 0)
990 { 972 {
991 result = b*log(x0/e0); 973 result = b*log(x0/e0);
992 } 974 }
993 else 975 else
994 { 976 {
995 result = y0*(x0 - e0*pow(d,a-1))/a; 977 result = y0*(x0 - e0*pow(d,a-1))/a;
996 } 978 }
997 a++; 979 a++;
998 if(a == 0) 980 if(a == 0)
999 { 981 {
1000 fIntegralPAIySection[0] += b*log(x0/e0) 982 fIntegralPAIySection[0] += b*log(x0/e0);
1001 } 983 }
1002 else 984 else
1003 { 985 {
1004 fIntegralPAIySection[0] += y0*(x0*x0 - 986 fIntegralPAIySection[0] += y0*(x0*x0 - e0*e0*pow(d,a-2))/a;
1005 } 987 }
1006 x0 = fSplineEnergy[i - 1]; 988 x0 = fSplineEnergy[i - 1];
1007 x1 = fSplineEnergy[i - 2]; 989 x1 = fSplineEnergy[i - 2];
1008 y0 = fDifPAIySection[i - 1]; 990 y0 = fDifPAIySection[i - 1];
1009 yy1 = fDifPAIySection[i - 2]; 991 yy1 = fDifPAIySection[i - 2];
1010 992
1011 //c = x1/x0; 993 //c = x1/x0;
1012 d = e0/x0; 994 d = e0/x0;
1013 a = log10(yy1/y0)/log10(x1/x0); 995 a = log10(yy1/y0)/log10(x1/x0);
1014 << 996 // b0 = log10(y0) - a*log10(x0);
1015 b = 0.0; << 997 b = y0/pow(x0,a);
1016 if(a < 20.) b = y0/pow(x0,a); <<
1017 <<
1018 a += 1; 998 a += 1;
1019 if(a == 0) 999 if(a == 0)
1020 { 1000 {
1021 result += b*log(e0/x0); 1001 result += b*log(e0/x0);
1022 } 1002 }
1023 else 1003 else
1024 { 1004 {
1025 result += y0*(e0*pow(d,a-1) - x0)/a; 1005 result += y0*(e0*pow(d,a-1) - x0)/a;
1026 } 1006 }
1027 a++; 1007 a++;
1028 if(a == 0) 1008 if(a == 0)
1029 { 1009 {
1030 fIntegralPAIySection[0] += b*log(e0/x0) 1010 fIntegralPAIySection[0] += b*log(e0/x0);
1031 } 1011 }
1032 else 1012 else
1033 { 1013 {
1034 fIntegralPAIySection[0] += y0*(e0*e0*po 1014 fIntegralPAIySection[0] += y0*(e0*e0*pow(d,a-2) - x0*x0)/a;
1035 } 1015 }
1036 return result; 1016 return result;
1037 1017
1038 } 1018 }
1039 1019
1040 ///////////////////////////////////////////// 1020 ///////////////////////////////////////////////////////////////////////
1041 1021
1042 G4double G4PAIySection::SumOverBorderdEdx( G4 1022 G4double G4PAIySection::SumOverBorderdEdx( G4int i ,
1043 G4doub 1023 G4double en0 )
1044 { 1024 {
1045 G4double x0,x1,y0,yy1,a,/*c,*/d,e0,result; 1025 G4double x0,x1,y0,yy1,a,/*c,*/d,e0,result;
1046 1026
1047 e0 = en0; 1027 e0 = en0;
1048 x0 = fSplineEnergy[i]; 1028 x0 = fSplineEnergy[i];
1049 x1 = fSplineEnergy[i+1]; 1029 x1 = fSplineEnergy[i+1];
1050 y0 = fDifPAIySection[i]; 1030 y0 = fDifPAIySection[i];
1051 yy1 = fDifPAIySection[i+1]; 1031 yy1 = fDifPAIySection[i+1];
1052 1032
>> 1033 //c = x1/x0;
1053 d = e0/x0; 1034 d = e0/x0;
1054 a = log10(yy1/y0)/log10(x1/x0); 1035 a = log10(yy1/y0)/log10(x1/x0);
1055 1036
1056 G4double b = 0.0; 1037 G4double b = 0.0;
1057 if(a < 20.) b = y0/pow(x0,a); 1038 if(a < 20.) b = y0/pow(x0,a);
1058 1039
1059 a += 2; 1040 a += 2;
1060 if(a == 0) 1041 if(a == 0)
1061 { 1042 {
1062 result = b*log(x0/e0); 1043 result = b*log(x0/e0);
1063 } 1044 }
1064 else 1045 else
1065 { 1046 {
1066 result = y0*(x0*x0 - e0*e0*pow(d,a-2))/ 1047 result = y0*(x0*x0 - e0*e0*pow(d,a-2))/a;
