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>> 26 // $Id: G4PAIySection.cc 96934 2016-05-18 09:10:41Z gcosmo $
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 // 23.06.13 V.Grichine arrays->G4DataVectors
45 // 46 //
46 47
47 #include "G4PAIySection.hh" 48 #include "G4PAIySection.hh"
48 49
49 #include "globals.hh" 50 #include "globals.hh"
50 #include "G4PhysicalConstants.hh" 51 #include "G4PhysicalConstants.hh"
51 #include "G4SystemOfUnits.hh" 52 #include "G4SystemOfUnits.hh"
52 #include "G4ios.hh" 53 #include "G4ios.hh"
53 #include "G4Poisson.hh" 54 #include "G4Poisson.hh"
54 #include "G4Material.hh" 55 #include "G4Material.hh"
55 #include "G4MaterialCutsCouple.hh" 56 #include "G4MaterialCutsCouple.hh"
56 #include "G4SandiaTable.hh" 57 #include "G4SandiaTable.hh"
57 #include "G4Exp.hh" 58 #include "G4Exp.hh"
58 #include "G4Log.hh" 59 #include "G4Log.hh"
59 60
60 using namespace std; 61 using namespace std;
61 62
62 // Local class constants 63 // Local class constants
63 64
64 const G4double G4PAIySection::fDelta = 0.005; 65 const G4double G4PAIySection::fDelta = 0.005; // energy shift from interval border
65 const G4double G4PAIySection::fError = 0.005; 66 const G4double G4PAIySection::fError = 0.005; // error in lin-log approximation
66 67
67 const G4int G4PAIySection::fMaxSplineSize = 50 68 const G4int G4PAIySection::fMaxSplineSize = 500; // Max size of output spline
68 69 // arrays
69 70
70 ////////////////////////////////////////////// 71 //////////////////////////////////////////////////////////////////
71 // 72 //
72 // Constructor 73 // Constructor
73 // 74 //
74 75
75 G4PAIySection::G4PAIySection() 76 G4PAIySection::G4PAIySection()
76 { 77 {
77 fSandia = nullptr; << 78 fSandia = 0;
78 fDensity = fElectronDensity = fNormalization 79 fDensity = fElectronDensity = fNormalizationCof = fLowEnergyCof = 0.0;
79 fIntervalNumber = fSplineNumber = 0; 80 fIntervalNumber = fSplineNumber = 0;
80 fVerbose = 0; 81 fVerbose = 0;
81 82
82 betaBohr = fine_structure_const; 83 betaBohr = fine_structure_const;
83 G4double cofBetaBohr = 4.0; 84 G4double cofBetaBohr = 4.0;
84 G4double betaBohr2 = fine_structure_const*fi << 85 G4double betaBohr2 = fine_structure_const*fine_structure_const;
85 betaBohr4 = betaBohr2*betaBohr2*cofBetaBohr; << 86 betaBohr4 = betaBohr2*betaBohr2*cofBetaBohr;
86 87
87 fSplineEnergy = G4DataVector(fMaxSp 88 fSplineEnergy = G4DataVector(fMaxSplineSize,0.0);
88 fRePartDielectricConst = G4DataVector(fMaxSp 89 fRePartDielectricConst = G4DataVector(fMaxSplineSize,0.0);
89 fImPartDielectricConst = G4DataVector(fMaxSp 90 fImPartDielectricConst = G4DataVector(fMaxSplineSize,0.0);
90 fIntegralTerm = G4DataVector(fMaxSp 91 fIntegralTerm = G4DataVector(fMaxSplineSize,0.0);
91 fDifPAIySection = G4DataVector(fMaxSp 92 fDifPAIySection = G4DataVector(fMaxSplineSize,0.0);
92 fdNdxCerenkov = G4DataVector(fMaxSp 93 fdNdxCerenkov = G4DataVector(fMaxSplineSize,0.0);
93 fdNdxPlasmon = G4DataVector(fMaxSp 94 fdNdxPlasmon = G4DataVector(fMaxSplineSize,0.0);
94 fIntegralPAIySection = G4DataVector(fMaxSp 95 fIntegralPAIySection = G4DataVector(fMaxSplineSize,0.0);
95 fIntegralPAIdEdx = G4DataVector(fMaxSp 96 fIntegralPAIdEdx = G4DataVector(fMaxSplineSize,0.0);
96 fIntegralCerenkov = G4DataVector(fMaxSp 97 fIntegralCerenkov = G4DataVector(fMaxSplineSize,0.0);
97 fIntegralPlasmon = G4DataVector(fMaxSp 98 fIntegralPlasmon = G4DataVector(fMaxSplineSize,0.0);
98 99
99 for( G4int i = 0; i < 500; ++i ) 100 for( G4int i = 0; i < 500; ++i )
100 { 101 {
101 for( G4int j = 0; j < 112; ++j ) { fPAItab 102 for( G4int j = 0; j < 112; ++j ) { fPAItable[i][j] = 0.0; }
102 } 103 }
103 } 104 }
104 105
105 ////////////////////////////////////////////// 106 ////////////////////////////////////////////////////////////////////////////
106 // 107 //
107 // << 108 // Destructor
108 109
109 G4double G4PAIySection::GetLorentzFactor(G4int << 110 G4PAIySection::~G4PAIySection()
110 { << 111 {}
111 return fLorentzFactor[j]; <<
112 } <<
113 112
114 ////////////////////////////////////////////// 113 ////////////////////////////////////////////////////////////////////////
115 // 114 //
116 // Constructor with beta*gamma square value ca 115 // Constructor with beta*gamma square value called from G4PAIModel
117 116
118 void G4PAIySection::Initialize( const G4Materi 117 void G4PAIySection::Initialize( const G4Material* material,
119 G4double maxEn 118 G4double maxEnergyTransfer,
120 G4double betaG 119 G4double betaGammaSq,
121 G4SandiaTable* 120 G4SandiaTable* sandia)
122 { 121 {
123 if(fVerbose > 0) 122 if(fVerbose > 0)
124 { 123 {
125 G4cout<<G4endl; 124 G4cout<<G4endl;
126 G4cout<<"G4PAIySection::Initialize(...,G4S 125 G4cout<<"G4PAIySection::Initialize(...,G4SandiaTable* sandia)"<<G4endl;
127 G4cout<<G4endl; 126 G4cout<<G4endl;
128 } 127 }
129 G4int i, j; 128 G4int i, j;
130 129
131 fSandia = sandia; 130 fSandia = sandia;
132 fIntervalNumber = sandia->GetMaxInterval(); 131 fIntervalNumber = sandia->GetMaxInterval();
133 fDensity = material->GetDensity(); 132 fDensity = material->GetDensity();
134 fElectronDensity = material->GetElectronDens 133 fElectronDensity = material->GetElectronDensity();
135 134
136 // fIntervalNumber--; 135 // fIntervalNumber--;
137 136
138 if( fVerbose > 0 ) 137 if( fVerbose > 0 )
139 { 138 {
140 G4cout<<"fDensity = "<<fDensity<<"\t"<<fEl 139 G4cout<<"fDensity = "<<fDensity<<"\t"<<fElectronDensity<<"\t fIntervalNumber = "
141 <<fIntervalNumber<< " (beta*gamma)^2 140 <<fIntervalNumber<< " (beta*gamma)^2= " << betaGammaSq << G4endl;
142 } 141 }
143 fEnergyInterval = G4DataVector(fIntervalNumb 142 fEnergyInterval = G4DataVector(fIntervalNumber+2,0.0);
144 fA1 = G4DataVector(fIntervalNumb 143 fA1 = G4DataVector(fIntervalNumber+2,0.0);
145 fA2 = G4DataVector(fIntervalNumb 144 fA2 = G4DataVector(fIntervalNumber+2,0.0);
146 fA3 = G4DataVector(fIntervalNumb 145 fA3 = G4DataVector(fIntervalNumber+2,0.0);
147 fA4 = G4DataVector(fIntervalNumb 146 fA4 = G4DataVector(fIntervalNumber+2,0.0);
148 147
149 for( i = 1; i <= fIntervalNumber; ++i ) << 148 for( i = 1; i <= fIntervalNumber; i++ )
150 { 149 {
151 if ( sandia->GetSandiaMatTablePAI(i-1,0) < 150 if ( sandia->GetSandiaMatTablePAI(i-1,0) < 1.*eV )
152 { 151 {
153 fIntervalNumber--; 152 fIntervalNumber--;
154 continue; 153 continue;
155 } 154 }
156 if( ( sandia->GetSandiaMatTablePAI(i-1,0) 155 if( ( sandia->GetSandiaMatTablePAI(i-1,0) >= maxEnergyTransfer )
157 || i >= fIntervalNumber ) 156 || i >= fIntervalNumber )
158 { 157 {
159 fEnergyInterval[i] = maxEnergyTransfer; 158 fEnergyInterval[i] = maxEnergyTransfer;
160 fIntervalNumber = i; 159 fIntervalNumber = i;
161 break; 160 break;
162 } 161 }
163 fEnergyInterval[i] = sandia->GetSandiaMatT 162 fEnergyInterval[i] = sandia->GetSandiaMatTablePAI(i-1,0);
164 fA1[i] = sandia->GetSandiaMatT 163 fA1[i] = sandia->GetSandiaMatTablePAI(i-1,1);
165 fA2[i] = sandia->GetSandiaMatT 164 fA2[i] = sandia->GetSandiaMatTablePAI(i-1,2);
166 fA3[i] = sandia->GetSandiaMatT 165 fA3[i] = sandia->GetSandiaMatTablePAI(i-1,3);
167 fA4[i] = sandia->GetSandiaMatT 166 fA4[i] = sandia->GetSandiaMatTablePAI(i-1,4);
168 167
169 if( fVerbose > 0 ) { 168 if( fVerbose > 0 ) {
170 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV< 169 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV<<"\t"<<fA1[i]<<"\t"<<fA2[i]<<"\t"
171 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4en 170 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl;
172 } 171 }
173 } 172 }
174 if( fVerbose > 0 ) { 173 if( fVerbose > 0 ) {
175 G4cout<<"last i = "<<i<<"; "<<"fIntervalNu 174 G4cout<<"last i = "<<i<<"; "<<"fIntervalNumber = "
176 <<fIntervalNumber<<G4endl; 175 <<fIntervalNumber<<G4endl;
177 } 176 }
178 if( fEnergyInterval[fIntervalNumber] != maxE 177 if( fEnergyInterval[fIntervalNumber] != maxEnergyTransfer )
179 { 178 {
180 fIntervalNumber++; 179 fIntervalNumber++;
181 fEnergyInterval[fIntervalNumber] = maxEn 180 fEnergyInterval[fIntervalNumber] = maxEnergyTransfer;
182 } 181 }
183 if( fVerbose > 0 ) 182 if( fVerbose > 0 )
184 { 183 {
185 for( i = 1; i <= fIntervalNumber; ++i ) << 184 for( i = 1; i <= fIntervalNumber; i++ )
186 { 185 {
187 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV< 186 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV<<"\t"<<fA1[i]<<"\t"<<fA2[i]<<"\t"
188 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl; 187 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl;
189 } 188 }
190 } 189 }
191 if( fVerbose > 0 ) { 190 if( fVerbose > 0 ) {
192 G4cout<<"Now checking, if two borders are 191 G4cout<<"Now checking, if two borders are too close together"<<G4endl;
193 } 192 }
194 for( i = 1; i < fIntervalNumber; ++i ) << 193 for( i = 1; i < fIntervalNumber; i++ )
195 { 194 {
196 if( fEnergyInterval[i+1]-fEnergyInterval[i 195 if( fEnergyInterval[i+1]-fEnergyInterval[i] >
197 1.5*fDelta*(fEnergyInterval[i+1]+fEne 196 1.5*fDelta*(fEnergyInterval[i+1]+fEnergyInterval[i]) ) continue;
198 else 197 else
199 { 198 {
200 for( j = i; j < fIntervalNumber; j++ ) 199 for( j = i; j < fIntervalNumber; j++ )
201 { 200 {
202 fEnergyInterval[j] = fEnergyInte 201 fEnergyInterval[j] = fEnergyInterval[j+1];
203 fA1[j] = fA1[j+1]; 202 fA1[j] = fA1[j+1];
204 fA2[j] = fA2[j+1]; 203 fA2[j] = fA2[j+1];
205 fA3[j] = fA3[j+1]; 204 fA3[j] = fA3[j+1];
206 fA4[j] = fA4[j+1]; 205 fA4[j] = fA4[j+1];
207 } 206 }
208 fIntervalNumber--; 207 fIntervalNumber--;
209 } 208 }
210 } 209 }
211 if( fVerbose > 0 ) 210 if( fVerbose > 0 )
212 { 211 {
213 for( i = 1; i <= fIntervalNumber; ++i ) << 212 for( i = 1; i <= fIntervalNumber; i++ )
214 { 213 {
215 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV< 214 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV<<"\t"<<fA1[i]<<"\t"<<fA2[i]<<"\t"
216 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl; 215 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl;
217 } 216 }
218 } 217 }
219 // Preparation of fSplineEnergy array corres 218 // Preparation of fSplineEnergy array corresponding to min ionisation, G~4
220 219
221 ComputeLowEnergyCof(material); 220 ComputeLowEnergyCof(material);
222 221
223 G4double betaGammaSqRef = 222 G4double betaGammaSqRef =
224 fLorentzFactor[fRefGammaNumber]*fLorentzFa 223 fLorentzFactor[fRefGammaNumber]*fLorentzFactor[fRefGammaNumber] - 1;
225 224
226 NormShift(betaGammaSqRef); 225 NormShift(betaGammaSqRef);
227 SplainPAI(betaGammaSqRef); 226 SplainPAI(betaGammaSqRef);
228 227
229 // Preparation of integral PAI cross section 228 // Preparation of integral PAI cross section for input betaGammaSq
230 229
231 for( i = 1; i <= fSplineNumber; ++i ) << 230 for( i = 1; i <= fSplineNumber; i++ )
232 { 231 {
233 fDifPAIySection[i] = DifPAIySection(i,bet 232 fDifPAIySection[i] = DifPAIySection(i,betaGammaSq);
234 233
235 if( fVerbose > 0 ) G4cout<<i<<"; dNdxPAI 234 if( fVerbose > 0 ) G4cout<<i<<"; dNdxPAI = "<<fDifPAIySection[i]<<G4endl;
236 } 235 }
237 IntegralPAIySection(); 236 IntegralPAIySection();
238 } 237 }
239 238
240 ////////////////////////////////////////////// 239 /////////////////////////////////////////////////////////////////////////
241 // 240 //
242 // Compute low energy cof. It reduces PAI xsc 241 // Compute low energy cof. It reduces PAI xsc for Lorentz factors less than 4.
