Geant4 10.7.0
Toolkit for the simulation of the passage of particles through matter
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G4ecpssrBaseKxsModel Class Reference

#include <G4ecpssrBaseKxsModel.hh>

+ Inheritance diagram for G4ecpssrBaseKxsModel:

Public Member Functions

 G4ecpssrBaseKxsModel ()
 
 ~G4ecpssrBaseKxsModel ()
 
G4double CalculateCrossSection (G4int, G4double, G4double)
 
G4double ExpIntFunction (G4int n, G4double x)
 
- Public Member Functions inherited from G4VecpssrKModel
 G4VecpssrKModel ()
 
virtual ~G4VecpssrKModel ()
 
virtual G4double CalculateCrossSection (G4int zTarget, G4double massIncident, G4double energyIncident)=0
 

Detailed Description

Definition at line 38 of file G4ecpssrBaseKxsModel.hh.

Constructor & Destructor Documentation

◆ G4ecpssrBaseKxsModel()

G4ecpssrBaseKxsModel::G4ecpssrBaseKxsModel ( )

Definition at line 46 of file G4ecpssrBaseKxsModel.cc.

47{
48 verboseLevel=0;
49
50 // Storing C coefficients for high velocity formula
51
52 G4String fileC1("pixe/uf/c1");
53 tableC1 = new G4CrossSectionDataSet(new G4SemiLogInterpolation, 1.,1.);
54
55 G4String fileC2("pixe/uf/c2");
56 tableC2 = new G4CrossSectionDataSet(new G4SemiLogInterpolation, 1.,1.);
57
58 G4String fileC3("pixe/uf/c3");
59 tableC3 = new G4CrossSectionDataSet(new G4SemiLogInterpolation, 1.,1.);
60
61 // Storing FK data needed for medium velocities region
62 char *path = 0;
63
64 path = std::getenv("G4LEDATA");
65
66 if (!path) {
67 G4Exception("G4ecpssrBaseKxsModel::G4ecpssrBaseKxsModel()", "em0006", FatalException,"G4LEDATA environment variable not set" );
68 return;
69 }
70
71 std::ostringstream fileName;
72 fileName << path << "/pixe/uf/FK.dat";
73 std::ifstream FK(fileName.str().c_str());
74
75 if (!FK)
76 G4Exception("G4ecpssrBaseKxsModel::G4ecpssrBaseKxsModel()", "em0003", FatalException,"error opening FK data file" );
77
78 dummyVec.push_back(0.);
79
80 while(!FK.eof())
81 {
82 double x;
83 double y;
84
85 FK>>x>>y;
86
87 // Mandatory vector initialization
88 if (x != dummyVec.back())
89 {
90 dummyVec.push_back(x);
91 aVecMap[x].push_back(-1.);
92 }
93
94 FK>>FKData[x][y];
95
96 if (y != aVecMap[x].back()) aVecMap[x].push_back(y);
97
98 }
99
100 tableC1->LoadData(fileC1);
101 tableC2->LoadData(fileC2);
102 tableC3->LoadData(fileC3);
103
104}
@ FatalException
void G4Exception(const char *originOfException, const char *exceptionCode, G4ExceptionSeverity severity, const char *description)
Definition: G4Exception.cc:35
virtual G4bool LoadData(const G4String &argFileName)

◆ ~G4ecpssrBaseKxsModel()

G4ecpssrBaseKxsModel::~G4ecpssrBaseKxsModel ( )

Definition at line 114 of file G4ecpssrBaseKxsModel.cc.

115{
116
117 delete tableC1;
118 delete tableC2;
119 delete tableC3;
120
121}

Member Function Documentation

◆ CalculateCrossSection()

G4double G4ecpssrBaseKxsModel::CalculateCrossSection ( G4int  zTarget,
G4double  massIncident,
G4double  energyIncident 
)
virtual

Implements G4VecpssrKModel.

Definition at line 197 of file G4ecpssrBaseKxsModel.cc.