1067 } 1048 }
1068 x0 = fSplineEnergy[i - 1]; 1049 x0 = fSplineEnergy[i - 1];
1069 x1 = fSplineEnergy[i - 2]; 1050 x1 = fSplineEnergy[i - 2];
1070 y0 = fDifPAIySection[i - 1]; 1051 y0 = fDifPAIySection[i - 1];
1071 yy1 = fDifPAIySection[i - 2]; 1052 yy1 = fDifPAIySection[i - 2];
1072 1053
>> 1054 //c = x1/x0;
1073 d = e0/x0; 1055 d = e0/x0;
1074 a = log10(yy1/y0)/log10(x1/x0); 1056 a = log10(yy1/y0)/log10(x1/x0);
1075 1057
1076 b = 0.0; <<
1077 if(a < 20.) b = y0/pow(x0,a); 1058 if(a < 20.) b = y0/pow(x0,a);
1078 1059
1079 a += 2; 1060 a += 2;
1080 if(a == 0) 1061 if(a == 0)
1081 { 1062 {
1082 result += b*log(e0/x0); 1063 result += b*log(e0/x0);
1083 } 1064 }
1084 else 1065 else
1085 { 1066 {
1086 result += y0*(e0*e0*pow(d,a-2) - x0*x0) 1067 result += y0*(e0*e0*pow(d,a-2) - x0*x0)/a;
1087 } 1068 }
1088 return result; 1069 return result;
>> 1070
1089 } 1071 }
1090 1072
1091 ///////////////////////////////////////////// 1073 ///////////////////////////////////////////////////////////////////////////////
1092 // 1074 //
1093 // Integration of Cerenkov cross-section for 1075 // Integration of Cerenkov cross-section for the case of
1094 // passing across border between intervals 1076 // passing across border between intervals
1095 1077
1096 G4double G4PAIySection::SumOverBordCerenkov( 1078 G4double G4PAIySection::SumOverBordCerenkov( G4int i ,
1097 1079 G4double en0 )
1098 { 1080 {
1099 G4double x0,x1,y0,yy1,a,e0,c,d,result; 1081 G4double x0,x1,y0,yy1,a,e0,c,d,result;
1100 1082
1101 e0 = en0; 1083 e0 = en0;
1102 x0 = fSplineEnergy[i]; 1084 x0 = fSplineEnergy[i];
1103 x1 = fSplineEnergy[i+1]; 1085 x1 = fSplineEnergy[i+1];
1104 y0 = fdNdxCerenkov[i]; 1086 y0 = fdNdxCerenkov[i];
1105 yy1 = fdNdxCerenkov[i+1]; 1087 yy1 = fdNdxCerenkov[i+1];
1106 1088
1107 // G4cout<<G4endl; 1089 // G4cout<<G4endl;
1108 //G4cout<<"SumBordC, i = "<<i<<"; en0 = "< 1090 //G4cout<<"SumBordC, i = "<<i<<"; en0 = "<<en0<<"; x0 ="<<x0<<"; x1 = "<<x1
1109 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G 1091 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4endl;
1110 c = x1/x0; 1092 c = x1/x0;
1111 d = e0/x0; 1093 d = e0/x0;
1112 a = log10(yy1/y0)/log10(c); 1094 a = log10(yy1/y0)/log10(c);
1113 1095
1114 G4double b = 0.0; 1096 G4double b = 0.0;
1115 if(a < 20.) b = y0/pow(x0,a); 1097 if(a < 20.) b = y0/pow(x0,a);
1116 1098
1117 a += 1.0; 1099 a += 1.0;
1118 if( a == 0 ) result = b*log(x0/e0); 1100 if( a == 0 ) result = b*log(x0/e0);
1119 else result = y0*(x0 - e0*pow(d,a- 1101 else result = y0*(x0 - e0*pow(d,a-1))/a;
1120 a += 1.0; 1102 a += 1.0;
1121 1103
1122 if( a == 0 ) fIntegralCerenkov[0] += b*log 1104 if( a == 0 ) fIntegralCerenkov[0] += b*log(x0/e0);
1123 else fIntegralCerenkov[0] += y0*(x 1105 else fIntegralCerenkov[0] += y0*(x0*x0 - e0*e0*pow(d,a-2))/a;
1124 1106
1125 //G4cout<<"a = "<<a<<"; b = "<<b<<"; resul 1107 //G4cout<<"a = "<<a<<"; b = "<<b<<"; result = "<<result<<G4endl;