243 // 242 //
244 243
245 void G4PAIySection::ComputeLowEnergyCof(const 244 void G4PAIySection::ComputeLowEnergyCof(const G4Material* material)
246 { 245 {
247 G4int i, numberOfElements = (G4int)material- << 246 G4int i, numberOfElements = material->GetNumberOfElements();
248 G4double sumZ = 0., sumCof = 0.; 247 G4double sumZ = 0., sumCof = 0.;
249 248
250 static const G4double p0 = 1.20923e+00; 249 static const G4double p0 = 1.20923e+00;
251 static const G4double p1 = 3.53256e-01; 250 static const G4double p1 = 3.53256e-01;
252 static const G4double p2 = -1.45052e-03; 251 static const G4double p2 = -1.45052e-03;
253 252
254 G4double* thisMaterialZ = new G4double[num 253 G4double* thisMaterialZ = new G4double[numberOfElements];
255 G4double* thisMaterialCof = new G4double[num 254 G4double* thisMaterialCof = new G4double[numberOfElements];
256 255
257 for( i = 0; i < numberOfElements; ++i ) << 256 for( i = 0; i < numberOfElements; i++ )
258 { 257 {
259 thisMaterialZ[i] = material->GetElement(i) 258 thisMaterialZ[i] = material->GetElement(i)->GetZ();
260 sumZ += thisMaterialZ[i]; 259 sumZ += thisMaterialZ[i];
261 thisMaterialCof[i] = p0+p1*thisMaterialZ[i 260 thisMaterialCof[i] = p0+p1*thisMaterialZ[i]+p2*thisMaterialZ[i]*thisMaterialZ[i];
262 } 261 }
263 for( i = 0; i < numberOfElements; ++i ) << 262 for( i = 0; i < numberOfElements; i++ )
264 { 263 {
265 sumCof += thisMaterialCof[i]*thisMaterialZ 264 sumCof += thisMaterialCof[i]*thisMaterialZ[i]/sumZ;
266 } 265 }
267 fLowEnergyCof = sumCof; 266 fLowEnergyCof = sumCof;
268 delete [] thisMaterialZ; 267 delete [] thisMaterialZ;
269 delete [] thisMaterialCof; 268 delete [] thisMaterialCof;
270 // G4cout<<"fLowEnergyCof = "<<fLowEnergyCof 269 // G4cout<<"fLowEnergyCof = "<<fLowEnergyCof<<G4endl;
271 } 270 }
272 271
273 ////////////////////////////////////////////// 272 /////////////////////////////////////////////////////////////////////////
274 // 273 //
275 // General control function for class G4PAIySe 274 // General control function for class G4PAIySection
276 // 275 //
277 276
278 void G4PAIySection::InitPAI() 277 void G4PAIySection::InitPAI()
279 { 278 {
280 G4int i; 279 G4int i;
281 G4double betaGammaSq = fLorentzFactor[fRefG 280 G4double betaGammaSq = fLorentzFactor[fRefGammaNumber]*
282 fLorentzFactor[fRefG 281 fLorentzFactor[fRefGammaNumber] - 1;
283 282
284 // Preparation of integral PAI cross sectio 283 // Preparation of integral PAI cross section for reference gamma
285 284
286 NormShift(betaGammaSq); 285 NormShift(betaGammaSq);
287 SplainPAI(betaGammaSq); 286 SplainPAI(betaGammaSq);
288 287
289 IntegralPAIySection(); 288 IntegralPAIySection();
290 IntegralCerenkov(); 289 IntegralCerenkov();
291 IntegralPlasmon(); 290 IntegralPlasmon();
292 291
293 for( i = 0; i<= fSplineNumber; ++i) << 292 for( i = 0; i<= fSplineNumber; i++)
294 { 293 {
295 fPAItable[i][fRefGammaNumber] = fIntegral 294 fPAItable[i][fRefGammaNumber] = fIntegralPAIySection[i];
296 295
297 if(i != 0) fPAItable[i][0] = fSplineEner 296 if(i != 0) fPAItable[i][0] = fSplineEnergy[i];
298 } 297 }
299 fPAItable[0][0] = fSplineNumber; 298 fPAItable[0][0] = fSplineNumber;
300 299
301 for( G4int j = 1; j < 112; ++j) // fo << 300 for( G4int j = 1; j < 112; j++) // for other gammas
302 { 301 {
303 if( j == fRefGammaNumber ) continue; 302 if( j == fRefGammaNumber ) continue;
304 303
305 betaGammaSq = fLorentzFactor[j]*fLorentz 304 betaGammaSq = fLorentzFactor[j]*fLorentzFactor[j] - 1;
306 305
307 for(i = 1; i <= fSplineNumber; ++i) << 306 for(i = 1; i <= fSplineNumber; i++)
308 { 307 {
309 fDifPAIySection[i] = DifPAIySection(i 308 fDifPAIySection[i] = DifPAIySection(i,betaGammaSq);
310 fdNdxCerenkov[i] = PAIdNdxCerenkov( 309 fdNdxCerenkov[i] = PAIdNdxCerenkov(i,betaGammaSq);
311 fdNdxPlasmon[i] = PAIdNdxPlasmon(i 310 fdNdxPlasmon[i] = PAIdNdxPlasmon(i,betaGammaSq);
312 } 311 }
313 IntegralPAIySection(); 312 IntegralPAIySection();
314 IntegralCerenkov(); 313 IntegralCerenkov();
315 IntegralPlasmon(); 314 IntegralPlasmon();
316 315
317 for(i = 0; i <= fSplineNumber; ++i) << 316 for(i = 0; i <= fSplineNumber; i++)
318 { 317 {
319 fPAItable[i][j] = fIntegralPAIySection 318 fPAItable[i][j] = fIntegralPAIySection[i];
320 } 319 }
321 } 320 }
322 } 321 }
323 322
324 ////////////////////////////////////////////// 323 ///////////////////////////////////////////////////////////////////////
325 // 324 //
326 // Shifting from borders to intervals Creation 325 // Shifting from borders to intervals Creation of first energy points
327 // 326 //
328 327
329 void G4PAIySection::NormShift(G4double betaGam 328 void G4PAIySection::NormShift(G4double betaGammaSq)
330 { 329 {
331 G4int i, j; 330 G4int i, j;
332 331
333 for( i = 1; i <= fIntervalNumber-1; ++i) << 332 for( i = 1; i <= fIntervalNumber-1; i++ )
334 { 333 {
335 for( j = 1; j <= 2; ++j) << 334 for( j = 1; j <= 2; j++ )
336 { 335 {
337 fSplineNumber = (i-1)*2 + j; 336 fSplineNumber = (i-1)*2 + j;
338 337
339 if( j == 1 ) fSplineEnergy[fSplineNumber 338 if( j == 1 ) fSplineEnergy[fSplineNumber] = fEnergyInterval[i ]*(1+fDelta);
340 else fSplineEnergy[fSplineNumber 339 else fSplineEnergy[fSplineNumber] = fEnergyInterval[i+1]*(1-fDelta);
341 // G4cout<<"cn = "<<fSplineNumber<<"; 340 // G4cout<<"cn = "<<fSplineNumber<<"; "<<"energy = "
342 // <<fSplineEnergy[fSplineNumber]<<G4en 341 // <<fSplineEnergy[fSplineNumber]<<G4endl;
343 } 342 }
344 } 343 }
345 fIntegralTerm[1]=RutherfordIntegral(1,fEnerg 344 fIntegralTerm[1]=RutherfordIntegral(1,fEnergyInterval[1],fSplineEnergy[1]);
346 345
347 j = 1; 346 j = 1;
348 347
349 for(i=2;i<=fSplineNumber;++i) << 348 for(i=2;i<=fSplineNumber;i++)
350 { 349 {
351 if(fSplineEnergy[i]<fEnergyInterval[j+1]) 350 if(fSplineEnergy[i]<fEnergyInterval[j+1])
352 { 351 {
353 fIntegralTerm[i] = fIntegralTerm[i-1] 352 fIntegralTerm[i] = fIntegralTerm[i-1] +
354 RutherfordIntegral 353 RutherfordIntegral(j,fSplineEnergy[i-1],
355 354 fSplineEnergy[i] );
356 } 355 }
357 else 356 else
358 { 357 {
359 G4double x = RutherfordIntegral(j,fSpli 358 G4double x = RutherfordIntegral(j,fSplineEnergy[i-1],
360 fEn 359 fEnergyInterval[j+1] );
361 j++; 360 j++;
362 fIntegralTerm[i] = fIntegralTerm[i-1] 361 fIntegralTerm[i] = fIntegralTerm[i-1] + x +
363 RutherfordIntegral 362 RutherfordIntegral(j,fEnergyInterval[j],
364 363 fSplineEnergy[i] );
365 } 364 }
366 // G4cout<<i<<"\t"<<fSplineEnergy[i]<<"\t" 365 // G4cout<<i<<"\t"<<fSplineEnergy[i]<<"\t"<<fIntegralTerm[i]<<"\n"<<G4endl;
367 } 366 }
368 static const G4double nfactor = 367 static const G4double nfactor =
369 2*pi*pi*hbarc*hbarc*fine_structure_const/e 368 2*pi*pi*hbarc*hbarc*fine_structure_const/electron_mass_c2;
370 fNormalizationCof = nfactor*fElectronDensity 369 fNormalizationCof = nfactor*fElectronDensity/fIntegralTerm[fSplineNumber];
371 370
372 // G4cout<<"fNormalizationCof = "<<fNormaliz 371 // G4cout<<"fNormalizationCof = "<<fNormalizationCof<<G4endl;
373 372
374 // Calculation of PAI differrential cross-se << 373 // Calculation of PAI differrential cross-section (1/(keV*cm))
375 // in the energy points near borders of ener << 374 // in the energy points near borders of energy intervals
376 375
377 for(G4int k=1; k<=fIntervalNumber-1; ++k) << 376 for(G4int k=1;k<=fIntervalNumber-1;k++)
378 { 377 {
379 for(j=1; j<=2; ++j) << 378 for(j=1;j<=2;j++)
380 { 379 {
381 i = (k-1)*2 + j; 380 i = (k-1)*2 + j;
382 fImPartDielectricConst[i] = fNormaliz 381 fImPartDielectricConst[i] = fNormalizationCof*
383 ImPartDie 382 ImPartDielectricConst(k,fSplineEnergy[i]);
384 fRePartDielectricConst[i] = fNormaliz 383 fRePartDielectricConst[i] = fNormalizationCof*
385 RePartDie 384 RePartDielectricConst(fSplineEnergy[i]);
386 fIntegralTerm[i] *= fNormalizationCof 385 fIntegralTerm[i] *= fNormalizationCof;
387 386
388 fDifPAIySection[i] = DifPAIySection(i 387 fDifPAIySection[i] = DifPAIySection(i,betaGammaSq);
389 fdNdxCerenkov[i] = PAIdNdxCerenkov( 388 fdNdxCerenkov[i] = PAIdNdxCerenkov(i,betaGammaSq);
390 fdNdxPlasmon[i] = PAIdNdxPlasmon(i 389 fdNdxPlasmon[i] = PAIdNdxPlasmon(i,betaGammaSq);
391 } 390 }
392 } 391 }
393 392
394 } // end of NormShift 393 } // end of NormShift
395 394
396 ////////////////////////////////////////////// 395 /////////////////////////////////////////////////////////////////////////