199{
200
201 // this K-CrossSection calculation method is done according to W.Brandt and G.Lapicki, Phys.Rev.A23(1981)//
202
203 G4NistManager* massManager = G4NistManager::Instance();
204
206
207 G4double zIncident = 0;
208 G4Proton* aProtone = G4Proton::Proton();
209 G4Alpha* aAlpha = G4Alpha::Alpha();
210
211 if (massIncident == aProtone->GetPDGMass() )
212 {
213 zIncident = (aProtone->GetPDGCharge())/eplus;
214 }
215 else
216 {
217 if (massIncident == aAlpha->GetPDGMass())
218 {
219 zIncident = (aAlpha->GetPDGCharge())/eplus;
220 }
221 else
222 {
223 G4cout << "*** WARNING in G4ecpssrBaseKxsModel::CalculateCrossSection : we can treat only Proton or Alpha incident particles " << G4endl;
224 return 0;
225 }
226 }
227
228 if (verboseLevel>0) G4cout << " massIncident=" << massIncident<< G4endl;
229
230 G4double kBindingEnergy = transitionManager->Shell(zTarget,0)->BindingEnergy();
231
232 if (verboseLevel>0) G4cout << " kBindingEnergy=" << kBindingEnergy/eV<< G4endl;
233
234 G4double massTarget = (massManager->GetAtomicMassAmu(zTarget))*amu_c2;
235
236 if (verboseLevel>0) G4cout << " massTarget=" << massTarget<< G4endl;
237
238 G4double systemMass =((massIncident*massTarget)/(massIncident+massTarget))/electron_mass_c2; //the mass of the system (projectile, target)
239
240 if (verboseLevel>0) G4cout << " systemMass=" << systemMass<< G4endl;
241
242 const G4double zkshell= 0.3;
243 // *** see Brandt, Phys Rev A23, p 1727
244
245 G4double screenedzTarget = zTarget-zkshell; // screenedzTarget is the screened nuclear charge of the target
246 // *** see Brandt, Phys Rev A23, p 1727
247
248 const G4double rydbergMeV= 13.6056923e-6;
249
250 G4double tetaK = kBindingEnergy/((screenedzTarget*screenedzTarget)*rydbergMeV); //tetaK denotes the reduced binding energy of the electron
251 // *** see Rice, ADANDT 20, p 504, f 2
252
253 if (verboseLevel>0) G4cout << " tetaK=" << tetaK<< G4endl;
254
255 G4double velocity =(2./(tetaK*screenedzTarget))*std::pow(((energyIncident*electron_mass_c2)/(massIncident*rydbergMeV)),0.5);
256 // *** also called xiK
257 // *** see Brandt, Phys Rev A23, p 1727
258 // *** see Basbas, Phys Rev A17, p 1656, f4
259
260 if (verboseLevel>0) G4cout << " velocity=" << velocity<< G4endl;
261
262 const G4double bohrPow2Barn=(Bohr_radius*Bohr_radius)/barn ;
263
264 if (verboseLevel>0) G4cout << " bohrPow2Barn=" << bohrPow2Barn<< G4endl;
265
266 G4double sigma0 = 8.*pi*(zIncident*zIncident)*bohrPow2Barn*std::pow(screenedzTarget,-4.); //sigma0 is the initial cross section of K shell at stable state
267 // *** see Benka, ADANDT 22, p 220, f2, for protons
268 // *** see Basbas, Phys Rev A7, p 1000
269
270 if (verboseLevel>0) G4cout << " sigma0=" << sigma0<< G4endl;
271
272 const G4double kAnalyticalApproximation= 1.5;
273 G4double x = kAnalyticalApproximation/velocity;
274 // *** see Brandt, Phys Rev A23, p 1727
275 // *** see Brandt, Phys Rev A20, p 469, f16 in expression of h
276
277 if (verboseLevel>0) G4cout << " x=" << x<< G4endl;
278
279 G4double electrIonizationEnergy;
280 // *** see Basbas, Phys Rev A17, p1665, f27
281 // *** see Brandt, Phys Rev A20, p469
282 // *** see Liu, Comp Phys Comm 97, p325, f A5
283
284 if ((0.< x) && (x <= 0.035))
285 {
286 electrIonizationEnergy= 0.75*pi*(std::log(1./(x*x))-1.);
287 }
288 else
289 {
290 if ( (0.035 < x) && (x <=3.))
291 {
292 electrIonizationEnergy =G4Exp(-2.*x)/(0.031+(0.213*std::pow(x,0.5))+(0.005*x)-(0.069*std::pow(x,3./2.))+(0.324*x*x));
293 }
294
295 else
296 {
297 if ( (3.< x) && (x<=11.))
298 {
299 electrIonizationEnergy =2.*G4Exp(-2.*x)/std::pow(x,1.6);
300 }
301
302 else electrIonizationEnergy =0.;
303 }
304 }
305