1126 1108
1127 x0 = fSplineEnergy[i - 1]; 1109 x0 = fSplineEnergy[i - 1];
1128 x1 = fSplineEnergy[i - 2]; 1110 x1 = fSplineEnergy[i - 2];
1129 y0 = fdNdxCerenkov[i - 1]; 1111 y0 = fdNdxCerenkov[i - 1];
1130 yy1 = fdNdxCerenkov[i - 2]; 1112 yy1 = fdNdxCerenkov[i - 2];
1131 1113
1132 //G4cout<<"x0 ="<<x0<<"; x1 = "<<x1 1114 //G4cout<<"x0 ="<<x0<<"; x1 = "<<x1
1133 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4 1115 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4endl;
1134 1116
1135 c = x1/x0; 1117 c = x1/x0;
1136 d = e0/x0; 1118 d = e0/x0;
1137 a = log10(yy1/y0)/log10(x1/x0); 1119 a = log10(yy1/y0)/log10(x1/x0);
1138 1120
1139 // G4cout << "a= " << a << G4endl; 1121 // G4cout << "a= " << a << G4endl;
>> 1122 if(a < 20.) b = y0/pow(x0,a);
>> 1123
1140 if(a > 20.0) b = 0.0; 1124 if(a > 20.0) b = 0.0;
1141 else b = y0/pow(x0,a); << 1125 else b = y0/pow(x0,a); // pow(10.,b0);
1142 1126
1143 //G4cout << "b= " << b << G4endl; 1127 //G4cout << "b= " << b << G4endl;
1144 1128
1145 a += 1.0; 1129 a += 1.0;
1146 if( a == 0 ) result += b*log(e0/x0); 1130 if( a == 0 ) result += b*log(e0/x0);
1147 else result += y0*(e0*pow(d,a-1) - 1131 else result += y0*(e0*pow(d,a-1) - x0 )/a;
1148 a += 1.0; 1132 a += 1.0;
1149 //G4cout << "result= " << result << G4endl 1133 //G4cout << "result= " << result << G4endl;
1150 1134
1151 if( a == 0 ) fIntegralCerenkov[0] += b*l 1135 if( a == 0 ) fIntegralCerenkov[0] += b*log(e0/x0);
1152 else fIntegralCerenkov[0] += y0* 1136 else fIntegralCerenkov[0] += y0*(e0*e0*pow(d,a-2) - x0*x0)/a;
1153 1137
1154 //G4cout<<"a = "<<a<<"; b = "<<b<<"; resul 1138 //G4cout<<"a = "<<a<<"; b = "<<b<<"; result = "<<result<<G4endl;
1155 1139
1156 return result; 1140 return result;
>> 1141
1157 } 1142 }
1158 1143
1159 ///////////////////////////////////////////// 1144 ///////////////////////////////////////////////////////////////////////////////
1160 // 1145 //
1161 // Integration of Plasmon cross-section for t 1146 // Integration of Plasmon cross-section for the case of
1162 // passing across border between intervals 1147 // passing across border between intervals
1163 1148
1164 G4double G4PAIySection::SumOverBordPlasmon( G 1149 G4double G4PAIySection::SumOverBordPlasmon( G4int i ,
1165 1150 G4double en0 )
1166 { 1151 {
1167 G4double x0,x1,y0,yy1,a,c,d,e0,result; 1152 G4double x0,x1,y0,yy1,a,c,d,e0,result;
1168 1153
1169 e0 = en0; 1154 e0 = en0;
1170 x0 = fSplineEnergy[i]; 1155 x0 = fSplineEnergy[i];
1171 x1 = fSplineEnergy[i+1]; 1156 x1 = fSplineEnergy[i+1];
1172 y0 = fdNdxPlasmon[i]; 1157 y0 = fdNdxPlasmon[i];
1173 yy1 = fdNdxPlasmon[i+1]; 1158 yy1 = fdNdxPlasmon[i+1];
1174 1159
1175 c = x1/x0; 1160 c = x1/x0;
1176 d = e0/x0; 1161 d = e0/x0;
1177 a = log10(yy1/y0)/log10(c); 1162 a = log10(yy1/y0)/log10(c);
1178 1163
1179 G4double b = 0.0; 1164 G4double b = 0.0;
1180 if(a < 20.) b = y0/pow(x0,a); 1165 if(a < 20.) b = y0/pow(x0,a);
1181 1166