397 // 396 //
398 // Creation of new energy points as geometrica 397 // Creation of new energy points as geometrical mean of existing
399 // one, calculation PAI_cs for them, while the 398 // one, calculation PAI_cs for them, while the error of logarithmic
400 // linear approximation would be smaller than 399 // linear approximation would be smaller than 'fError'
401 400
402 void G4PAIySection::SplainPAI(G4double betaGam 401 void G4PAIySection::SplainPAI(G4double betaGammaSq)
403 { 402 {
404 G4int k = 1; 403 G4int k = 1;
405 G4int i = 1; 404 G4int i = 1;
406 405
407 while ( (i < fSplineNumber) && (fSplineNumb 406 while ( (i < fSplineNumber) && (fSplineNumber < fMaxSplineSize-1) )
408 { 407 {
409 if(fSplineEnergy[i+1] > fEnergyInterval[ 408 if(fSplineEnergy[i+1] > fEnergyInterval[k+1])
410 { 409 {
411 k++; // Here next energy point is 410 k++; // Here next energy point is in next energy interval
412 ++i; << 411 i++;
413 continue; 412 continue;
414 } 413 }
415 // Shifting of arrayes for inserting the << 414 // Shifting of arrayes for inserting the geometrical
416 // average of 'i' and 'i+1' energy point << 415 // average of 'i' and 'i+1' energy points to 'i+1' place
417 fSplineNumber++; 416 fSplineNumber++;
418 417
419 for(G4int j = fSplineNumber; j >= i+2; j 418 for(G4int j = fSplineNumber; j >= i+2; j-- )
420 { 419 {
421 fSplineEnergy[j] = fSplineEn 420 fSplineEnergy[j] = fSplineEnergy[j-1];
422 fImPartDielectricConst[j] = fImPartDi 421 fImPartDielectricConst[j] = fImPartDielectricConst[j-1];
423 fRePartDielectricConst[j] = fRePartDi 422 fRePartDielectricConst[j] = fRePartDielectricConst[j-1];
424 fIntegralTerm[j] = fIntegral 423 fIntegralTerm[j] = fIntegralTerm[j-1];
425 424
426 fDifPAIySection[j] = fDifPAIySection[ 425 fDifPAIySection[j] = fDifPAIySection[j-1];
427 fdNdxCerenkov[j] = fdNdxCerenkov[j- 426 fdNdxCerenkov[j] = fdNdxCerenkov[j-1];
428 fdNdxPlasmon[j] = fdNdxPlasmon[j-1 427 fdNdxPlasmon[j] = fdNdxPlasmon[j-1];
429 } 428 }
430 G4double x1 = fSplineEnergy[i]; 429 G4double x1 = fSplineEnergy[i];
431 G4double x2 = fSplineEnergy[i+1]; 430 G4double x2 = fSplineEnergy[i+1];
432 G4double yy1 = fDifPAIySection[i]; 431 G4double yy1 = fDifPAIySection[i];
433 G4double y2 = fDifPAIySection[i+1]; 432 G4double y2 = fDifPAIySection[i+1];
434 433
435 G4double en1 = sqrt(x1*x2); 434 G4double en1 = sqrt(x1*x2);
436 fSplineEnergy[i+1] = en1; 435 fSplineEnergy[i+1] = en1;
437 436
438 // Calculation of logarithmic linear app << 437 // Calculation of logarithmic linear approximation
439 // in this (enr) energy point, which num << 438 // in this (enr) energy point, which number is 'i+1' now
440 439
441 G4double a = log10(y2/yy1)/log10(x2/x1); 440 G4double a = log10(y2/yy1)/log10(x2/x1);
442 G4double b = log10(yy1) - a*log10(x1); 441 G4double b = log10(yy1) - a*log10(x1);
443 G4double y = a*log10(en1) + b; 442 G4double y = a*log10(en1) + b;
444 y = pow(10.,y); 443 y = pow(10.,y);
445 444
446 // Calculation of the PAI dif. cross-sec << 445 // Calculation of the PAI dif. cross-section at this point
447 446
448 fImPartDielectricConst[i+1] = fNormaliza 447 fImPartDielectricConst[i+1] = fNormalizationCof*
449 ImPartDiel 448 ImPartDielectricConst(k,fSplineEnergy[i+1]);
450 fRePartDielectricConst[i+1] = fNormaliza 449 fRePartDielectricConst[i+1] = fNormalizationCof*
451 RePartDiel 450 RePartDielectricConst(fSplineEnergy[i+1]);
452 fIntegralTerm[i+1] = fIntegralTerm[i] + 451 fIntegralTerm[i+1] = fIntegralTerm[i] + fNormalizationCof*
453 RutherfordIntegral( 452 RutherfordIntegral(k,fSplineEnergy[i],
454 453 fSplineEnergy[i+1]);
455 454
456 fDifPAIySection[i+1] = DifPAIySection(i+ 455 fDifPAIySection[i+1] = DifPAIySection(i+1,betaGammaSq);
457 fdNdxCerenkov[i+1] = PAIdNdxCerenkov(i 456 fdNdxCerenkov[i+1] = PAIdNdxCerenkov(i+1,betaGammaSq);
458 fdNdxPlasmon[i+1] = PAIdNdxPlasmon(i+ 457 fdNdxPlasmon[i+1] = PAIdNdxPlasmon(i+1,betaGammaSq);
459 458
460 // Condition for next divisi 459 // Condition for next division of this segment or to pass
461 // to higher energies 460 // to higher energies
462 461
463 G4double x = 2*(fDifPAIySection[i+1] - y 462 G4double x = 2*(fDifPAIySection[i+1] - y)/(fDifPAIySection[i+1] + y);
464 463
465 G4double delta = 2.*(fSplineEnergy[i+1]- 464 G4double delta = 2.*(fSplineEnergy[i+1]-fSplineEnergy[i])
466 /(fSplineEnergy[i+1]+fSplineEnergy[i]) << 465 /(fSplineEnergy[i+1]+fSplineEnergy[i]);
467 466
468 if( x < 0 ) 467 if( x < 0 )
469 { 468 {
470 x = -x; 469 x = -x;
471 } 470 }
472 if( x > fError && fSplineNumber < fMaxSp 471 if( x > fError && fSplineNumber < fMaxSplineSize-1 && delta > 2.*fDelta )
473 { 472 {
474 continue; // next division 473 continue; // next division
475 } 474 }
476 i += 2; // pass to next segment 475 i += 2; // pass to next segment
477 476
478 // Loop checking, 03-Aug-2015, Vladimir 477 // Loop checking, 03-Aug-2015, Vladimir Ivanchenko
479 } // close 'while' 478 } // close 'while'
480 479
481 } // end of SplainPAI 480 } // end of SplainPAI
482 481
483 482
484 ////////////////////////////////////////////// 483 ////////////////////////////////////////////////////////////////////
485 // 484 //
486 // Integration over electrons that could be co 485 // Integration over electrons that could be considered
487 // quasi-free at energy transfer of interest 486 // quasi-free at energy transfer of interest
488 487
489 G4double G4PAIySection::RutherfordIntegral( G4 488 G4double G4PAIySection::RutherfordIntegral( G4int k,
490 G4 489 G4double x1,
491 490 G4double x2 )
492 { 491 {
493 G4double c1, c2, c3; 492 G4double c1, c2, c3;
494 // G4cout<<"RI: x1 = "<<x1<<"; "<<"x2 = "<< 493 // G4cout<<"RI: x1 = "<<x1<<"; "<<"x2 = "<<x2<<G4endl;
495 G4double x12 = x1*x2; 494 G4double x12 = x1*x2;
496 c1 = (x2 - x1)/x12; 495 c1 = (x2 - x1)/x12;
497 c2 = (x2 - x1)*(x2 + x1)/(x12*x12); 496 c2 = (x2 - x1)*(x2 + x1)/(x12*x12);
498 c3 = (x2 - x1)*(x1*x1 + x1*x2 + x2*x2)/(x12 497 c3 = (x2 - x1)*(x1*x1 + x1*x2 + x2*x2)/(x12*x12*x12);
499 // G4cout<<" RI: c1 = "<<c1<<"; "<<"c2 = "< 498 // G4cout<<" RI: c1 = "<<c1<<"; "<<"c2 = "<<c2<<"; "<<"c3 = "<<c3<<G4endl;
500 499
501 return fA1[k]*log(x2/x1) + fA2[k]*c1 + fA3 500 return fA1[k]*log(x2/x1) + fA2[k]*c1 + fA3[k]*c2/2 + fA4[k]*c3/3;
502 501
503 } // end of RutherfordIntegral 502 } // end of RutherfordIntegral
504 503
505 504
506 ////////////////////////////////////////////// 505 /////////////////////////////////////////////////////////////////
507 // 506 //
508 // Imaginary part of dielectric constant 507 // Imaginary part of dielectric constant
509 // (G4int k - interval number, G4double en1 - 508 // (G4int k - interval number, G4double en1 - energy point)
510 509
511 G4double G4PAIySection::ImPartDielectricConst( << 510 G4double G4PAIySection::ImPartDielectricConst( G4int k ,
>> 511 G4double energy1 )
512 { 512 {
513 G4double energy2,energy3,energy4,result; 513 G4double energy2,energy3,energy4,result;
514 514
515 energy2 = energy1*energy1; 515 energy2 = energy1*energy1;
516 energy3 = energy2*energy1; 516 energy3 = energy2*energy1;
517 energy4 = energy3*energy1; 517 energy4 = energy3*energy1;
518 518
519 result = fA1[k]/energy1+fA2[k]/energy2+fA3[ 519 result = fA1[k]/energy1+fA2[k]/energy2+fA3[k]/energy3+fA4[k]/energy4;
520 result *=hbarc/energy1; 520 result *=hbarc/energy1;
521 521
522 return result; 522 return result;
523 523
524 } // end of ImPartDielectricConst 524 } // end of ImPartDielectricConst
525 525
526 526
527 ////////////////////////////////////////////// 527 //////////////////////////////////////////////////////////////////////////////
528 // 528 //
529 // Real part of dielectric constant minus unit 529 // Real part of dielectric constant minus unit: epsilon_1 - 1
530 // (G4double enb - energy point) 530 // (G4double enb - energy point)
531 // 531 //
532 532
533 G4double G4PAIySection::RePartDielectricConst( 533 G4double G4PAIySection::RePartDielectricConst(G4double enb)
534 { 534 {
535 G4double x0, x02, x03, x04, x05, x1, x2, xx 535 G4double x0, x02, x03, x04, x05, x1, x2, xx1 ,xx2 , xx12,
536 c1, c2, c3, cof1, cof2, xln1, xln2 536 c1, c2, c3, cof1, cof2, xln1, xln2, xln3, result;
537 537
538 x0 = enb; 538 x0 = enb;
539 result = 0; 539 result = 0;
540 540
541 for(G4int i=1;i<=fIntervalNumber-1;++i) << 541 for(G4int i=1;i<=fIntervalNumber-1;i++)