306 if (verboseLevel>0) G4cout << " electrIonizationEnergy=" << electrIonizationEnergy<< G4endl;
307
308 G4double hFunction =(electrIonizationEnergy*2.)/(tetaK*std::pow(velocity,3)); //hFunction represents the correction for polarization effet
309 // *** see Brandt, Phys Rev A20, p 469, f16
310
311 if (verboseLevel>0) G4cout << " hFunction=" << hFunction<< G4endl;
312
313 G4double gFunction = (1.+(9.*velocity)+(31.*velocity*velocity)+(98.*std::pow(velocity,3.))+(12.*std::pow(velocity,4.))+(25.*std::pow(velocity,5.))
314 +(4.2*std::pow(velocity,6.))+(0.515*std::pow(velocity,7.)))/std::pow(1.+velocity,9.); //gFunction represents the correction for binding effet
315 // *** see Brandt, Phys Rev A20, p 469, f19
316
317 if (verboseLevel>0) G4cout << " gFunction=" << gFunction<< G4endl;
318
319 //-----------------------------------------------------------------------------------------------------------------------------
320
321 G4double sigmaPSS = 1.+(((2.*zIncident)/(screenedzTarget*tetaK))*(gFunction-hFunction)); //describes the perturbed stationnairy state of the affected atomic electon
322 // *** also called dzeta
323 // *** also called epsilon
324 // *** see Basbas, Phys Rev A17, p1667, f45
325
326 if (verboseLevel>0) G4cout << " sigmaPSS=" << sigmaPSS<< G4endl;
327
328 if (verboseLevel>0) G4cout << " sigmaPSS*tetaK=" << sigmaPSS*tetaK<< G4endl;
329
330 //----------------------------------------------------------------------------------------------------------------------------
331
332 const G4double cNaturalUnit= 1/fine_structure_const; // it's the speed of light according to Atomic-Unit-System
333
334 if (verboseLevel>0) G4cout << " cNaturalUnit=" << cNaturalUnit<< G4endl;
335
336 G4double ykFormula=0.4*(screenedzTarget/cNaturalUnit)*(screenedzTarget/cNaturalUnit)/(velocity/sigmaPSS);
337 // *** also called yS
338 // *** see Brandt, Phys Rev A20, p467, f6
339 // *** see Brandt, Phys Rev A23, p1728
340
341 if (verboseLevel>0) G4cout << " ykFormula=" << ykFormula<< G4endl;
342
343 G4double relativityCorrection = std::pow((1.+(1.1*ykFormula*ykFormula)),0.5)+ykFormula;// the relativistic correction parameter
344 // *** also called mRS
345 // *** see Brandt, Phys Rev A20, p467, f6
346
347 if (verboseLevel>0) G4cout << " relativityCorrection=" << relativityCorrection<< G4endl;
348
349 G4double reducedVelocity = velocity*std::pow(relativityCorrection,0.5); // presents the reduced collision velocity parameter
350 // *** also called xiR
351 // *** see Brandt, Phys Rev A20, p468, f7
352 // *** see Brandt, Phys Rev A23, p1728
353
354 if (verboseLevel>0) G4cout << " reducedVelocity=" << reducedVelocity<< G4endl;
355
356 G4double etaOverTheta2 = (energyIncident*electron_mass_c2)/(massIncident*rydbergMeV*screenedzTarget*screenedzTarget)
357 /(sigmaPSS*tetaK)/(sigmaPSS*tetaK);
358 // *** see Benka, ADANDT 22, p220, f4 for eta
359 // then we use sigmaPSS*tetaK == epsilon*tetaK
360
361 if (verboseLevel>0) G4cout << " etaOverTheta2=" << etaOverTheta2<< G4endl;
362
363 G4double universalFunction = 0;
364
365 // low velocity formula
366 // *****************
367 if ( velocity < 1. )
368 // OR
369 //if ( reducedVelocity/sigmaPSS < 1.)
370 // *** see Brandt, Phys Rev A23, p1727
371 // *** reducedVelocity/sigmaPSS is also called xiR/dzeta
372 // *****************
373 {
374 if (verboseLevel>0) G4cout << " Notice : FK is computed from low velocity formula" << G4endl;
375
376 universalFunction = (std::pow(2.,9.)/45.)*std::pow(reducedVelocity/sigmaPSS,8.)*std::pow((1.+(1.72*(reducedVelocity/sigmaPSS)*(reducedVelocity/sigmaPSS))),-4.);// is the reduced universal cross section
377 // *** see Brandt, Phys Rev A23, p1728
378