1182 a += 1.0; 1167 a += 1.0;
1183 if( a == 0 ) result = b*log(x0/e0); 1168 if( a == 0 ) result = b*log(x0/e0);
1184 else result = y0*(x0 - e0*pow(d,a- 1169 else result = y0*(x0 - e0*pow(d,a-1))/a;
1185 a += 1.0; 1170 a += 1.0;
1186 1171
1187 if( a == 0 ) fIntegralPlasmon[0] += b*log( 1172 if( a == 0 ) fIntegralPlasmon[0] += b*log(x0/e0);
1188 else fIntegralPlasmon[0] += y0*(x0 1173 else fIntegralPlasmon[0] += y0*(x0*x0 - e0*e0*pow(d,a-2))/a;
1189 1174
1190 x0 = fSplineEnergy[i - 1]; 1175 x0 = fSplineEnergy[i - 1];
1191 x1 = fSplineEnergy[i - 2]; 1176 x1 = fSplineEnergy[i - 2];
1192 y0 = fdNdxPlasmon[i - 1]; 1177 y0 = fdNdxPlasmon[i - 1];
1193 yy1 = fdNdxPlasmon[i - 2]; 1178 yy1 = fdNdxPlasmon[i - 2];
1194 1179
1195 c = x1/x0; 1180 c = x1/x0;
1196 d = e0/x0; 1181 d = e0/x0;
1197 a = log10(yy1/y0)/log10(c); 1182 a = log10(yy1/y0)/log10(c);
1198 1183
1199 if(a < 20.) b = y0/pow(x0,a); 1184 if(a < 20.) b = y0/pow(x0,a);
1200 1185
1201 a += 1.0; 1186 a += 1.0;
1202 if( a == 0 ) result += b*log(e0/x0); 1187 if( a == 0 ) result += b*log(e0/x0);
1203 else result += y0*(e0*pow(d,a-1) - 1188 else result += y0*(e0*pow(d,a-1) - x0)/a;
1204 a += 1.0; 1189 a += 1.0;
1205 1190
1206 if( a == 0 ) fIntegralPlasmon[0] += b*lo 1191 if( a == 0 ) fIntegralPlasmon[0] += b*log(e0/x0);
1207 else fIntegralPlasmon[0] += y0*( 1192 else fIntegralPlasmon[0] += y0*(e0*e0*pow(d,a-2) - x0*x0)/a;
1208 1193
1209 return result; 1194 return result;
1210 1195
1211 } 1196 }
1212 1197
1213 ///////////////////////////////////////////// 1198 /////////////////////////////////////////////////////////////////////////
1214 // 1199 //
1215 // 1200 //
1216 1201
1217 G4double G4PAIySection::GetStepEnergyLoss( G4 1202 G4double G4PAIySection::GetStepEnergyLoss( G4double step )
1218 { 1203 {
1219 G4int iTransfer ; 1204 G4int iTransfer ;
1220 G4long numOfCollisions; 1205 G4long numOfCollisions;
1221 G4double loss = 0.0; 1206 G4double loss = 0.0;
1222 G4double meanNumber, position; 1207 G4double meanNumber, position;
1223 1208
1224 // G4cout<<" G4PAIySection::GetStepEnergyLo 1209 // G4cout<<" G4PAIySection::GetStepEnergyLoss "<<G4endl;
1225 1210
1226 1211
1227 1212
1228 meanNumber = fIntegralPAIySection[1]*step; 1213 meanNumber = fIntegralPAIySection[1]*step;
1229 numOfCollisions = G4Poisson(meanNumber); 1214 numOfCollisions = G4Poisson(meanNumber);
1230 1215
1231 // G4cout<<"numOfCollisions = "<<numOfCol 1216 // G4cout<<"numOfCollisions = "<<numOfCollisions<<G4endl;
1232 1217
1233 while(numOfCollisions) 1218 while(numOfCollisions)
1234 { 1219 {
1235 position = fIntegralPAIySection[1]*G4Unif 1220 position = fIntegralPAIySection[1]*G4UniformRand();
1236 1221
1237 for( iTransfer=1; iTransfer<=fSplineNumbe 1222 for( iTransfer=1; iTransfer<=fSplineNumber; iTransfer++ )
1238 { 1223 {
1239 if( position >= fIntegralPAIySection[ 1224 if( position >= fIntegralPAIySection[iTransfer] ) break;
1240 } 1225 }
1241 loss += fSplineEnergy[iTransfer] ; 1226 loss += fSplineEnergy[iTransfer] ;