542 { 542 {
543 x1 = fEnergyInterval[i]; 543 x1 = fEnergyInterval[i];
544 x2 = fEnergyInterval[i+1]; 544 x2 = fEnergyInterval[i+1];
545 xx1 = x1 - x0; 545 xx1 = x1 - x0;
546 xx2 = x2 - x0; 546 xx2 = x2 - x0;
547 xx12 = xx2/xx1; 547 xx12 = xx2/xx1;
548 548
549 if(xx12<0.) << 549 if(xx12<0)
550 { 550 {
551 xx12 = -xx12; 551 xx12 = -xx12;
552 } 552 }
553 xln1 = log(x2/x1); 553 xln1 = log(x2/x1);
554 xln2 = log(xx12); 554 xln2 = log(xx12);
555 xln3 = log((x2 + x0)/(x1 + x0)); 555 xln3 = log((x2 + x0)/(x1 + x0));
556 x02 = x0*x0; 556 x02 = x0*x0;
557 x03 = x02*x0; 557 x03 = x02*x0;
558 x04 = x03*x0; 558 x04 = x03*x0;
559 x05 = x04*x0; 559 x05 = x04*x0;
560 G4double x12 = x1*x2; 560 G4double x12 = x1*x2;
561 c1 = (x2 - x1)/x12; 561 c1 = (x2 - x1)/x12;
562 c2 = (x2 - x1)*(x2 +x1)/(x12*x12); 562 c2 = (x2 - x1)*(x2 +x1)/(x12*x12);
563 c3 = (x2 -x1)*(x1*x1 + x1*x2 + x2*x2)/( 563 c3 = (x2 -x1)*(x1*x1 + x1*x2 + x2*x2)/(x12*x12*x12);
564 564
565 result -= (fA1[i]/x02 + fA3[i]/x04)*xln1 565 result -= (fA1[i]/x02 + fA3[i]/x04)*xln1;
566 result -= (fA2[i]/x02 + fA4[i]/x04)*c1; 566 result -= (fA2[i]/x02 + fA4[i]/x04)*c1;
567 result -= fA3[i]*c2/2/x02; 567 result -= fA3[i]*c2/2/x02;
568 result -= fA4[i]*c3/3/x02; 568 result -= fA4[i]*c3/3/x02;
569 569
570 cof1 = fA1[i]/x02 + fA3[i]/x04; 570 cof1 = fA1[i]/x02 + fA3[i]/x04;
571 cof2 = fA2[i]/x03 + fA4[i]/x05; 571 cof2 = fA2[i]/x03 + fA4[i]/x05;
572 572
573 result += 0.5*(cof1 +cof2)*xln2; 573 result += 0.5*(cof1 +cof2)*xln2;
574 result += 0.5*(cof1 - cof2)*xln3; 574 result += 0.5*(cof1 - cof2)*xln3;
575 } 575 }
576 result *= 2*hbarc/pi; 576 result *= 2*hbarc/pi;
577 577
578 return result; 578 return result;
579 579
580 } // end of RePartDielectricConst 580 } // end of RePartDielectricConst
581 581
582 ////////////////////////////////////////////// 582 //////////////////////////////////////////////////////////////////////
583 // 583 //
584 // PAI differential cross-section in terms of 584 // PAI differential cross-section in terms of
585 // simplified Allison's equation 585 // simplified Allison's equation
586 // 586 //
587 587
588 G4double G4PAIySection::DifPAIySection( G4int 588 G4double G4PAIySection::DifPAIySection( G4int i ,
589 G4doub 589 G4double betaGammaSq )
590 { 590 {
591 G4double beta, be2,cof,x1,x2,x3,x4,x5,x6,x7 << 591 G4double beta, be2,cof,x1,x2,x3,x4,x5,x6,x7,x8,result;
>> 592 //G4double beta, be4;
>> 593 //G4double be4;
>> 594 // G4double betaBohr2 = fine_structure_const*fine_structure_const;
>> 595 // G4double betaBohr4 = betaBohr2*betaBohr2*4.0;
592 be2 = betaGammaSq/(1 + betaGammaSq); 596 be2 = betaGammaSq/(1 + betaGammaSq);
593 beta = std::sqrt(be2); << 597 //be4 = be2*be2;
>> 598 beta = sqrt(be2);
594 cof = 1; 599 cof = 1;
595 x1 = log(2*electron_mass_c2/fSplineEnergy[i 600 x1 = log(2*electron_mass_c2/fSplineEnergy[i]);
596 601
597 if( betaGammaSq < 0.01 ) x2 = log(be2); 602 if( betaGammaSq < 0.01 ) x2 = log(be2);
598 else 603 else
599 { 604 {
600 x2 = -log( (1/betaGammaSq - fRePartDielec 605 x2 = -log( (1/betaGammaSq - fRePartDielectricConst[i])*
601 (1/betaGammaSq - fRePartDielec 606 (1/betaGammaSq - fRePartDielectricConst[i]) +
602 fImPartDielectricConst[i]*fImP 607 fImPartDielectricConst[i]*fImPartDielectricConst[i] )/2;
603 } 608 }
604 if( fImPartDielectricConst[i] == 0.0 ||beta 609 if( fImPartDielectricConst[i] == 0.0 ||betaGammaSq < 0.01 )
605 { 610 {
606 x6=0; 611 x6=0;
607 } 612 }
608 else 613 else
609 { 614 {
610 x3 = -fRePartDielectricConst[i] + 1/betaG 615 x3 = -fRePartDielectricConst[i] + 1/betaGammaSq;
611 x5 = -1 - fRePartDielectricConst[i] + 616 x5 = -1 - fRePartDielectricConst[i] +
612 be2*((1 +fRePartDielectricConst[i])* 617 be2*((1 +fRePartDielectricConst[i])*(1 + fRePartDielectricConst[i]) +
613 fImPartDielectricConst[i]*fImPartDie 618 fImPartDielectricConst[i]*fImPartDielectricConst[i]);
614 619
615 x7 = std::atan2(fImPartDielectricConst[i] << 620 x7 = atan2(fImPartDielectricConst[i],x3);
616 x6 = x5 * x7; 621 x6 = x5 * x7;
617 } 622 }
>> 623 // if(fImPartDielectricConst[i] == 0) x6 = 0;
>> 624
618 x4 = ((x1 + x2)*fImPartDielectricConst[i] + 625 x4 = ((x1 + x2)*fImPartDielectricConst[i] + x6)/hbarc;
>> 626 // if( x4 < 0.0 ) x4 = 0.0;
619 x8 = (1 + fRePartDielectricConst[i])*(1 + f 627 x8 = (1 + fRePartDielectricConst[i])*(1 + fRePartDielectricConst[i]) +
620 fImPartDielectricConst[i]*fImPartDiele 628 fImPartDielectricConst[i]*fImPartDielectricConst[i];
621 629
622 result = (x4 + cof*fIntegralTerm[i]/fSpline 630 result = (x4 + cof*fIntegralTerm[i]/fSplineEnergy[i]/fSplineEnergy[i]);
623 result = std::max(result, 1.0e-8); 631 result = std::max(result, 1.0e-8);
624 result *= fine_structure_const/(be2*pi); << 632 result *= fine_structure_const/be2/pi;
625 // low energy correction 633 // low energy correction
626 634
627 G4double lowCof = fLowEnergyCof; // 6.0 ; / 635 G4double lowCof = fLowEnergyCof; // 6.0 ; // Ar ~ 4.; -> fLowCof as f(Z1,Z2)?
628 636
629 result *= (1 - std::exp(-beta/(betaBohr*low << 637 result *= (1 - exp(-beta/betaBohr/lowCof));
>> 638
>> 639 // result *= (1-exp(-beta/betaBohr))*(1-exp(-beta/betaBohr));
>> 640 // result *= (1-exp(-be2/betaBohr2));
>> 641 // result *= (1-exp(-be4/betaBohr4));
>> 642 // if(fDensity >= 0.1)
630 if(x8 > 0.) 643 if(x8 > 0.)
631 { 644 {
632 result /= x8; << 645 result /= x8;
633 } 646 }
634 return result; 647 return result;
635 648
636 } // end of DifPAIySection 649 } // end of DifPAIySection
637 650
638 ////////////////////////////////////////////// 651 //////////////////////////////////////////////////////////////////////////
639 // 652 //
640 // Calculation od dN/dx of collisions with cre 653 // Calculation od dN/dx of collisions with creation of Cerenkov pseudo-photons
641 654
642 G4double G4PAIySection::PAIdNdxCerenkov( G4int << 655 G4double G4PAIySection::PAIdNdxCerenkov( G4int i ,
>> 656 G4double betaGammaSq )
643 { 657 {
644 G4double logarithm, x3, x5, argument, modul 658 G4double logarithm, x3, x5, argument, modul2, dNdxC;
645 G4double be2, be4; 659 G4double be2, be4;
646 660
>> 661 //G4double cof = 1.0;
>> 662
647 be2 = betaGammaSq/(1 + betaGammaSq); 663 be2 = betaGammaSq/(1 + betaGammaSq);
648 be4 = be2*be2; 664 be4 = be2*be2;
649 665
650 if( betaGammaSq < 0.01 ) logarithm = log(1. 666 if( betaGammaSq < 0.01 ) logarithm = log(1.0+betaGammaSq); // 0.0;
651 else 667 else
652 { 668 {
653 logarithm = -std::log( (1/betaGammaSq - f << 669 logarithm = -log( (1/betaGammaSq - fRePartDielectricConst[i])*
654 (1/betaGammaSq - fRePa 670 (1/betaGammaSq - fRePartDielectricConst[i]) +
655 fImPartDielectricConst 671 fImPartDielectricConst[i]*fImPartDielectricConst[i] )*0.5;
656 logarithm += std::log(1+1.0/betaGammaSq); << 672 logarithm += log(1+1.0/betaGammaSq);
657 } 673 }
658 674
659 if( fImPartDielectricConst[i] == 0.0 || bet 675 if( fImPartDielectricConst[i] == 0.0 || betaGammaSq < 0.01 )
660 { 676 {
661 argument = 0.0; 677 argument = 0.0;
662 } 678 }
663 else 679 else
664 { 680 {
665 x3 = -fRePartDielectricConst[i] + 1.0/bet 681 x3 = -fRePartDielectricConst[i] + 1.0/betaGammaSq;
666 x5 = -1.0 - fRePartDielectricConst[i] + 682 x5 = -1.0 - fRePartDielectricConst[i] +
667 be2*((1.0 +fRePartDielectricConst[i] 683 be2*((1.0 +fRePartDielectricConst[i])*(1.0 + fRePartDielectricConst[i]) +
668 fImPartDielectricConst[i]*fImPartDie 684 fImPartDielectricConst[i]*fImPartDielectricConst[i]);
669 if( x3 == 0.0 ) argument = 0.5*pi; 685 if( x3 == 0.0 ) argument = 0.5*pi;
670 else argument = std::atan2(fIm << 686 else argument = atan2(fImPartDielectricConst[i],x3);
671 argument *= x5 ; 687 argument *= x5 ;
672 } 688 }
673 dNdxC = ( logarithm*fImPartDielectricConst[ 689 dNdxC = ( logarithm*fImPartDielectricConst[i] + argument )/hbarc;
674 690
675 if(dNdxC < 1.0e-8) dNdxC = 1.0e-8; 691 if(dNdxC < 1.0e-8) dNdxC = 1.0e-8;
676 692
677 dNdxC *= fine_structure_const/be2/pi; 693 dNdxC *= fine_structure_const/be2/pi;
678 694
679 dNdxC *= (1 - std::exp(-be4/betaBohr4)); << 695 dNdxC *= (1-exp(-be4/betaBohr4));
680 696
>> 697 // if(fDensity >= 0.1)
>> 698 // {
681 modul2 = (1.0 + fRePartDielectricConst[i])* 699 modul2 = (1.0 + fRePartDielectricConst[i])*(1.0 + fRePartDielectricConst[i]) +
682 fImPartDielectricConst[i]* 700 fImPartDielectricConst[i]*fImPartDielectricConst[i];
683 if(modul2 > 0.) 701 if(modul2 > 0.)