379 if (verboseLevel>0) G4cout << " universalFunction by Brandt 1981 =" << universalFunction<< G4endl;
380
381 }
382
383 else
384
385 {
386
387 if ( etaOverTheta2 > 86.6 && (sigmaPSS*tetaK) > 0.4 && (sigmaPSS*tetaK) < 2.9996 )
388 {
389 // High and medium energies. Method from Rice ADANDT 20, p506, 1977 on tables from Benka 1978
390
391 if (verboseLevel>0) G4cout << " Notice : FK is computed from high velocity formula" << G4endl;
392
393 if (verboseLevel>0) G4cout << " sigmaPSS*tetaK=" << sigmaPSS*tetaK << G4endl;
394
395 G4double C1= tableC1->FindValue(sigmaPSS*tetaK);
396 G4double C2= tableC2->FindValue(sigmaPSS*tetaK);
397 G4double C3= tableC3->FindValue(sigmaPSS*tetaK);
398
399 if (verboseLevel>0) G4cout << " C1=" << C1 << G4endl;
400 if (verboseLevel>0) G4cout << " C2=" << C2 << G4endl;
401 if (verboseLevel>0) G4cout << " C3=" << C3 << G4endl;
402
403 G4double etaK = (energyIncident*electron_mass_c2)/(massIncident*rydbergMeV*screenedzTarget*screenedzTarget);
404 // *** see Benka, ADANDT 22, p220, f4 for eta
405
406 if (verboseLevel>0) G4cout << " etaK=" << etaK << G4endl;
407
408 G4double etaT = (sigmaPSS*tetaK)*(sigmaPSS*tetaK)*(86.6); // at any theta, the largest tabulated etaOverTheta2 is 86.6
409 // *** see Rice, ADANDT 20, p506
410
411 if (verboseLevel>0) G4cout << " etaT=" << etaT << G4endl;
412
413 G4double fKT = FunctionFK((sigmaPSS*tetaK),86.6)*(etaT/(sigmaPSS*tetaK));
414 // *** see Rice, ADANDT 20, p506
415
416 if (FunctionFK((sigmaPSS*tetaK),86.6)<=0.)
417 {
418 G4cout <<
419 "*** WARNING in G4ecpssrBaseKxsModel::CalculateCrossSection : unable to interpolate FK function in high velocity region ! ***" << G4endl;
420 return 0;
421 }
422
423 if (verboseLevel>0) G4cout << " FunctionFK=" << FunctionFK((sigmaPSS*tetaK),86.6) << G4endl;
424
425 if (verboseLevel>0) G4cout << " fKT=" << fKT << G4endl;
426
427 G4double GK = C2/(4*etaK) + C3/(32*etaK*etaK);
428
429 if (verboseLevel>0) G4cout << " GK=" << GK << G4endl;
430
431 G4double GT = C2/(4*etaT) + C3/(32*etaT*etaT);
432
433 if (verboseLevel>0) G4cout << " GT=" << GT << G4endl;
434
435 G4double DT = fKT - C1*std::log(etaT) + GT;
436
437 if (verboseLevel>0) G4cout << " DT=" << DT << G4endl;
438
439 G4double fKK = C1*std::log(etaK) + DT - GK;
440
441 if (verboseLevel>0) G4cout << " fKK=" << fKK << G4endl;
442
443 G4double universalFunction3= fKK/(etaK/tetaK);
444 // *** see Rice, ADANDT 20, p505, f7
445
446 if (verboseLevel>0) G4cout << " universalFunction3=" << universalFunction3 << G4endl;
447
448 universalFunction=universalFunction3;
449
450 }
451
452 else if ( etaOverTheta2 >= 1.e-3 && etaOverTheta2 <= 86.6 && (sigmaPSS*tetaK) >= 0.4 && (sigmaPSS*tetaK) <= 2.9996 )
453
454 {
455 // From Benka 1978
456
457 if (verboseLevel>0) G4cout << " Notice : FK is computed from INTERPOLATED data" << G4endl;
458
459 G4double universalFunction2 = FunctionFK((sigmaPSS*tetaK),etaOverTheta2);
460
461 if (universalFunction2<=0)
462 {
463 G4cout <<
464 "*** WARNING : G4ecpssrBaseKxsModel::CalculateCrossSection is unable to interpolate FK function in medium velocity region ! ***" << G4endl;
465 return 0;
466 }
467
468 if (verboseLevel>0) G4cout << " universalFunction2=" << universalFunction2 << " for theta=" << sigmaPSS*tetaK << " and etaOverTheta2=" << etaOverTheta2 << G4endl;
469
470 universalFunction=universalFunction2;
471 }
472
473 }
474
475 //----------------------------------------------------------------------------------------------------------------------
476
477 G4double sigmaPSSR = (sigma0/(sigmaPSS*tetaK))*universalFunction; //sigmaPSSR is the straight-line K-shell ionization cross section
478 // *** see Benka, ADANDT 22, p220, f1
479
480 if (verboseLevel>0) G4cout << " sigmaPSSR=" << sigmaPSSR<< G4endl;