1242 numOfCollisions--; 1227 numOfCollisions--;
1243 // Loop checking, 03-Aug-2015, Vladimir I <<
1244 } 1228 }
1245 // G4cout<<"PAI energy loss = "<<loss/keV<< 1229 // G4cout<<"PAI energy loss = "<<loss/keV<<" keV"<<G4endl;
1246 1230
1247 return loss; 1231 return loss;
1248 } 1232 }
1249 1233
1250 ///////////////////////////////////////////// 1234 /////////////////////////////////////////////////////////////////////////
1251 // 1235 //
1252 // 1236 //
1253 1237
1254 G4double G4PAIySection::GetStepCerenkovLoss( 1238 G4double G4PAIySection::GetStepCerenkovLoss( G4double step )
1255 { 1239 {
1256 G4int iTransfer ; 1240 G4int iTransfer ;
1257 G4long numOfCollisions; 1241 G4long numOfCollisions;
1258 G4double loss = 0.0; 1242 G4double loss = 0.0;
1259 G4double meanNumber, position; 1243 G4double meanNumber, position;
1260 1244
1261 // G4cout<<" G4PAIySection::GetStepCreLosnk 1245 // G4cout<<" G4PAIySection::GetStepCreLosnkovs "<<G4endl;
1262 1246
1263 1247
1264 1248
1265 meanNumber = fIntegralCerenkov[1]*step; 1249 meanNumber = fIntegralCerenkov[1]*step;
1266 numOfCollisions = G4Poisson(meanNumber); 1250 numOfCollisions = G4Poisson(meanNumber);
1267 1251
1268 // G4cout<<"numOfCollisions = "<<numOfCol 1252 // G4cout<<"numOfCollisions = "<<numOfCollisions<<G4endl;
1269 1253
1270 while(numOfCollisions) 1254 while(numOfCollisions)
1271 { 1255 {
1272 position = fIntegralCerenkov[1]*G4Uniform 1256 position = fIntegralCerenkov[1]*G4UniformRand();
1273 1257
1274 for( iTransfer=1; iTransfer<=fSplineNumbe 1258 for( iTransfer=1; iTransfer<=fSplineNumber; iTransfer++ )
1275 { 1259 {
1276 if( position >= fIntegralCerenkov[iTr 1260 if( position >= fIntegralCerenkov[iTransfer] ) break;
1277 } 1261 }
1278 loss += fSplineEnergy[iTransfer] ; 1262 loss += fSplineEnergy[iTransfer] ;
1279 numOfCollisions--; 1263 numOfCollisions--;
1280 // Loop checking, 03-Aug-2015, Vladimir I <<
1281 } 1264 }
1282 // G4cout<<"PAI Cerenkov loss = "<<loss/keV 1265 // G4cout<<"PAI Cerenkov loss = "<<loss/keV<<" keV"<<G4endl;
1283 1266
1284 return loss; 1267 return loss;
1285 } 1268 }
1286 1269
1287 ///////////////////////////////////////////// 1270 /////////////////////////////////////////////////////////////////////////
1288 // 1271 //
1289 // 1272 //
1290 1273
1291 G4double G4PAIySection::GetStepPlasmonLoss( G 1274 G4double G4PAIySection::GetStepPlasmonLoss( G4double step )
1292 { 1275 {
1293 G4int iTransfer ; 1276 G4int iTransfer ;
1294 G4long numOfCollisions; 1277 G4long numOfCollisions;
1295 G4double loss = 0.0; 1278 G4double loss = 0.0;
1296 G4double meanNumber, position; 1279 G4double meanNumber, position;
1297 1280
1298 // G4cout<<" G4PAIySection::GetStepCreLosnk 1281 // G4cout<<" G4PAIySection::GetStepCreLosnkovs "<<G4endl;
1299 1282
1300 1283
1301 1284
1302 meanNumber = fIntegralPlasmon[1]*step; 1285 meanNumber = fIntegralPlasmon[1]*step;