684 { 702 {
685 dNdxC /= modul2; 703 dNdxC /= modul2;
686 } 704 }
687 return dNdxC; 705 return dNdxC;
688 706
689 } // end of PAIdNdxCerenkov 707 } // end of PAIdNdxCerenkov
690 708
691 ////////////////////////////////////////////// 709 //////////////////////////////////////////////////////////////////////////
692 // 710 //
693 // Calculation od dN/dx of collisions with cre 711 // Calculation od dN/dx of collisions with creation of longitudinal EM
694 // excitations (plasmons, delta-electrons) 712 // excitations (plasmons, delta-electrons)
695 713
696 G4double G4PAIySection::PAIdNdxPlasmon( G4int << 714 G4double G4PAIySection::PAIdNdxPlasmon( G4int i ,
>> 715 G4double betaGammaSq )
697 { 716 {
698 G4double cof, resonance, modul2, dNdxP; 717 G4double cof, resonance, modul2, dNdxP;
699 G4double be2, be4; 718 G4double be2, be4;
700 719
701 cof = 1; 720 cof = 1;
702 721
703 be2 = betaGammaSq/(1 + betaGammaSq); 722 be2 = betaGammaSq/(1 + betaGammaSq);
704 be4 = be2*be2; 723 be4 = be2*be2;
705 724
706 resonance = std::log(2*electron_mass_c2*be2 << 725 resonance = log(2*electron_mass_c2*be2/fSplineEnergy[i]);
707 resonance *= fImPartDielectricConst[i]/hbar 726 resonance *= fImPartDielectricConst[i]/hbarc;
708 727
709 dNdxP = ( resonance + cof*fIntegralTerm[i]/ 728 dNdxP = ( resonance + cof*fIntegralTerm[i]/fSplineEnergy[i]/fSplineEnergy[i] );
710 729
711 dNdxP = std::max(dNdxP, 1.0e-8); 730 dNdxP = std::max(dNdxP, 1.0e-8);
712 731
713 dNdxP *= fine_structure_const/be2/pi; 732 dNdxP *= fine_structure_const/be2/pi;
714 dNdxP *= (1 - std::exp(-be4/betaBohr4)); << 733 dNdxP *= (1-exp(-be4/betaBohr4));
715 734
>> 735 // if( fDensity >= 0.1 )
>> 736 // {
716 modul2 = (1 + fRePartDielectricConst[i])*(1 737 modul2 = (1 + fRePartDielectricConst[i])*(1 + fRePartDielectricConst[i]) +
717 fImPartDielectricConst[i]*fImPartDielectr 738 fImPartDielectricConst[i]*fImPartDielectricConst[i];
718 if(modul2 > 0.) 739 if(modul2 > 0.)
719 { 740 {
720 dNdxP /= modul2; 741 dNdxP /= modul2;
721 } 742 }
722 return dNdxP; 743 return dNdxP;
723 744
724 } // end of PAIdNdxPlasmon 745 } // end of PAIdNdxPlasmon
725 746
726 ////////////////////////////////////////////// 747 ////////////////////////////////////////////////////////////////////////
727 // 748 //
728 // Calculation of the PAI integral cross-secti 749 // Calculation of the PAI integral cross-section
729 // fIntegralPAIySection[1] = specific primary 750 // fIntegralPAIySection[1] = specific primary ionisation, 1/cm
730 // and fIntegralPAIySection[0] = mean energy l 751 // and fIntegralPAIySection[0] = mean energy loss per cm in keV/cm
731 752
732 void G4PAIySection::IntegralPAIySection() 753 void G4PAIySection::IntegralPAIySection()
733 { 754 {
734 fIntegralPAIySection[fSplineNumber] = 0; 755 fIntegralPAIySection[fSplineNumber] = 0;
735 fIntegralPAIdEdx[fSplineNumber] = 0; 756 fIntegralPAIdEdx[fSplineNumber] = 0;
736 fIntegralPAIySection[0] = 0; 757 fIntegralPAIySection[0] = 0;
737 G4int k = fIntervalNumber -1; 758 G4int k = fIntervalNumber -1;
738 759
739 for(G4int i = fSplineNumber-1; i >= 1; i--) 760 for(G4int i = fSplineNumber-1; i >= 1; i--)
740 { 761 {
741 if(fSplineEnergy[i] >= fEnergyInterval[k]) 762 if(fSplineEnergy[i] >= fEnergyInterval[k])
742 { 763 {
743 fIntegralPAIySection[i] = fIntegralPAIyS 764 fIntegralPAIySection[i] = fIntegralPAIySection[i+1] + SumOverInterval(i);
744 fIntegralPAIdEdx[i] = fIntegralPAIdEdx[i 765 fIntegralPAIdEdx[i] = fIntegralPAIdEdx[i+1] + SumOverIntervaldEdx(i);
745 } 766 }
746 else 767 else
747 { 768 {
748 fIntegralPAIySection[i] = fIntegralPAIyS 769 fIntegralPAIySection[i] = fIntegralPAIySection[i+1] +
749 SumOverBord 770 SumOverBorder(i+1,fEnergyInterval[k]);
750 fIntegralPAIdEdx[i] = fIntegralPAIdEdx[i 771 fIntegralPAIdEdx[i] = fIntegralPAIdEdx[i+1] +
751 SumOverBord 772 SumOverBorderdEdx(i+1,fEnergyInterval[k]);
752 k--; 773 k--;
753 } 774 }
754 } 775 }
755 } // end of IntegralPAIySection 776 } // end of IntegralPAIySection
756 777
757 ////////////////////////////////////////////// 778 ////////////////////////////////////////////////////////////////////////
758 // 779 //
759 // Calculation of the PAI Cerenkov integral cr 780 // Calculation of the PAI Cerenkov integral cross-section
760 // fIntegralCrenkov[1] = specific Crenkov ioni 781 // fIntegralCrenkov[1] = specific Crenkov ionisation, 1/cm
761 // and fIntegralCerenkov[0] = mean Cerenkov lo 782 // and fIntegralCerenkov[0] = mean Cerenkov loss per cm in keV/cm
762 783
763 void G4PAIySection::IntegralCerenkov() 784 void G4PAIySection::IntegralCerenkov()
764 { 785 {
765 G4int i, k; 786 G4int i, k;
766 fIntegralCerenkov[fSplineNumber] = 0; 787 fIntegralCerenkov[fSplineNumber] = 0;
767 fIntegralCerenkov[0] = 0; 788 fIntegralCerenkov[0] = 0;
768 k = fIntervalNumber -1; 789 k = fIntervalNumber -1;
769 790
770 for( i = fSplineNumber-1; i >= 1; i-- ) 791 for( i = fSplineNumber-1; i >= 1; i-- )
771 { 792 {
772 if(fSplineEnergy[i] >= fEnergyInterval[k 793 if(fSplineEnergy[i] >= fEnergyInterval[k])
773 { 794 {
774 fIntegralCerenkov[i] = fIntegralCerenk 795 fIntegralCerenkov[i] = fIntegralCerenkov[i+1] + SumOverInterCerenkov(i);
775 // G4cout<<"int: i = "<<i<<"; sumC = " 796 // G4cout<<"int: i = "<<i<<"; sumC = "<<fIntegralCerenkov[i]<<G4endl;
776 } 797 }
777 else 798 else
778 { 799 {
779 fIntegralCerenkov[i] = fIntegralCerenk 800 fIntegralCerenkov[i] = fIntegralCerenkov[i+1] +
780 SumOverBord 801 SumOverBordCerenkov(i+1,fEnergyInterval[k]);
781 k--; 802 k--;
782 // G4cout<<"bord: i = "<<i<<"; sumC = 803 // G4cout<<"bord: i = "<<i<<"; sumC = "<<fIntegralCerenkov[i]<<G4endl;
783 } 804 }
784 } 805 }
785 806
786 } // end of IntegralCerenkov 807 } // end of IntegralCerenkov
787 808
788 ////////////////////////////////////////////// 809 ////////////////////////////////////////////////////////////////////////
789 // 810 //
790 // Calculation of the PAI Plasmon integral cro 811 // Calculation of the PAI Plasmon integral cross-section
791 // fIntegralPlasmon[1] = splasmon primary ioni 812 // fIntegralPlasmon[1] = splasmon primary ionisation, 1/cm
792 // and fIntegralPlasmon[0] = mean plasmon loss 813 // and fIntegralPlasmon[0] = mean plasmon loss per cm in keV/cm
793 814
794 void G4PAIySection::IntegralPlasmon() 815 void G4PAIySection::IntegralPlasmon()
795 { 816 {
796 fIntegralPlasmon[fSplineNumber] = 0; 817 fIntegralPlasmon[fSplineNumber] = 0;
797 fIntegralPlasmon[0] = 0; 818 fIntegralPlasmon[0] = 0;
798 G4int k = fIntervalNumber -1; 819 G4int k = fIntervalNumber -1;
799 for(G4int i=fSplineNumber-1;i>=1;i--) 820 for(G4int i=fSplineNumber-1;i>=1;i--)
800 { 821 {
801 if(fSplineEnergy[i] >= fEnergyInterval[k 822 if(fSplineEnergy[i] >= fEnergyInterval[k])
802 { 823 {
803 fIntegralPlasmon[i] = fIntegralPlasmon 824 fIntegralPlasmon[i] = fIntegralPlasmon[i+1] + SumOverInterPlasmon(i);
804 } 825 }
805 else 826 else
806 { 827 {
807 fIntegralPlasmon[i] = fIntegralPlasmon 828 fIntegralPlasmon[i] = fIntegralPlasmon[i+1] +
808 SumOverBord 829 SumOverBordPlasmon(i+1,fEnergyInterval[k]);
809 k--; 830 k--;
810 } 831 }
811 } 832 }
>> 833
812 } // end of IntegralPlasmon 834 } // end of IntegralPlasmon
813 835
814 ////////////////////////////////////////////// 836 //////////////////////////////////////////////////////////////////////
815 // 837 //
816 // Calculation the PAI integral cross-section 838 // Calculation the PAI integral cross-section inside
817 // of interval of continuous values of photo-i 839 // of interval of continuous values of photo-ionisation
818 // cross-section. Parameter 'i' is the number 840 // cross-section. Parameter 'i' is the number of interval.
819 841
820 G4double G4PAIySection::SumOverInterval( G4int 842 G4double G4PAIySection::SumOverInterval( G4int i )
821 { 843 {
822 G4double x0,x1,y0,yy1,a,b,c,result; 844 G4double x0,x1,y0,yy1,a,b,c,result;
823 845
824 x0 = fSplineEnergy[i]; 846 x0 = fSplineEnergy[i];
825 x1 = fSplineEnergy[i+1]; 847 x1 = fSplineEnergy[i+1];
826 848
827 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) 849 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) return 0.;
828 850
829 y0 = fDifPAIySection[i]; 851 y0 = fDifPAIySection[i];
830 yy1 = fDifPAIySection[i+1]; 852 yy1 = fDifPAIySection[i+1];
831 //G4cout << "## x0= " << x0 << " x1= " << x 853 //G4cout << "## x0= " << x0 << " x1= " << x1 << G4endl;
832 c = x1/x0; 854 c = x1/x0;
833 //G4cout << "c= " << c << " y0= " << y0 << 855 //G4cout << "c= " << c << " y0= " << y0 << " yy1= " << yy1 << G4endl;
834 a = log10(yy1/y0)/log10(c); 856 a = log10(yy1/y0)/log10(c);
835 //G4cout << "a= " << a << G4endl; 857 //G4cout << "a= " << a << G4endl;
836 << 858 // b = log10(y0) - a*log10(x0);
837 b = 0.0; << 859 b = y0/pow(x0,a);
838 if(a < 20.) b = y0/pow(x0,a); <<
839 <<
840 a += 1; 860 a += 1;
841 if(a == 0) 861 if(a == 0)
842 { 862 {
843 result = b*log(x1/x0); 863 result = b*log(x1/x0);
844 } 864 }
845 else 865 else
846 { 866 {
847 result = y0*(x1*pow(c,a-1) - x0)/a; 867 result = y0*(x1*pow(c,a-1) - x0)/a;
848 } 868 }
849 a++; 869 a++;
850 if(a == 0) 870 if(a == 0)
851 { 871 {
852 fIntegralPAIySection[0] += b*log(x1/x0); 872 fIntegralPAIySection[0] += b*log(x1/x0);
853 } 873 }
854 else 874 else
855 { 875 {
856 fIntegralPAIySection[0] += y0*(x1*x1*pow 876 fIntegralPAIySection[0] += y0*(x1*x1*pow(c,a-2) - x0*x0)/a;
857 } 877 }
858 return result; 878 return result;
859 879
860 } // end of SumOverInterval 880 } // end of SumOverInterval
861 881
862 ///////////////////////////////// 882 /////////////////////////////////
863 883
864 G4double G4PAIySection::SumOverIntervaldEdx( G 884 G4double G4PAIySection::SumOverIntervaldEdx( G4int i )
865 { 885 {
866 G4double x0,x1,y0,yy1,a,b,c,result; 886 G4double x0,x1,y0,yy1,a,b,c,result;
867 887
868 x0 = fSplineEnergy[i]; 888 x0 = fSplineEnergy[i];
869 x1 = fSplineEnergy[i+1]; 889 x1 = fSplineEnergy[i+1];
870 890
871 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) 891 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) return 0.;
872 892
873 y0 = fDifPAIySection[i]; 893 y0 = fDifPAIySection[i];
874 yy1 = fDifPAIySection[i+1]; 894 yy1 = fDifPAIySection[i+1];
875 c = x1/x0; 895 c = x1/x0;
876 a = log10(yy1/y0)/log10(c); 896 a = log10(yy1/y0)/log10(c);
877 << 897 // b = log10(y0) - a*log10(x0);
878 b = 0.0; << 898 b = y0/pow(x0,a);
879 if(a < 20.) b = y0/pow(x0,a); <<
880 <<
881 a += 2; 899 a += 2;
882 if(a == 0) 900 if(a == 0)
883 { 901 {
884 result = b*log(x1/x0); 902 result = b*log(x1/x0);
885 } 903 }
886 else 904 else
887 { 905 {
888 result = y0*(x1*x1*pow(c,a-2) - x0*x0)/a; 906 result = y0*(x1*x1*pow(c,a-2) - x0*x0)/a;
889 } 907 }
890 return result; 908 return result;
891 909
892 } // end of SumOverInterval 910 } // end of SumOverInterval
893 911
894 ////////////////////////////////////////////// 912 //////////////////////////////////////////////////////////////////////
895 // 913 //
896 // Calculation the PAI Cerenkov integral cross 914 // Calculation the PAI Cerenkov integral cross-section inside
897 // of interval of continuous values of photo-i 915 // of interval of continuous values of photo-ionisation Cerenkov
898 // cross-section. Parameter 'i' is the number 916 // cross-section. Parameter 'i' is the number of interval.
899 917
900 G4double G4PAIySection::SumOverInterCerenkov( 918 G4double G4PAIySection::SumOverInterCerenkov( G4int i )
901 { 919 {
902 G4double x0,x1,y0,yy1,a,c,result; 920 G4double x0,x1,y0,yy1,a,c,result;
903 921
904 x0 = fSplineEnergy[i]; 922 x0 = fSplineEnergy[i];
905 x1 = fSplineEnergy[i+1]; 923 x1 = fSplineEnergy[i+1];
906 924
907 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) 925 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) return 0.;
908 926
909 y0 = fdNdxCerenkov[i]; 927 y0 = fdNdxCerenkov[i];
910 yy1 = fdNdxCerenkov[i+1]; 928 yy1 = fdNdxCerenkov[i+1];
911 // G4cout<<"SumC, i = "<<i<<"; x0 ="<<x0<<" 929 // G4cout<<"SumC, i = "<<i<<"; x0 ="<<x0<<"; x1 = "<<x1
912 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4en 930 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4endl;
913 931
914 c = x1/x0; 932 c = x1/x0;
915 a = log10(yy1/y0)/log10(c); 933 a = log10(yy1/y0)/log10(c);
916 G4double b = 0.0; 934 G4double b = 0.0;
917 if(a < 20.) b = y0/pow(x0,a); 935 if(a < 20.) b = y0/pow(x0,a);
918 936
919 a += 1.0; 937 a += 1.0;
920 if(a == 0) result = b*log(c); 938 if(a == 0) result = b*log(c);
921 else result = y0*(x1*pow(c,a-1) - x0) 939 else result = y0*(x1*pow(c,a-1) - x0)/a;
922 a += 1.0; 940 a += 1.0;
923 941
924 if( a == 0 ) fIntegralCerenkov[0] += b*log( 942 if( a == 0 ) fIntegralCerenkov[0] += b*log(x1/x0);
925 else fIntegralCerenkov[0] += y0*(x1 943 else fIntegralCerenkov[0] += y0*(x1*x1*pow(c,a-2) - x0*x0)/a;
926 // G4cout<<"a = "<<a<<"; b = "<<b<<"; resu 944 // G4cout<<"a = "<<a<<"; b = "<<b<<"; result = "<<result<<G4endl;
927 return result; 945 return result;
928 946
929 } // end of SumOverInterCerenkov 947 } // end of SumOverInterCerenkov
930 948
931 ////////////////////////////////////////////// 949 //////////////////////////////////////////////////////////////////////
932 // 950 //
933 // Calculation the PAI Plasmon integral cross- 951 // Calculation the PAI Plasmon integral cross-section inside
934 // of interval of continuous values of photo-i 952 // of interval of continuous values of photo-ionisation Plasmon
935 // cross-section. Parameter 'i' is the number 953 // cross-section. Parameter 'i' is the number of interval.
936 954
937 G4double G4PAIySection::SumOverInterPlasmon( G 955 G4double G4PAIySection::SumOverInterPlasmon( G4int i )
938 { 956 {
939 G4double x0,x1,y0,yy1,a,c,result; 957 G4double x0,x1,y0,yy1,a,c,result;
940 958
941 x0 = fSplineEnergy[i]; 959 x0 = fSplineEnergy[i];
942 x1 = fSplineEnergy[i+1]; 960 x1 = fSplineEnergy[i+1];
943 961
944 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) 962 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) return 0.;
945 963
946 y0 = fdNdxPlasmon[i]; 964 y0 = fdNdxPlasmon[i];
947 yy1 = fdNdxPlasmon[i+1]; 965 yy1 = fdNdxPlasmon[i+1];
948 c = x1/x0; 966 c = x1/x0;
949 a = log10(yy1/y0)/log10(c); 967 a = log10(yy1/y0)/log10(c);
950 968
951 G4double b = 0.0; 969 G4double b = 0.0;
952 if(a < 20.) b = y0/pow(x0,a); 970 if(a < 20.) b = y0/pow(x0,a);
953 971
954 a += 1.0; 972 a += 1.0;
955 if(a == 0) result = b*log(x1/x0); 973 if(a == 0) result = b*log(x1/x0);
956 else result = y0*(x1*pow(c,a-1) - x0) 974 else result = y0*(x1*pow(c,a-1) - x0)/a;
957 a += 1.0; 975 a += 1.0;
958 976
959 if( a == 0 ) fIntegralPlasmon[0] += b*log(x 977 if( a == 0 ) fIntegralPlasmon[0] += b*log(x1/x0);
960 else fIntegralPlasmon[0] += y0*(x1* 978 else fIntegralPlasmon[0] += y0*(x1*x1*pow(c,a-2) - x0*x0)/a;
961 979
962 return result; 980 return result;
963 981
964 } // end of SumOverInterPlasmon 982 } // end of SumOverInterPlasmon
965 983
966 ////////////////////////////////////////////// 984 ///////////////////////////////////////////////////////////////////////////////
967 // 985 //
968 // Integration of PAI cross-section for the ca 986 // Integration of PAI cross-section for the case of
969 // passing across border between intervals 987 // passing across border between intervals
970 988
971 G4double G4PAIySection::SumOverBorder( G4int 989 G4double G4PAIySection::SumOverBorder( G4int i ,
972 G4doubl 990 G4double en0 )
973 { 991 {
974 G4double x0,x1,y0,yy1,a,d,e0,result; << 992 G4double x0,x1,y0,yy1,a,/*c,*/d,e0,result;
975 993
976 e0 = en0; 994 e0 = en0;
977 x0 = fSplineEnergy[i]; 995 x0 = fSplineEnergy[i];
978 x1 = fSplineEnergy[i+1]; 996 x1 = fSplineEnergy[i+1];
979 y0 = fDifPAIySection[i]; 997 y0 = fDifPAIySection[i];
980 yy1 = fDifPAIySection[i+1]; 998 yy1 = fDifPAIySection[i+1];
981 999
>> 1000 //c = x1/x0;
982 d = e0/x0; 1001 d = e0/x0;
983 a = log10(yy1/y0)/log10(x1/x0); 1002 a = log10(yy1/y0)/log10(x1/x0);
984 1003
985 G4double b = 0.0; 1004 G4double b = 0.0;
986 if(a < 20.) b = y0/pow(x0,a); 1005 if(a < 20.) b = y0/pow(x0,a);
987 1006
988 a += 1; 1007 a += 1;
989 if(a == 0) 1008 if(a == 0)
990 { 1009 {
991 result = b*log(x0/e0); 1010 result = b*log(x0/e0);
992 } 1011 }
993 else 1012 else
994 { 1013 {
995 result = y0*(x0 - e0*pow(d,a-1))/a; 1014 result = y0*(x0 - e0*pow(d,a-1))/a;
996 } 1015 }
997 a++; 1016 a++;
998 if(a == 0) 1017 if(a == 0)
999 { 1018 {
1000 fIntegralPAIySection[0] += b*log(x0/e0) 1019 fIntegralPAIySection[0] += b*log(x0/e0);
1001 } 1020 }
1002 else 1021 else
1003 { 1022 {
1004 fIntegralPAIySection[0] += y0*(x0*x0 - 1023 fIntegralPAIySection[0] += y0*(x0*x0 - e0*e0*pow(d,a-2))/a;
1005 } 1024 }
1006 x0 = fSplineEnergy[i - 1]; 1025 x0 = fSplineEnergy[i - 1];
1007 x1 = fSplineEnergy[i - 2]; 1026 x1 = fSplineEnergy[i - 2];
1008 y0 = fDifPAIySection[i - 1]; 1027 y0 = fDifPAIySection[i - 1];
1009 yy1 = fDifPAIySection[i - 2]; 1028 yy1 = fDifPAIySection[i - 2];
1010 1029
1011 //c = x1/x0; 1030 //c = x1/x0;
1012 d = e0/x0; 1031 d = e0/x0;
1013 a = log10(yy1/y0)/log10(x1/x0); 1032 a = log10(yy1/y0)/log10(x1/x0);
1014 << 1033 // b0 = log10(y0) - a*log10(x0);
1015 b = 0.0; << 1034 b = y0/pow(x0,a);
1016 if(a < 20.) b = y0/pow(x0,a); <<
1017 <<
1018 a += 1; 1035 a += 1;
1019 if(a == 0) 1036 if(a == 0)
1020 { 1037 {
1021 result += b*log(e0/x0); 1038 result += b*log(e0/x0);
1022 } 1039 }
1023 else 1040 else
1024 { 1041 {
1025 result += y0*(e0*pow(d,a-1) - x0)/a; 1042 result += y0*(e0*pow(d,a-1) - x0)/a;
1026 } 1043 }
1027 a++; 1044 a++;
1028 if(a == 0) 1045 if(a == 0)
1029 { 1046 {
1030 fIntegralPAIySection[0] += b*log(e0/x0) 1047 fIntegralPAIySection[0] += b*log(e0/x0);
1031 } 1048 }
1032 else 1049 else
1033 { 1050 {
1034 fIntegralPAIySection[0] += y0*(e0*e0*po 1051 fIntegralPAIySection[0] += y0*(e0*e0*pow(d,a-2) - x0*x0)/a;
1035 } 1052 }
1036 return result; 1053 return result;
1037 1054
1038 } 1055 }
1039 1056
1040 ///////////////////////////////////////////// 1057 ///////////////////////////////////////////////////////////////////////
1041 1058
1042 G4double G4PAIySection::SumOverBorderdEdx( G4 1059 G4double G4PAIySection::SumOverBorderdEdx( G4int i ,
1043 G4doub 1060 G4double en0 )
1044 { 1061 {
1045 G4double x0,x1,y0,yy1,a,/*c,*/d,e0,result; 1062 G4double x0,x1,y0,yy1,a,/*c,*/d,e0,result;
1046 1063
1047 e0 = en0; 1064 e0 = en0;
1048 x0 = fSplineEnergy[i]; 1065 x0 = fSplineEnergy[i];
1049 x1 = fSplineEnergy[i+1]; 1066 x1 = fSplineEnergy[i+1];
1050 y0 = fDifPAIySection[i]; 1067 y0 = fDifPAIySection[i];
1051 yy1 = fDifPAIySection[i+1]; 1068 yy1 = fDifPAIySection[i+1];
1052 1069
>> 1070 //c = x1/x0;
1053 d = e0/x0; 1071 d = e0/x0;
1054 a = log10(yy1/y0)/log10(x1/x0); 1072 a = log10(yy1/y0)/log10(x1/x0);
1055 1073
1056 G4double b = 0.0; 1074 G4double b = 0.0;
1057 if(a < 20.) b = y0/pow(x0,a); 1075 if(a < 20.) b = y0/pow(x0,a);
1058 1076
1059 a += 2; 1077 a += 2;
1060 if(a == 0) 1078 if(a == 0)
1061 { 1079 {
1062 result = b*log(x0/e0); 1080 result = b*log(x0/e0);
1063 } 1081 }
1064 else 1082 else
1065 { 1083 {
1066 result = y0*(x0*x0 - e0*e0*pow(d,a-2))/ 1084 result = y0*(x0*x0 - e0*e0*pow(d,a-2))/a;
1067 } 1085 }
1068 x0 = fSplineEnergy[i - 1]; 1086 x0 = fSplineEnergy[i - 1];
1069 x1 = fSplineEnergy[i - 2]; 1087 x1 = fSplineEnergy[i - 2];
1070 y0 = fDifPAIySection[i - 1]; 1088 y0 = fDifPAIySection[i - 1];
1071 yy1 = fDifPAIySection[i - 2]; 1089 yy1 = fDifPAIySection[i - 2];
1072 1090
>> 1091 //c = x1/x0;
1073 d = e0/x0; 1092 d = e0/x0;
1074 a = log10(yy1/y0)/log10(x1/x0); 1093 a = log10(yy1/y0)/log10(x1/x0);
1075 1094
1076 b = 0.0; <<
1077 if(a < 20.) b = y0/pow(x0,a); 1095 if(a < 20.) b = y0/pow(x0,a);
1078 1096
1079 a += 2; 1097 a += 2;
1080 if(a == 0) 1098 if(a == 0)
1081 { 1099 {
1082 result += b*log(e0/x0); 1100 result += b*log(e0/x0);
1083 } 1101 }
1084 else 1102 else
1085 { 1103 {
1086 result += y0*(e0*e0*pow(d,a-2) - x0*x0) 1104 result += y0*(e0*e0*pow(d,a-2) - x0*x0)/a;
1087 } 1105 }
1088 return result; 1106 return result;
>> 1107
1089 } 1108 }
1090 1109
1091 ///////////////////////////////////////////// 1110 ///////////////////////////////////////////////////////////////////////////////
1092 // 1111 //
1093 // Integration of Cerenkov cross-section for 1112 // Integration of Cerenkov cross-section for the case of
1094 // passing across border between intervals 1113 // passing across border between intervals
1095 1114
1096 G4double G4PAIySection::SumOverBordCerenkov( 1115 G4double G4PAIySection::SumOverBordCerenkov( G4int i ,
1097 1116 G4double en0 )
1098 { 1117 {
1099 G4double x0,x1,y0,yy1,a,e0,c,d,result; 1118 G4double x0,x1,y0,yy1,a,e0,c,d,result;
1100 1119
1101 e0 = en0; 1120 e0 = en0;
1102 x0 = fSplineEnergy[i]; 1121 x0 = fSplineEnergy[i];
1103 x1 = fSplineEnergy[i+1]; 1122 x1 = fSplineEnergy[i+1];
1104 y0 = fdNdxCerenkov[i]; 1123 y0 = fdNdxCerenkov[i];
1105 yy1 = fdNdxCerenkov[i+1]; 1124 yy1 = fdNdxCerenkov[i+1];
1106 1125
1107 // G4cout<<G4endl; 1126 // G4cout<<G4endl;
1108 //G4cout<<"SumBordC, i = "<<i<<"; en0 = "< 1127 //G4cout<<"SumBordC, i = "<<i<<"; en0 = "<<en0<<"; x0 ="<<x0<<"; x1 = "<<x1
1109 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G 1128 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4endl;
1110 c = x1/x0; 1129 c = x1/x0;
1111 d = e0/x0; 1130 d = e0/x0;
1112 a = log10(yy1/y0)/log10(c); 1131 a = log10(yy1/y0)/log10(c);
1113 1132
1114 G4double b = 0.0; 1133 G4double b = 0.0;
1115 if(a < 20.) b = y0/pow(x0,a); 1134 if(a < 20.) b = y0/pow(x0,a);
1116 1135
1117 a += 1.0; 1136 a += 1.0;
1118 if( a == 0 ) result = b*log(x0/e0); 1137 if( a == 0 ) result = b*log(x0/e0);
1119 else result = y0*(x0 - e0*pow(d,a- 1138 else result = y0*(x0 - e0*pow(d,a-1))/a;
1120 a += 1.0; 1139 a += 1.0;
1121 1140
1122 if( a == 0 ) fIntegralCerenkov[0] += b*log 1141 if( a == 0 ) fIntegralCerenkov[0] += b*log(x0/e0);
1123 else fIntegralCerenkov[0] += y0*(x 1142 else fIntegralCerenkov[0] += y0*(x0*x0 - e0*e0*pow(d,a-2))/a;
1124 1143
1125 //G4cout<<"a = "<<a<<"; b = "<<b<<"; resul 1144 //G4cout<<"a = "<<a<<"; b = "<<b<<"; result = "<<result<<G4endl;
1126 1145
1127 x0 = fSplineEnergy[i - 1]; 1146 x0 = fSplineEnergy[i - 1];
1128 x1 = fSplineEnergy[i - 2]; 1147 x1 = fSplineEnergy[i - 2];
1129 y0 = fdNdxCerenkov[i - 1]; 1148 y0 = fdNdxCerenkov[i - 1];
1130 yy1 = fdNdxCerenkov[i - 2]; 1149 yy1 = fdNdxCerenkov[i - 2];
1131 1150
1132 //G4cout<<"x0 ="<<x0<<"; x1 = "<<x1 1151 //G4cout<<"x0 ="<<x0<<"; x1 = "<<x1
1133 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4 1152 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4endl;
1134 1153
1135 c = x1/x0; 1154 c = x1/x0;
1136 d = e0/x0; 1155 d = e0/x0;
1137 a = log10(yy1/y0)/log10(x1/x0); 1156 a = log10(yy1/y0)/log10(x1/x0);
1138 1157
1139 // G4cout << "a= " << a << G4endl; 1158 // G4cout << "a= " << a << G4endl;
1140 if(a > 20.0) b = 0.0; 1159 if(a > 20.0) b = 0.0;
1141 else b = y0/pow(x0,a); 1160 else b = y0/pow(x0,a);
1142 1161
1143 //G4cout << "b= " << b << G4endl; 1162 //G4cout << "b= " << b << G4endl;
1144 1163
1145 a += 1.0; 1164 a += 1.0;
1146 if( a == 0 ) result += b*log(e0/x0); 1165 if( a == 0 ) result += b*log(e0/x0);
1147 else result += y0*(e0*pow(d,a-1) - 1166 else result += y0*(e0*pow(d,a-1) - x0 )/a;
1148 a += 1.0; 1167 a += 1.0;
1149 //G4cout << "result= " << result << G4endl 1168 //G4cout << "result= " << result << G4endl;
1150 1169
1151 if( a == 0 ) fIntegralCerenkov[0] += b*l 1170 if( a == 0 ) fIntegralCerenkov[0] += b*log(e0/x0);
1152 else fIntegralCerenkov[0] += y0* 1171 else fIntegralCerenkov[0] += y0*(e0*e0*pow(d,a-2) - x0*x0)/a;
1153 1172
1154 //G4cout<<"a = "<<a<<"; b = "<<b<<"; resul 1173 //G4cout<<"a = "<<a<<"; b = "<<b<<"; result = "<<result<<G4endl;
1155 1174
1156 return result; 1175 return result;
>> 1176
1157 } 1177 }
1158 1178
1159 ///////////////////////////////////////////// 1179 ///////////////////////////////////////////////////////////////////////////////
1160 // 1180 //
1161 // Integration of Plasmon cross-section for t 1181 // Integration of Plasmon cross-section for the case of
1162 // passing across border between intervals 1182 // passing across border between intervals
1163 1183
1164 G4double G4PAIySection::SumOverBordPlasmon( G 1184 G4double G4PAIySection::SumOverBordPlasmon( G4int i ,
1165 1185 G4double en0 )
1166 { 1186 {
1167 G4double x0,x1,y0,yy1,a,c,d,e0,result; 1187 G4double x0,x1,y0,yy1,a,c,d,e0,result;
1168 1188
1169 e0 = en0; 1189 e0 = en0;
1170 x0 = fSplineEnergy[i]; 1190 x0 = fSplineEnergy[i];
1171 x1 = fSplineEnergy[i+1]; 1191 x1 = fSplineEnergy[i+1];
1172 y0 = fdNdxPlasmon[i]; 1192 y0 = fdNdxPlasmon[i];
1173 yy1 = fdNdxPlasmon[i+1]; 1193 yy1 = fdNdxPlasmon[i+1];
1174 1194
1175 c = x1/x0; 1195 c = x1/x0;
1176 d = e0/x0; 1196 d = e0/x0;
1177 a = log10(yy1/y0)/log10(c); 1197 a = log10(yy1/y0)/log10(c);
1178 1198
1179 G4double b = 0.0; 1199 G4double b = 0.0;
1180 if(a < 20.) b = y0/pow(x0,a); 1200 if(a < 20.) b = y0/pow(x0,a);
1181 1201
1182 a += 1.0; 1202 a += 1.0;
1183 if( a == 0 ) result = b*log(x0/e0); 1203 if( a == 0 ) result = b*log(x0/e0);
1184 else result = y0*(x0 - e0*pow(d,a- 1204 else result = y0*(x0 - e0*pow(d,a-1))/a;
1185 a += 1.0; 1205 a += 1.0;
1186 1206
1187 if( a == 0 ) fIntegralPlasmon[0] += b*log( 1207 if( a == 0 ) fIntegralPlasmon[0] += b*log(x0/e0);
1188 else fIntegralPlasmon[0] += y0*(x0 1208 else fIntegralPlasmon[0] += y0*(x0*x0 - e0*e0*pow(d,a-2))/a;
1189 1209
1190 x0 = fSplineEnergy[i - 1]; 1210 x0 = fSplineEnergy[i - 1];
1191 x1 = fSplineEnergy[i - 2]; 1211 x1 = fSplineEnergy[i - 2];
1192 y0 = fdNdxPlasmon[i - 1]; 1212 y0 = fdNdxPlasmon[i - 1];
1193 yy1 = fdNdxPlasmon[i - 2]; 1213 yy1 = fdNdxPlasmon[i - 2];
1194 1214
1195 c = x1/x0; 1215 c = x1/x0;
1196 d = e0/x0; 1216 d = e0/x0;
1197 a = log10(yy1/y0)/log10(c); 1217 a = log10(yy1/y0)/log10(c);
1198 1218
1199 if(a < 20.) b = y0/pow(x0,a); 1219 if(a < 20.) b = y0/pow(x0,a);
1200 1220
1201 a += 1.0; 1221 a += 1.0;
1202 if( a == 0 ) result += b*log(e0/x0); 1222 if( a == 0 ) result += b*log(e0/x0);
1203 else result += y0*(e0*pow(d,a-1) - 1223 else result += y0*(e0*pow(d,a-1) - x0)/a;
1204 a += 1.0; 1224 a += 1.0;
1205 1225
1206 if( a == 0 ) fIntegralPlasmon[0] += b*lo 1226 if( a == 0 ) fIntegralPlasmon[0] += b*log(e0/x0);
1207 else fIntegralPlasmon[0] += y0*( 1227 else fIntegralPlasmon[0] += y0*(e0*e0*pow(d,a-2) - x0*x0)/a;
1208 1228
1209 return result; 1229 return result;
1210 1230
1211 } 1231 }
1212 1232
1213 ///////////////////////////////////////////// 1233 /////////////////////////////////////////////////////////////////////////
1214 // 1234 //
1215 // 1235 //
1216 1236
1217 G4double G4PAIySection::GetStepEnergyLoss( G4 1237 G4double G4PAIySection::GetStepEnergyLoss( G4double step )
1218 { 1238 {
1219 G4int iTransfer ; 1239 G4int iTransfer ;
1220 G4long numOfCollisions; 1240 G4long numOfCollisions;
1221 G4double loss = 0.0; 1241 G4double loss = 0.0;
1222 G4double meanNumber, position; 1242 G4double meanNumber, position;
1223 1243
1224 // G4cout<<" G4PAIySection::GetStepEnergyLo 1244 // G4cout<<" G4PAIySection::GetStepEnergyLoss "<<G4endl;
1225 1245
1226 1246
1227 1247
1228 meanNumber = fIntegralPAIySection[1]*step; 1248 meanNumber = fIntegralPAIySection[1]*step;
1229 numOfCollisions = G4Poisson(meanNumber); 1249 numOfCollisions = G4Poisson(meanNumber);
1230 1250
1231 // G4cout<<"numOfCollisions = "<<numOfCol 1251 // G4cout<<"numOfCollisions = "<<numOfCollisions<<G4endl;
1232 1252
1233 while(numOfCollisions) 1253 while(numOfCollisions)
1234 { 1254 {
1235 position = fIntegralPAIySection[1]*G4Unif 1255 position = fIntegralPAIySection[1]*G4UniformRand();
1236 1256
1237 for( iTransfer=1; iTransfer<=fSplineNumbe 1257 for( iTransfer=1; iTransfer<=fSplineNumber; iTransfer++ )
1238 { 1258 {
1239 if( position >= fIntegralPAIySection[ 1259 if( position >= fIntegralPAIySection[iTransfer] ) break;
1240 } 1260 }
1241 loss += fSplineEnergy[iTransfer] ; 1261 loss += fSplineEnergy[iTransfer] ;
1242 numOfCollisions--; 1262 numOfCollisions--;
1243 // Loop checking, 03-Aug-2015, Vladimir I 1263 // Loop checking, 03-Aug-2015, Vladimir Ivanchenko
1244 } 1264 }
1245 // G4cout<<"PAI energy loss = "<<loss/keV<< 1265 // G4cout<<"PAI energy loss = "<<loss/keV<<" keV"<<G4endl;
1246 1266
1247 return loss; 1267 return loss;
1248 } 1268 }
1249 1269
1250 ///////////////////////////////////////////// 1270 /////////////////////////////////////////////////////////////////////////
1251 // 1271 //
1252 // 1272 //
1253 1273
1254 G4double G4PAIySection::GetStepCerenkovLoss( 1274 G4double G4PAIySection::GetStepCerenkovLoss( G4double step )
1255 { 1275 {
1256 G4int iTransfer ; 1276 G4int iTransfer ;
1257 G4long numOfCollisions; 1277 G4long numOfCollisions;
1258 G4double loss = 0.0; 1278 G4double loss = 0.0;
1259 G4double meanNumber, position; 1279 G4double meanNumber, position;
1260 1280
1261 // G4cout<<" G4PAIySection::GetStepCreLosnk 1281 // G4cout<<" G4PAIySection::GetStepCreLosnkovs "<<G4endl;
1262 1282
1263 1283
1264 1284
1265 meanNumber = fIntegralCerenkov[1]*step; 1285 meanNumber = fIntegralCerenkov[1]*step;
1266 numOfCollisions = G4Poisson(meanNumber); 1286 numOfCollisions = G4Poisson(meanNumber);
1267 1287
1268 // G4cout<<"numOfCollisions = "<<numOfCol 1288 // G4cout<<"numOfCollisions = "<<numOfCollisions<<G4endl;
1269 1289
1270 while(numOfCollisions) 1290 while(numOfCollisions)
1271 { 1291 {
1272 position = fIntegralCerenkov[1]*G4Uniform 1292 position = fIntegralCerenkov[1]*G4UniformRand();
1273 1293
1274 for( iTransfer=1; iTransfer<=fSplineNumbe 1294 for( iTransfer=1; iTransfer<=fSplineNumber; iTransfer++ )
1275 { 1295 {
1276 if( position >= fIntegralCerenkov[iTr 1296 if( position >= fIntegralCerenkov[iTransfer] ) break;
1277 } 1297 }
1278 loss += fSplineEnergy[iTransfer] ; 1298 loss += fSplineEnergy[iTransfer] ;
1279 numOfCollisions--; 1299 numOfCollisions--;
1280 // Loop checking, 03-Aug-2015, Vladimir I 1300 // Loop checking, 03-Aug-2015, Vladimir Ivanchenko
1281 } 1301 }
1282 // G4cout<<"PAI Cerenkov loss = "<<loss/keV 1302 // G4cout<<"PAI Cerenkov loss = "<<loss/keV<<" keV"<<G4endl;
1283 1303
1284 return loss; 1304 return loss;
1285 } 1305 }
1286 1306
1287 ///////////////////////////////////////////// 1307 /////////////////////////////////////////////////////////////////////////
1288 // 1308 //
1289 // 1309 //
1290 1310
1291 G4double G4PAIySection::GetStepPlasmonLoss( G 1311 G4double G4PAIySection::GetStepPlasmonLoss( G4double step )
1292 { 1312 {
1293 G4int iTransfer ; 1313 G4int iTransfer ;
1294 G4long numOfCollisions; 1314 G4long numOfCollisions;
1295 G4double loss = 0.0; 1315 G4double loss = 0.0;
1296 G4double meanNumber, position; 1316 G4double meanNumber, position;
1297 1317
1298 // G4cout<<" G4PAIySection::GetStepCreLosnk 1318 // G4cout<<" G4PAIySection::GetStepCreLosnkovs "<<G4endl;
1299 1319
1300 1320
1301 1321
1302 meanNumber = fIntegralPlasmon[1]*step; 1322 meanNumber = fIntegralPlasmon[1]*step;
1303 numOfCollisions = G4Poisson(meanNumber); 1323 numOfCollisions = G4Poisson(meanNumber);
1304 1324
1305 // G4cout<<"numOfCollisions = "<<numOfCol 1325 // G4cout<<"numOfCollisions = "<<numOfCollisions<<G4endl;
1306 1326
1307 while(numOfCollisions) 1327 while(numOfCollisions)
1308 { 1328 {
1309 position = fIntegralPlasmon[1]*G4UniformR 1329 position = fIntegralPlasmon[1]*G4UniformRand();
1310 1330
1311 for( iTransfer=1; iTransfer<=fSplineNumbe 1331 for( iTransfer=1; iTransfer<=fSplineNumber; iTransfer++ )
1312 { 1332 {
1313 if( position >= fIntegralPlasmon[iTra 1333 if( position >= fIntegralPlasmon[iTransfer] ) break;
1314 } 1334 }
1315 loss += fSplineEnergy[iTransfer] ; 1335 loss += fSplineEnergy[iTransfer] ;
1316 numOfCollisions--; 1336 numOfCollisions--;
1317 // Loop checking, 03-Aug-2015, Vladimir I 1337 // Loop checking, 03-Aug-2015, Vladimir Ivanchenko
1318 } 1338 }
1319 // G4cout<<"PAI Plasmon loss = "<<loss/keV< 1339 // G4cout<<"PAI Plasmon loss = "<<loss/keV<<" keV"<<G4endl;
1320 1340
1321 return loss; 1341 return loss;
1322 } 1342 }
1323 1343
1324 ///////////////////////////////////////////// 1344 /////////////////////////////////////////////////////////////////////////////
1325 // 1345 //
1326 1346
1327 void G4PAIySection::CallError(G4int i, const 1347 void G4PAIySection::CallError(G4int i, const G4String& methodName) const
1328 { 1348 {
1329 G4String head = "G4PAIySection::" + methodN 1349 G4String head = "G4PAIySection::" + methodName + "()";
1330 G4ExceptionDescription ed; 1350 G4ExceptionDescription ed;
1331 ed << "Wrong index " << i << " fSplineNumbe 1351 ed << "Wrong index " << i << " fSplineNumber= " << fSplineNumber;
1332 G4Exception(head,"pai001",FatalException,ed 1352 G4Exception(head,"pai001",FatalException,ed);
1333 } 1353 }
1334 1354
1335 ///////////////////////////////////////////// 1355 /////////////////////////////////////////////////////////////////////////////
1336 // 1356 //
1337 // Init array of Lorentz factors 1357 // Init array of Lorentz factors
1338 // 1358 //
1339 1359
1340 G4int G4PAIySection::fNumberOfGammas = 111; 1360 G4int G4PAIySection::fNumberOfGammas = 111;
1341 1361
1342 const G4double G4PAIySection::fLorentzFactor[ 1362 const G4double G4PAIySection::fLorentzFactor[112] = // fNumberOfGammas+1
1343 { 1363 {
1344 0.0, 1364 0.0,
1345 1.094989e+00, 1.107813e+00, 1.122369e+00, 1.1 1365 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 1366 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 1367 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 1368 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 1369 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 1370 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 1371 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 1372 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 1373 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 1374 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 1375 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 1376 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 1377 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 1378 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 1379 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 1380 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 1381 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 1382 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 1383 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 1384 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 1385 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 1386 5.658206e+04, 6.422112e+04, 7.289153e+04, 8.273254e+04, 9.390219e+04, // 110
1367 1.065799e+05 1387 1.065799e+05
1368 }; 1388 };
1369 1389
1370 ///////////////////////////////////////////// 1390 ///////////////////////////////////////////////////////////////////////
1371 // 1391 //
1372 // The number of gamma for creation of splin 1392 // The number of gamma for creation of spline (near ion-min , G ~ 4 )
1373 // 1393 //
1374 1394
1375 const G4int G4PAIySection::fRefGammaNumber = 1395 const G4int G4PAIySection::fRefGammaNumber = 29;
1376 1396
1377 // 1397 //
1378 // end of G4PAIySection implementation file 1398 // end of G4PAIySection implementation file
1379 // 1399 //
1380 ///////////////////////////////////////////// 1400 ////////////////////////////////////////////////////////////////////////////
1381 1401
1382 1402