source: trunk/source/processes/electromagnetic/lowenergy/src/G4LowEnergyBremsstrahlung.cc@ 1036

Last change on this file since 1036 was 1007, checked in by garnier, 17 years ago

update to geant4.9.2
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[819]1//
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25//
26// $Id: G4LowEnergyBremsstrahlung.cc,v 1.71 2006/06/29 19:40:13 gunter Exp $
[1007]27// GEANT4 tag $Name: geant4-09-02 $
[819]28//
29// --------------------------------------------------------------
30//
31// File name: G4LowEnergyBremsstrahlung
32//
33// Author: Alessandra Forti, Vladimir Ivanchenko
34//
35// Creation date: March 1999
36//
37// Modifications:
38// 18.04.2000 V.L.
39// - First implementation of continuous energy loss.
40// 17.02.2000 Veronique Lefebure
41// - correct bug : the gamma energy was not deposited when the gamma was
42// not produced when its energy was < cutForLowEnergySecondaryPhotons
43//
44// Added Livermore data table construction methods A. Forti
45// Modified BuildMeanFreePath to read new data tables A. Forti
46// Modified PostStepDoIt to insert sampling with with EEDL data A. Forti
47// Added SelectRandomAtom A. Forti
48// Added map of the elements A. Forti
49// 20.09.00 update printout V.Ivanchenko
50// 24.04.01 V.Ivanchenko remove RogueWave
51// 29.09.2001 V.Ivanchenko: major revision based on design iteration
52// 10.10.2001 MGP Revision to improve code quality and consistency with design
53// 18.10.2001 MGP Revision to improve code quality
54// 28.10.2001 VI Update printout
55// 29.11.2001 VI New parametrisation
56// 30.07.2002 VI Fix in restricted energy loss
57// 21.01.2003 VI Cut per region
58// 21.02.2003 V.Ivanchenko Energy bins for spectrum are defined here
59// 28.02.03 V.Ivanchenko Filename is defined in the constructor
60// 24.03.2003 P.Rodrigues Changes to accommodate new angular generators
61// 20.05.2003 MGP Removed memory leak related to angularDistribution
62// 06.11.2003 MGP Improved user interface to select angular distribution model
63//
64// --------------------------------------------------------------
65
66#include "G4LowEnergyBremsstrahlung.hh"
67#include "G4eBremsstrahlungSpectrum.hh"
68#include "G4BremsstrahlungCrossSectionHandler.hh"
69#include "G4VBremAngularDistribution.hh"
70#include "G4ModifiedTsai.hh"
71#include "G4Generator2BS.hh"
72#include "G4Generator2BN.hh"
73#include "G4VDataSetAlgorithm.hh"
74#include "G4LogLogInterpolation.hh"
75#include "G4VEMDataSet.hh"
76#include "G4EnergyLossTables.hh"
77#include "G4UnitsTable.hh"
78#include "G4Electron.hh"
79#include "G4Gamma.hh"
80#include "G4ProductionCutsTable.hh"
81
82
83G4LowEnergyBremsstrahlung::G4LowEnergyBremsstrahlung(const G4String& nam)
84 : G4eLowEnergyLoss(nam),
85 crossSectionHandler(0),
86 theMeanFreePath(0),
87 energySpectrum(0)
88{
89 cutForPhotons = 0.;
90 verboseLevel = 0;
91 generatorName = "tsai";
92 angularDistribution = new G4ModifiedTsai("TsaiGenerator"); // default generator
93// angularDistribution->PrintGeneratorInformation();
94 TsaiAngularDistribution = new G4ModifiedTsai("TsaiGenerator");
95}
96
97/*
98G4LowEnergyBremsstrahlung::G4LowEnergyBremsstrahlung(const G4String& nam, G4VBremAngularDistribution* distribution)
99 : G4eLowEnergyLoss(nam),
100 crossSectionHandler(0),
101 theMeanFreePath(0),
102 energySpectrum(0),
103 angularDistribution(distribution)
104{
105 cutForPhotons = 0.;
106 verboseLevel = 0;
107
108 angularDistribution->PrintGeneratorInformation();
109
110 TsaiAngularDistribution = new G4ModifiedTsai("TsaiGenerator");
111}
112*/
113
114G4LowEnergyBremsstrahlung::~G4LowEnergyBremsstrahlung()
115{
116 if(crossSectionHandler) delete crossSectionHandler;
117 if(energySpectrum) delete energySpectrum;
118 if(theMeanFreePath) delete theMeanFreePath;
119 delete angularDistribution;
120 delete TsaiAngularDistribution;
121 energyBins.clear();
122}
123
124
125void G4LowEnergyBremsstrahlung::BuildPhysicsTable(const G4ParticleDefinition& aParticleType)
126{
127 if(verboseLevel > 0) {
128 G4cout << "G4LowEnergyBremsstrahlung::BuildPhysicsTable start"
129 << G4endl;
130 }
131
132 cutForSecondaryPhotons.clear();
133
134 // Create and fill BremsstrahlungParameters once
135 if( energySpectrum != 0 ) delete energySpectrum;
136 energyBins.clear();
137 for(size_t i=0; i<15; i++) {
138 G4double x = 0.1*((G4double)i);
139 if(i == 0) x = 0.01;
140 if(i == 10) x = 0.95;
141 if(i == 11) x = 0.97;
142 if(i == 12) x = 0.99;
143 if(i == 13) x = 0.995;
144 if(i == 14) x = 1.0;
145 energyBins.push_back(x);
146 }
147 const G4String dataName("/brem/br-sp.dat");
148 energySpectrum = new G4eBremsstrahlungSpectrum(energyBins,dataName);
149
150 if(verboseLevel > 0) {
151 G4cout << "G4LowEnergyBremsstrahlungSpectrum is initialized"
152 << G4endl;
153 }
154
155 // Create and fill G4CrossSectionHandler once
156
157 if( crossSectionHandler != 0 ) delete crossSectionHandler;
158 G4VDataSetAlgorithm* interpolation = new G4LogLogInterpolation();
159 G4double lowKineticEnergy = GetLowerBoundEloss();
160 G4double highKineticEnergy = GetUpperBoundEloss();
161 G4int totBin = GetNbinEloss();
162 crossSectionHandler = new G4BremsstrahlungCrossSectionHandler(energySpectrum, interpolation);
163 crossSectionHandler->Initialise(0,lowKineticEnergy, highKineticEnergy, totBin);
164 crossSectionHandler->LoadShellData("brem/br-cs-");
165
166 if (verboseLevel > 0) {
167 G4cout << GetProcessName()
168 << " is created; Cross section data: "
169 << G4endl;
170 crossSectionHandler->PrintData();
171 G4cout << "Parameters: "
172 << G4endl;
173 energySpectrum->PrintData();
174 }
175
176 // Build loss table for Bremsstrahlung
177
178 BuildLossTable(aParticleType);
179
180 if(verboseLevel > 0) {
181 G4cout << "The loss table is built"
182 << G4endl;
183 }
184
185 if (&aParticleType==G4Electron::Electron()) {
186
187 RecorderOfElectronProcess[CounterOfElectronProcess] = (*this).theLossTable;
188 CounterOfElectronProcess++;
189 PrintInfoDefinition();
190
191 } else {
192
193 RecorderOfPositronProcess[CounterOfPositronProcess] = (*this).theLossTable;
194 CounterOfPositronProcess++;
195 }
196
197 // Build mean free path data using cut values
198
199 if( theMeanFreePath != 0 ) delete theMeanFreePath;
200 theMeanFreePath = crossSectionHandler->
201 BuildMeanFreePathForMaterials(&cutForSecondaryPhotons);
202
203 if(verboseLevel > 0) {
204 G4cout << "The MeanFreePath table is built"
205 << G4endl;
206 }
207
208 // Build common DEDX table for all ionisation processes
209
210 BuildDEDXTable(aParticleType);
211
212 if(verboseLevel > 0) {
213 G4cout << "G4LowEnergyBremsstrahlung::BuildPhysicsTable end"
214 << G4endl;
215 }
216
217}
218
219
220void G4LowEnergyBremsstrahlung::BuildLossTable(const G4ParticleDefinition& )
221{
222 // Build table for energy loss due to soft brems
223 // the tables are built for *MATERIALS* binning is taken from LowEnergyLoss
224
225 G4double lowKineticEnergy = GetLowerBoundEloss();
226 G4double highKineticEnergy = GetUpperBoundEloss();
227 size_t totBin = GetNbinEloss();
228
229 // create table
230
231 if (theLossTable) {
232 theLossTable->clearAndDestroy();
233 delete theLossTable;
234 }
235 const G4ProductionCutsTable* theCoupleTable=
236 G4ProductionCutsTable::GetProductionCutsTable();
237 size_t numOfCouples = theCoupleTable->GetTableSize();
238 theLossTable = new G4PhysicsTable(numOfCouples);
239
240 // Clean up the vector of cuts
241 cutForSecondaryPhotons.clear();
242
243 // Loop for materials
244
245 for (size_t j=0; j<numOfCouples; j++) {
246
247 // create physics vector and fill it
248 G4PhysicsLogVector* aVector = new G4PhysicsLogVector(lowKineticEnergy,
249 highKineticEnergy,
250 totBin);
251
252 // get material parameters needed for the energy loss calculation
253 const G4MaterialCutsCouple* couple = theCoupleTable->GetMaterialCutsCouple(j);
254 const G4Material* material= couple->GetMaterial();
255
256 // the cut cannot be below lowest limit
257 G4double tCut = (*(theCoupleTable->GetEnergyCutsVector(0)))[j];
258 tCut = std::min(highKineticEnergy, tCut);
259 cutForSecondaryPhotons.push_back(tCut);
260
261 const G4ElementVector* theElementVector = material->GetElementVector();
262 size_t NumberOfElements = material->GetNumberOfElements() ;
263 const G4double* theAtomicNumDensityVector =
264 material->GetAtomicNumDensityVector();
265 if(verboseLevel > 1) {
266 G4cout << "Energy loss for material # " << j
267 << " tCut(keV)= " << tCut/keV
268 << G4endl;
269 }
270
271 // now comes the loop for the kinetic energy values
272 for (size_t i = 0; i<totBin; i++) {
273
274 G4double lowEdgeEnergy = aVector->GetLowEdgeEnergy(i);
275 G4double ionloss = 0.;
276
277 // loop for elements in the material
278 for (size_t iel=0; iel<NumberOfElements; iel++ ) {
279 G4int Z = (G4int)((*theElementVector)[iel]->GetZ());
280 G4double e = energySpectrum->AverageEnergy(Z, 0.0, tCut, lowEdgeEnergy);
281 G4double cs= crossSectionHandler->FindValue(Z, lowEdgeEnergy);
282 ionloss += e * cs * theAtomicNumDensityVector[iel];
283 if(verboseLevel > 1) {
284 G4cout << "Z= " << Z
285 << "; tCut(keV)= " << tCut/keV
286 << "; E(keV)= " << lowEdgeEnergy/keV
287 << "; Eav(keV)= " << e/keV
288 << "; cs= " << cs
289 << "; loss= " << ionloss
290 << G4endl;
291 }
292 }
293 aVector->PutValue(i,ionloss);
294 }
295 theLossTable->insert(aVector);
296 }
297}
298
299
300G4VParticleChange* G4LowEnergyBremsstrahlung::PostStepDoIt(const G4Track& track,
301 const G4Step& step)
302{
303 aParticleChange.Initialize(track);
304
305 const G4MaterialCutsCouple* couple = track.GetMaterialCutsCouple();
306 G4double kineticEnergy = track.GetKineticEnergy();
307 G4int index = couple->GetIndex();
308 G4double tCut = cutForSecondaryPhotons[index];
309
310 // Control limits
311 if(tCut >= kineticEnergy)
312 return G4VContinuousDiscreteProcess::PostStepDoIt(track, step);
313
314 G4int Z = crossSectionHandler->SelectRandomAtom(couple, kineticEnergy);
315
316 G4double tGamma = energySpectrum->SampleEnergy(Z, tCut, kineticEnergy, kineticEnergy);
317 G4double totalEnergy = kineticEnergy + electron_mass_c2;
318 G4double finalEnergy = kineticEnergy - tGamma; // electron/positron final energy
319 G4double theta = 0;
320
321 if((kineticEnergy < 1*MeV && kineticEnergy > 1*keV && generatorName == "2bn")){
322 theta = angularDistribution->PolarAngle(kineticEnergy,finalEnergy,Z);
323 }else{
324 theta = TsaiAngularDistribution->PolarAngle(kineticEnergy,finalEnergy,Z);
325 }
326
327 G4double phi = twopi * G4UniformRand();
328 G4double dirZ = std::cos(theta);
329 G4double sinTheta = std::sqrt(1. - dirZ*dirZ);
330 G4double dirX = sinTheta*std::cos(phi);
331 G4double dirY = sinTheta*std::sin(phi);
332
333 G4ThreeVector gammaDirection (dirX, dirY, dirZ);
334 G4ThreeVector electronDirection = track.GetMomentumDirection();
335
336 //
337 // Update the incident particle
338 //
339 gammaDirection.rotateUz(electronDirection);
340
341 // Kinematic problem
342 if (finalEnergy < 0.) {
343 tGamma += finalEnergy;
344 finalEnergy = 0.0;
345 }
346
347 G4double momentum = std::sqrt((totalEnergy + electron_mass_c2)*kineticEnergy);
348
349 G4double finalX = momentum*electronDirection.x() - tGamma*gammaDirection.x();
350 G4double finalY = momentum*electronDirection.y() - tGamma*gammaDirection.y();
351 G4double finalZ = momentum*electronDirection.z() - tGamma*gammaDirection.z();
352
353 aParticleChange.SetNumberOfSecondaries(1);
354 G4double norm = 1./std::sqrt(finalX*finalX + finalY*finalY + finalZ*finalZ);
355 aParticleChange.ProposeMomentumDirection(finalX*norm, finalY*norm, finalZ*norm);
356 aParticleChange.ProposeEnergy( finalEnergy );
357
358 // create G4DynamicParticle object for the gamma
359 G4DynamicParticle* aGamma= new G4DynamicParticle (G4Gamma::Gamma(),
360 gammaDirection, tGamma);
361 aParticleChange.AddSecondary(aGamma);
362
363 return G4VContinuousDiscreteProcess::PostStepDoIt(track, step);
364}
365
366
367void G4LowEnergyBremsstrahlung::PrintInfoDefinition()
368{
369 G4String comments = "Total cross sections from EEDL database.";
370 comments += "\n Gamma energy sampled from a parameterised formula.";
371 comments += "\n Implementation of the continuous dE/dx part.";
372 comments += "\n At present it can be used for electrons ";
373 comments += "in the energy range [250eV,100GeV].";
374 comments += "\n The process must work with G4LowEnergyIonisation.";
375
376 G4cout << G4endl << GetProcessName() << ": " << comments << G4endl;
377}
378
379G4bool G4LowEnergyBremsstrahlung::IsApplicable(const G4ParticleDefinition& particle)
380{
381 return ( (&particle == G4Electron::Electron()) );
382}
383
384
385G4double G4LowEnergyBremsstrahlung::GetMeanFreePath(const G4Track& track,
386 G4double,
387 G4ForceCondition* cond)
388{
389 *cond = NotForced;
390 G4int index = (track.GetMaterialCutsCouple())->GetIndex();
391 const G4VEMDataSet* data = theMeanFreePath->GetComponent(index);
392 G4double meanFreePath = data->FindValue(track.GetKineticEnergy());
393 return meanFreePath;
394}
395
396void G4LowEnergyBremsstrahlung::SetCutForLowEnSecPhotons(G4double cut)
397{
398 cutForPhotons = cut;
399}
400
401void G4LowEnergyBremsstrahlung::SetAngularGenerator(G4VBremAngularDistribution* distribution)
402{
403 angularDistribution = distribution;
404 angularDistribution->PrintGeneratorInformation();
405}
406
407void G4LowEnergyBremsstrahlung::SetAngularGenerator(const G4String& name)
408{
409 if (name == "tsai")
410 {
411 delete angularDistribution;
412 angularDistribution = new G4ModifiedTsai("TsaiGenerator");
413 generatorName = name;
414 }
415 else if (name == "2bn")
416 {
417 delete angularDistribution;
418 angularDistribution = new G4Generator2BN("2BNGenerator");
419 generatorName = name;
420 }
421 else if (name == "2bs")
422 {
423 delete angularDistribution;
424 angularDistribution = new G4Generator2BS("2BSGenerator");
425 generatorName = name;
426 }
427 else
428 {
429 G4Exception("G4LowEnergyBremsstrahlung::SetAngularGenerator - generator does not exist");
430 }
431
432 angularDistribution->PrintGeneratorInformation();
433}
434
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