1303 numOfCollisions = G4Poisson(meanNumber); 1286 numOfCollisions = G4Poisson(meanNumber);
1304 1287
1305 // G4cout<<"numOfCollisions = "<<numOfCol 1288 // G4cout<<"numOfCollisions = "<<numOfCollisions<<G4endl;
1306 1289
1307 while(numOfCollisions) 1290 while(numOfCollisions)
1308 { 1291 {
1309 position = fIntegralPlasmon[1]*G4UniformR 1292 position = fIntegralPlasmon[1]*G4UniformRand();
1310 1293
1311 for( iTransfer=1; iTransfer<=fSplineNumbe 1294 for( iTransfer=1; iTransfer<=fSplineNumber; iTransfer++ )
1312 { 1295 {
1313 if( position >= fIntegralPlasmon[iTra 1296 if( position >= fIntegralPlasmon[iTransfer] ) break;
1314 } 1297 }
1315 loss += fSplineEnergy[iTransfer] ; 1298 loss += fSplineEnergy[iTransfer] ;
1316 numOfCollisions--; 1299 numOfCollisions--;
1317 // Loop checking, 03-Aug-2015, Vladimir I <<
1318 } 1300 }
1319 // G4cout<<"PAI Plasmon loss = "<<loss/keV< 1301 // G4cout<<"PAI Plasmon loss = "<<loss/keV<<" keV"<<G4endl;
1320 1302
1321 return loss; 1303 return loss;
1322 } 1304 }
1323 1305
1324 ///////////////////////////////////////////// 1306 /////////////////////////////////////////////////////////////////////////////
1325 // 1307 //
1326 1308
1327 void G4PAIySection::CallError(G4int i, const 1309 void G4PAIySection::CallError(G4int i, const G4String& methodName) const
1328 { 1310 {
1329 G4String head = "G4PAIySection::" + methodN 1311 G4String head = "G4PAIySection::" + methodName + "()";
1330 G4ExceptionDescription ed; 1312 G4ExceptionDescription ed;
1331 ed << "Wrong index " << i << " fSplineNumbe << 1313 ed << "Wrong index " << i << " fSplineNumber= " << fSplineNumber << G4endl;
1332 G4Exception(head,"pai001",FatalException,ed 1314 G4Exception(head,"pai001",FatalException,ed);
1333 } 1315 }
1334 1316
1335 ///////////////////////////////////////////// 1317 /////////////////////////////////////////////////////////////////////////////
1336 // 1318 //
1337 // Init array of Lorentz factors 1319 // Init array of Lorentz factors
1338 // 1320 //
1339 1321
1340 G4int G4PAIySection::fNumberOfGammas = 111; 1322 G4int G4PAIySection::fNumberOfGammas = 111;
1341 1323
1342 const G4double G4PAIySection::fLorentzFactor[ 1324 const G4double G4PAIySection::fLorentzFactor[112] = // fNumberOfGammas+1
1343 { 1325 {
1344 0.0, 1326 0.0,
1345 1.094989e+00, 1.107813e+00, 1.122369e+00, 1.1 1327 1.094989e+00, 1.107813e+00, 1.122369e+00, 1.138890e+00, 1.157642e+00,
1346 1.178925e+00, 1.203082e+00, 1.230500e+00, 1.2 1328 1.178925e+00, 1.203082e+00, 1.230500e+00, 1.261620e+00, 1.296942e+00, // 10
1347 1.337032e+00, 1.382535e+00, 1.434181e+00, 1.4 1329 1.337032e+00, 1.382535e+00, 1.434181e+00, 1.492800e+00, 1.559334e+00,
1348 1.634850e+00, 1.720562e+00, 1.817845e+00, 1.9 1330 1.634850e+00, 1.720562e+00, 1.817845e+00, 1.928263e+00, 2.053589e+00, // 20
1349 2.195835e+00, 2.357285e+00, 2.540533e+00, 2.7 1331 2.195835e+00, 2.357285e+00, 2.540533e+00, 2.748522e+00, 2.984591e+00,