481
482 //-----------------------------------------------------------------------------------------------------------------------
483
484 G4double pssDeltaK = (4./(systemMass*sigmaPSS*tetaK))*(sigmaPSS/velocity)*(sigmaPSS/velocity);
485 // *** also called dzetaK*deltaK
486 // *** see Brandt, Phys Rev A23, p1727, f B2
487
488 if (verboseLevel>0) G4cout << " pssDeltaK=" << pssDeltaK<< G4endl;
489
490 if (pssDeltaK>1) return 0.;
491
492 G4double energyLoss = std::pow(1-pssDeltaK,0.5); //energyLoss incorporates the straight-line energy-loss
493 // *** also called zK
494 // *** see Brandt, Phys Rev A23, p1727, after f B2
495
496 if (verboseLevel>0) G4cout << " energyLoss=" << energyLoss<< G4endl;
497
498 G4double energyLossFunction = (std::pow(2.,-9)/8.)*((((9.*energyLoss)-1.)*std::pow(1.+energyLoss,9.))+(((9.*energyLoss)+1.)*std::pow(1.-energyLoss,9.)));//energy loss function
499 // *** also called fs
500 // *** see Brandt, Phys Rev A23, p1718, f7
501
502 if (verboseLevel>0) G4cout << " energyLossFunction=" << energyLossFunction<< G4endl;
503
504 //----------------------------------------------------------------------------------------------------------------------------------------------
505
506 G4double coulombDeflection = (4.*pi*zIncident/systemMass)*std::pow(tetaK*sigmaPSS,-2.)*std::pow(velocity/sigmaPSS,-3.)*(zTarget/screenedzTarget); //incorporates Coulomb deflection parameter
507 // *** see Brandt, Phys Rev A23, p1727, f B3
508
509 if (verboseLevel>0) G4cout << " cParameter-short=" << coulombDeflection<< G4endl;
510
511 G4double cParameter = 2.*coulombDeflection/(energyLoss*(energyLoss+1.));
512 // *** see Brandt, Phys Rev A23, p1727, f B4
513
514 if (verboseLevel>0) G4cout << " cParameter-full=" << cParameter<< G4endl;
515
516 G4double coulombDeflectionFunction = 9.*ExpIntFunction(10,cParameter); //this function describes Coulomb-deflection effect
517 // *** see Brandt, Phys Rev A23, p1727
518
519 if (verboseLevel>0) G4cout << " ExpIntFunction(10,cParameter) =" << ExpIntFunction(10,cParameter) << G4endl;
520
521 if (verboseLevel>0) G4cout << " coulombDeflectionFunction =" << coulombDeflectionFunction << G4endl;
522
523 //--------------------------------------------------------------------------------------------------------------------------------------------------
524
525 G4double crossSection = 0;
526
527 crossSection = energyLossFunction* coulombDeflectionFunction*sigmaPSSR; //this ECPSSR cross section is estimated at perturbed-stationnairy-state(PSS)
528 //and it's reduced by the energy-loss(E),the Coulomb deflection(C),
529 //and the relativity(R) effects
530
531 //--------------------------------------------------------------------------------------------------------------------------------------------------
532
533 if (crossSection >= 0) {
534 return crossSection * barn;
535 }
536 else {return 0;}
537
538}
@ GT
Definition: Evaluator.cc:65
G4double G4Exp(G4double initial_x)
Exponential Function double precision.
Definition: G4Exp.hh:179
double G4double
Definition: G4Types.hh:83
#define G4endl
Definition: G4ios.hh:57
G4GLOB_DLL std::ostream G4cout
const double C2
#define C1
#define C3
static G4Alpha * Alpha()
Definition: G4Alpha.cc:88
G4double BindingEnergy() const
G4AtomicShell * Shell(G4int Z, size_t shellIndex) const
static G4AtomicTransitionManager * Instance()
virtual G4double FindValue(G4double e, G4int componentId=0) const
static G4NistManager * Instance()
G4double GetAtomicMassAmu(const G4String &symb) const
G4double GetPDGCharge() const
static G4Proton * Proton()
Definition: G4Proton.cc:92
G4double ExpIntFunction(G4int n, G4double x)
const G4double pi