1350 3.252533e+00, 3.556649e+00, 3.901824e+00, 4.2 1332 3.252533e+00, 3.556649e+00, 3.901824e+00, 4.293602e+00, 4.738274e+00, // 30
1351 5.242981e+00, 5.815829e+00, 6.466019e+00, 7.2 1333 5.242981e+00, 5.815829e+00, 6.466019e+00, 7.203990e+00, 8.041596e+00,
1352 8.992288e+00, 1.007133e+01, 1.129606e+01, 1.2 1334 8.992288e+00, 1.007133e+01, 1.129606e+01, 1.268614e+01, 1.426390e+01, // 40
1353 1.605467e+01, 1.808721e+01, 2.039417e+01, 2.3 1335 1.605467e+01, 1.808721e+01, 2.039417e+01, 2.301259e+01, 2.598453e+01,
1354 2.935771e+01, 3.318630e+01, 3.753180e+01, 4.2 1336 2.935771e+01, 3.318630e+01, 3.753180e+01, 4.246399e+01, 4.806208e+01, // 50
1355 5.441597e+01, 6.162770e+01, 6.981310e+01, 7.9 1337 5.441597e+01, 6.162770e+01, 6.981310e+01, 7.910361e+01, 8.964844e+01,
1356 1.016169e+02, 1.152013e+02, 1.306197e+02, 1.4 1338 1.016169e+02, 1.152013e+02, 1.306197e+02, 1.481198e+02, 1.679826e+02, // 60
1357 1.905270e+02, 2.161152e+02, 2.451581e+02, 2.7 1339 1.905270e+02, 2.161152e+02, 2.451581e+02, 2.781221e+02, 3.155365e+02,
1358 3.580024e+02, 4.062016e+02, 4.609081e+02, 5.2 1340 3.580024e+02, 4.062016e+02, 4.609081e+02, 5.230007e+02, 5.934765e+02, // 70
1359 6.734672e+02, 7.642575e+02, 8.673056e+02, 9.8 1341 6.734672e+02, 7.642575e+02, 8.673056e+02, 9.842662e+02, 1.117018e+03,
1360 1.267692e+03, 1.438709e+03, 1.632816e+03, 1.8 1342 1.267692e+03, 1.438709e+03, 1.632816e+03, 1.853128e+03, 2.103186e+03, // 80
1361 2.387004e+03, 2.709140e+03, 3.074768e+03, 3.4 1343 2.387004e+03, 2.709140e+03, 3.074768e+03, 3.489760e+03, 3.960780e+03,
1362 4.495394e+03, 5.102185e+03, 5.790900e+03, 6.5 1344 4.495394e+03, 5.102185e+03, 5.790900e+03, 6.572600e+03, 7.459837e+03, // 90
1363 8.466860e+03, 9.609843e+03, 1.090714e+04, 1.2 1345 8.466860e+03, 9.609843e+03, 1.090714e+04, 1.237959e+04, 1.405083e+04,
1364 1.594771e+04, 1.810069e+04, 2.054434e+04, 2.3 1346 1.594771e+04, 1.810069e+04, 2.054434e+04, 2.331792e+04, 2.646595e+04, // 100
1365 3.003901e+04, 3.409446e+04, 3.869745e+04, 4.3 1347 3.003901e+04, 3.409446e+04, 3.869745e+04, 4.392189e+04, 4.985168e+04,
1366 5.658206e+04, 6.422112e+04, 7.289153e+04, 8.2 1348 5.658206e+04, 6.422112e+04, 7.289153e+04, 8.273254e+04, 9.390219e+04, // 110
1367 1.065799e+05 1349 1.065799e+05
1368 }; 1350 };
1369 1351
1370 ///////////////////////////////////////////// 1352 ///////////////////////////////////////////////////////////////////////
1371 // 1353 //
1372 // The number of gamma for creation of splin 1354 // The number of gamma for creation of spline (near ion-min , G ~ 4 )
1373 // 1355 //
1374 1356
1375 const G4int G4PAIySection::fRefGammaNumber = << 1357 const
>> 1358 G4int G4PAIySection::fRefGammaNumber = 29;
1376 1359
>> 1360
1377 // 1361 //
1378 // end of G4PAIySection implementation file 1362 // end of G4PAIySection implementation file
1379 // 1363 //
1380 ///////////////////////////////////////////// 1364 ////////////////////////////////////////////////////////////////////////////
1381 1365
1382 1366