◆ ExpIntFunction()

G4double G4ecpssrBaseKxsModel::ExpIntFunction ( G4int  n,
G4double  x 
)

Definition at line 125 of file G4ecpssrBaseKxsModel.cc.

127{
128// this "ExpIntFunction" function allows fast evaluation of the n order exponential integral function En(x)
129
130 G4int i;
131 G4int ii;
132 G4int nm1;
133 G4double a;
134 G4double b;
135 G4double c;
136 G4double d;
137 G4double del;
138 G4double fact;
139 G4double h;
140 G4double psi;
141 G4double ans = 0;
142 const G4double euler= 0.5772156649;
143 const G4int maxit= 100;
144 const G4double fpmin = 1.0e-30;
145 const G4double eps = 1.0e-7;
146 nm1=n-1;
147 if (n<0 || x<0.0 || (x==0.0 && (n==0 || n==1))) {
148 G4cout << "*** WARNING in G4ecpssrBaseKxsModel::ExpIntFunction: bad arguments in ExpIntFunction" << G4endl;
149 G4cout << n << ", " << x << G4endl;
150 }
151 else {
152 if (n==0) ans=G4Exp(-x)/x;
153 else {
154 if (x==0.0) ans=1.0/nm1;
155 else {
156 if (x > 1.0) {
157 b=x+n;
158 c=1.0/fpmin;
159 d=1.0/b;
160 h=d;
161 for (i=1;i<=maxit;i++) {
162 a=-i*(nm1+i);
163 b +=2.0;
164 d=1.0/(a*d+b);
165 c=b+a/c;
166 del=c*d;
167 h *=del;
168 if (std::fabs(del-1.0) < eps) {
169 ans=h*G4Exp(-x);
170 return ans;
171 }
172 }
173 } else {
174 ans = (nm1!=0 ? 1.0/nm1 : -std::log(x)-euler);
175 fact=1.0;
176 for (i=1;i<=maxit;i++) {
177 fact *=-x/i;
178 if (i !=nm1) del = -fact/(i-nm1);
179 else {
180 psi = -euler;
181 for (ii=1;ii<=nm1;ii++) psi +=1.0/ii;
182 del=fact*(-std::log(x)+psi);
183 }
184 ans += del;
185 if (std::fabs(del) < std::fabs(ans)*eps) return ans;
186 }
187 }
188 }
189 }
190 }
191return ans;
192}
int G4int
Definition: G4Types.hh:85

Referenced by CalculateCrossSection().


The documentation for this class was generated from the following files: