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27 // ----------------------------------------------------------------------------
28 //
29 //
30 // File name: G4GSMottCorrection
31 //
32 // Author: Mihaly Novak
33 //
34 // Creation date: 23.08.2017
35 //
36 // Modifications:
37 // 02.02.2018 M.Novak: fixed initialization of first moment correction.
38 //
39 // Class description: see the header file.
40 //
41 // -----------------------------------------------------------------------------
42
43 #include "G4GSMottCorrection.hh"
44
45 #include "G4PhysicalConstants.hh"
46 #include "zlib.h"
47 #include "Randomize.hh"
48 #include "G4Log.hh"
49 #include "G4Exp.hh"
50
51 #include "G4ProductionCutsTable.hh"
52 #include "G4MaterialCutsCouple.hh"
53 #include "G4Material.hh"
54 #include "G4ElementVector.hh"
55 #include "G4Element.hh"
56 #include "G4EmParameters.hh"
57
58 #include <iostream>
59 #include <fstream>
60 #include <cmath>
61 #include <algorithm>
62
63
64 const std::string G4GSMottCorrection::gElemSymbols[] = {"H","He","Li","Be","B" ,
65 "C" ,"N" ,"O" ,"F" ,"Ne","Na","Mg","Al","Si","P" , "S","Cl","Ar","K" ,"Ca","Sc",
66 "Ti","V" ,"Cr","Mn","Fe","Co","Ni","Cu","Zn","Ga","Ge","As","Se","Br","Kr","Rb",
67 "Sr","Y" ,"Zr","Nb","Mo","Tc","Ru","Rh","Pd","Ag","Cd","In","Sn","Sb","Te","I" ,
68 "Xe","Cs","Ba","La","Ce","Pr","Nd","Pm","Sm","Eu","Gd","Tb","Dy","Ho","Er","Tm",
69 "Yb","Lu","Hf","Ta","W" ,"Re","Os","Ir","Pt","Au","Hg","Tl","Pb","Bi","Po","At",
70 "Rn","Fr","Ra","Ac","Th","Pa","U" ,"Np","Pu","Am","Cm","Bk","Cf"};
71
72 G4GSMottCorrection::G4GSMottCorrection(G4bool iselectron) : fIsElectron(iselectron) {
73 // init grids related data member values
74 fMaxEkin = CLHEP::electron_mass_c2*(1./std::sqrt(1.-gMaxBeta2)-1.);
75 fLogMinEkin = G4Log(gMinEkin);
76 fInvLogDelEkin = (gNumEkin-gNumBeta2)/G4Log(gMidEkin/gMinEkin);
77 G4double pt2 = gMidEkin*(gMidEkin+2.0*CLHEP::electron_mass_c2);
78 fMinBeta2 = pt2/(pt2+CLHEP::electron_mass_c2*CLHEP::electron_mass_c2);
79 fInvDelBeta2 = (gNumBeta2-1.)/(gMaxBeta2-fMinBeta2);
80 fInvDelDelta = (gNumDelta-1.)/gMaxDelta;
81 fInvDelAngle = gNumAngle-1.;
82 }
83
84
85 G4GSMottCorrection::~G4GSMottCorrection() {
86 ClearMCDataPerElement();
87 ClearMCDataPerMaterial();
88 }
89
90
91 void G4GSMottCorrection::GetMottCorrectionFactors(G4double logekin, G4double beta2, G4int matindx, G4double &mcToScr,
92 G4double &mcToQ1, G4double &mcToG2PerG1) {
93 G4int ekinIndxLow = 0;
94 G4double remRfaction = 0.;
95 if (beta2>=gMaxBeta2) {
96 ekinIndxLow = gNumEkin - 1;
97 // remRfaction = -1.
98 } else if (beta2>=fMinBeta2) { // linear interpolation on \beta^2
99 remRfaction = (beta2 - fMinBeta2) * fInvDelBeta2;
100 ekinIndxLow = (G4int)remRfaction;
101 remRfaction -= ekinIndxLow;
102 ekinIndxLow += (gNumEkin - gNumBeta2);
103 } else if (logekin>=fLogMinEkin) {
104 remRfaction = (logekin - fLogMinEkin) * fInvLogDelEkin;
105 ekinIndxLow = (G4int)remRfaction;
106 remRfaction -= ekinIndxLow;
107 } // the defaults otherwise i.e. use the lowest energy values when ekin is smaller than the minum ekin
108 //
109 DataPerEkin *perEkinLow = fMCDataPerMaterial[matindx]->fDataPerEkin[ekinIndxLow];
110 mcToScr = perEkinLow->fMCScreening;
111 mcToQ1 = perEkinLow->fMCFirstMoment;
112 mcToG2PerG1 = perEkinLow->fMCSecondMoment;
113 if (remRfaction>0.) {
114 DataPerEkin *perEkinHigh = fMCDataPerMaterial[matindx]->fDataPerEkin[ekinIndxLow+1];
115 mcToScr += remRfaction*(perEkinHigh->fMCScreening - perEkinLow->fMCScreening);
116 mcToQ1 += remRfaction*(perEkinHigh->fMCFirstMoment - perEkinLow->fMCFirstMoment);
117 mcToG2PerG1 += remRfaction*(perEkinHigh->fMCSecondMoment - perEkinLow->fMCSecondMoment);
118 }
119 }
120
121
122 // accept cost if rndm [0,1] < return value
123 double G4GSMottCorrection::GetMottRejectionValue(G4double logekin, G4double beta2, G4double q1, G4double cost,
124 G4int matindx, G4int &ekindx, G4int &deltindx) {
125 G4double val = 1.0;
126 G4double delta = q1/(0.5+q1);
127 // check if converged to 1 for all angles => accept cost
128 if (delta>=gMaxDelta) {
129 return val;
130 }
131 //
132 // check if kinetic energy index needs to be determined
133 if (ekindx<0) {
134 G4int ekinIndxLow = 0;
135 G4double probIndxHigh = 0.; // will be the prob. of taking the ekinIndxLow+1 bin
136 if (beta2>gMaxBeta2) {
137 ekinIndxLow = gNumEkin - 1;
138 // probIndxHigh = -1.
139 } else if (beta2>=fMinBeta2) { // linear interpolation on \beta^2
140 probIndxHigh = (beta2 - fMinBeta2) * fInvDelBeta2;
141 ekinIndxLow = (G4int)probIndxHigh;
142 probIndxHigh -= ekinIndxLow;
143 ekinIndxLow += (gNumEkin - gNumBeta2);
144 } else if (logekin>fLogMinEkin) { // linear interpolation on \ln(E_{kin})
145 probIndxHigh = (logekin - fLogMinEkin) * fInvLogDelEkin;
146 ekinIndxLow = (G4int)probIndxHigh;
147 probIndxHigh -= ekinIndxLow;
148 } // the defaults otherwise i.e. use the lowest energy values when ekin is smaller than the minum ekin
149 //
150 // check if need to take the higher ekin index
151 if (G4UniformRand()<probIndxHigh) {
152 ++ekinIndxLow;
153 }
154 // set kinetic energy grid index
155 ekindx = ekinIndxLow;
156 }
157 // check if delta value index needs to be determined (note: in case of single scattering deltindx will be set to 0 by
158 // by the caller but the ekindx will be -1: kinetic energy index is not known but the delta index is known)
159 if (deltindx<0) {
160 // note: delta is for sure < gMaxDelta at this point ( and minimum delta value is 0)
161 G4double probIndxHigh = delta*fInvDelDelta; // will be the prob. of taking the deltIndxLow+1 bin
162 G4int deltIndxLow = (G4int)probIndxHigh;
163 probIndxHigh -= deltIndxLow;
164 // check if need to take the higher delta index
165 if (G4UniformRand()<probIndxHigh) {
166 ++deltIndxLow;
167 }
168 // set the delta value grid index
169 deltindx = deltIndxLow;
170 }
171 //
172 // get the corresponding distribution
173 DataPerDelta *perDelta = fMCDataPerMaterial[matindx]->fDataPerEkin[ekindx]->fDataPerDelta[deltindx];
174 //
175 // determine lower index of the angular bin
176 G4double ang = std::sqrt(0.5*(1.-cost)); // sin(0.5\theta) in [0,1]
177 G4double remRfaction = ang*fInvDelAngle;
178 G4int angIndx = (G4int)remRfaction;
179 remRfaction -= angIndx;
180 if (angIndx<gNumAngle-2) { // normal case: linear interpolation
181 val = remRfaction*(perDelta->fRejFuntion[angIndx+1]-perDelta->fRejFuntion[angIndx]) + perDelta->fRejFuntion[angIndx];
182 } else { // last bin
183 G4double dum = ang-1.+1./fInvDelAngle;
184 val = perDelta->fSA + dum*(perDelta->fSB + dum*(perDelta->fSC + dum*perDelta->fSD));
185 }
186 return val;
187 }
188
189
190 void G4GSMottCorrection::Initialise() {
191 // load Mott-correction data for each elements that belongs to materials that are used in the detector
192 InitMCDataPerElement();
193 // clrea Mott-correction data per material
194 ClearMCDataPerMaterial();
195 // initialise Mott-correction data for the materials that are used in the detector
196 InitMCDataPerMaterials();
197 }
198
199
200 void G4GSMottCorrection::InitMCDataPerElement() {
201 // do it only once
202 if (fMCDataPerElement.size()<gMaxZet+1) {
203 fMCDataPerElement.resize(gMaxZet+1,nullptr);
204 }
205 // loop over all materials, for those that are used check the list of elements and load data from file if the
206 // corresponding data has not been loaded yet
207 G4ProductionCutsTable *thePCTable = G4ProductionCutsTable::GetProductionCutsTable();
208 G4int numMatCuts = (G4int)thePCTable->GetTableSize();
209 for (G4int imc=0; imc<numMatCuts; ++imc) {
210 const G4MaterialCutsCouple *matCut = thePCTable->GetMaterialCutsCouple(imc);
211 if (!matCut->IsUsed()) {
212 continue;
213 }
214 const G4Material *mat = matCut->GetMaterial();
215 const G4ElementVector *elemVect = mat->GetElementVector();
216 //
217 std::size_t numElems = elemVect->size();
218 for (std::size_t ielem=0; ielem<numElems; ++ielem) {
219 const G4Element *elem = (*elemVect)[ielem];
220 G4int izet = G4lrint(elem->GetZ());
221 if (izet>gMaxZet) {
222 izet = gMaxZet;
223 }
224 if (!fMCDataPerElement[izet]) {
225 LoadMCDataElement(elem);
226 }
227 }
228 }
229 }
230
231
232 void G4GSMottCorrection::InitMCDataPerMaterials() {
233 // prepare size of the container
234 std::size_t numMaterials = G4Material::GetNumberOfMaterials();
235 if (fMCDataPerMaterial.size()!=numMaterials) {
236 fMCDataPerMaterial.resize(numMaterials);
237 }
238 // init. Mott-correction data for the Materials that are used in the geometry
239 G4ProductionCutsTable *thePCTable = G4ProductionCutsTable::GetProductionCutsTable();
240 G4int numMatCuts = (G4int)thePCTable->GetTableSize();
241 for (G4int imc=0; imc<numMatCuts; ++imc) {
242 const G4MaterialCutsCouple *matCut = thePCTable->GetMaterialCutsCouple(imc);
243 if (!matCut->IsUsed()) {
244 continue;
245 }
246 const G4Material *mat = matCut->GetMaterial();
247 if (!fMCDataPerMaterial[mat->GetIndex()]) {
248 InitMCDataMaterial(mat);
249 }
250 }
251 }
252
253
254 // it's called only if data has not been loaded for this element yet
255 void G4GSMottCorrection::LoadMCDataElement(const G4Element *elem) {
256 // allocate memory
257 G4int izet = elem->GetZasInt();
258 if (izet>gMaxZet) {
259 izet = gMaxZet;
260 }
261 auto perElem = new DataPerMaterial();
262 AllocateDataPerMaterial(perElem);
263 fMCDataPerElement[izet] = perElem;
264 //
265 // load data from file
266 std::string path = G4EmParameters::Instance()->GetDirLEDATA();
267 if (fIsElectron) {
268 path += "/msc_GS/MottCor/el/";
269 } else {
270 path += "/msc_GS/MottCor/pos/";
271 }
272 std::string fname = path+"rej_"+gElemSymbols[izet-1];
273 std::istringstream infile(std::ios::in);
274 ReadCompressedFile(fname, infile);
275 // check if file is open !!!
276 for (G4int iek=0; iek<gNumEkin; ++iek) {
277 DataPerEkin *perEkin = perElem->fDataPerEkin[iek];
278 // 1. get the 3 Mott-correction factors for the current kinetic energy
279 infile >> perEkin->fMCScreening;
280 infile >> perEkin->fMCFirstMoment;
281 infile >> perEkin->fMCSecondMoment;
282 // 2. load each data per delta:
283 for (G4int idel=0; idel<gNumDelta; ++idel) {
284 DataPerDelta *perDelta = perEkin->fDataPerDelta[idel];
285 // 2./a. : first the rejection function values
286 for (G4int iang=0; iang<gNumAngle; ++iang) {
287 infile >> perDelta->fRejFuntion[iang];
288 }
289 // 2./b. : then the 4 spline parameter for the last bin
290 infile >> perDelta->fSA;
291 infile >> perDelta->fSB;
292 infile >> perDelta->fSC;
293 infile >> perDelta->fSD;
294 }
295 }
296 }
297
298 // uncompress one data file into the input string stream
299 void G4GSMottCorrection::ReadCompressedFile(const std::string& fname, std::istringstream &iss) {
300 std::string *dataString = nullptr;
301 std::string compfilename(fname+".z");
302 // create input stream with binary mode operation and positioning at the end of the file
303 std::ifstream in(compfilename, std::ios::binary | std::ios::ate);
304 if (in.good()) {
305 // get current position in the stream (was set to the end)
306 std::streamoff fileSize = in.tellg();
307 // set current position being the beginning of the stream
308 in.seekg(0,std::ios::beg);
309 // create (zlib) byte buffer for the data
310 Bytef *compdata = new Bytef[fileSize];
311 while(in) {
312 in.read((char*)compdata, fileSize);
313 }
314 // create (zlib) byte buffer for the uncompressed data
315 uLongf complen = (uLongf)(fileSize*4);
316 Bytef *uncompdata = new Bytef[complen];
317 while (Z_OK!=uncompress(uncompdata, &complen, compdata, fileSize)) {
318 // increase uncompressed byte buffer
319 delete[] uncompdata;
320 complen *= 2;
321 uncompdata = new Bytef[complen];
322 }
323 // delete the compressed data buffer
324 delete [] compdata;
325 // create a string from the uncompressed data (will be deallocated by the caller)
326 dataString = new std::string((char*)uncompdata, (long)complen);
327 // delete the uncompressed data buffer
328 delete [] uncompdata;
329 } else {
330 std::string msg = " Problem while trying to read " + compfilename + " data file.\n";
331 G4Exception("G4GSMottCorrection::ReadCompressedFile","em0006", FatalException,msg.c_str());
332 return;
333 }
334 // create the input string stream from the data string
335 if (dataString) {
336 iss.str(*dataString);
337 in.close();
338 delete dataString;
339 }
340 }
341
342
343 void G4GSMottCorrection::InitMCDataMaterial(const G4Material *mat) {
344 constexpr G4double const1 = 7821.6; // [cm2/g]
345 constexpr G4double const2 = 0.1569; // [cm2 MeV2 / g]
346 constexpr G4double finstrc2 = 5.325135453E-5; // fine-structure const. square
347
348 G4double constFactor = CLHEP::electron_mass_c2*CLHEP::fine_structure_const/0.88534;
349 constFactor *= constFactor; // (mc^2)^2\alpha^2/( C_{TF}^2)
350 // allocate memory
351 auto perMat = new DataPerMaterial();
352 AllocateDataPerMaterial(perMat);
353 fMCDataPerMaterial[mat->GetIndex()] = perMat;
354 //
355 const G4ElementVector* elemVect = mat->GetElementVector();
356 const G4int numElems = (G4int)mat->GetNumberOfElements();
357 const G4double* nbAtomsPerVolVect = mat->GetVecNbOfAtomsPerVolume();
358 G4double totNbAtomsPerVol = mat->GetTotNbOfAtomsPerVolume();
359 //
360 // 1. Compute material dependent part of Moliere's b_c \chi_c^2
361 // (with \xi=1 (i.e. total sub-threshold scattering power correction)
362 G4double moliereBc = 0.0;
363 G4double moliereXc2 = 0.0;
364 G4double zs = 0.0;
365 G4double ze = 0.0;
366 G4double zx = 0.0;
367 G4double sa = 0.0;
368 G4double xi = 1.0;
369 for (G4int ielem=0; ielem<numElems; ++ielem) {
370 G4double zet = (*elemVect)[ielem]->GetZ();
371 if (zet>gMaxZet) {
372 zet = (G4double)gMaxZet;
373 }
374 G4double iwa = (*elemVect)[ielem]->GetN();
375 G4double ipz = nbAtomsPerVolVect[ielem]/totNbAtomsPerVol;
376 G4double dum = ipz*zet*(zet+xi);
377 zs += dum;
378 ze += dum*(-2.0/3.0)*G4Log(zet);
379 zx += dum*G4Log(1.0+3.34*finstrc2*zet*zet);
380 sa += ipz*iwa;
381 }
382 G4double density = mat->GetDensity()*CLHEP::cm3/CLHEP::g; // [g/cm3]
383 //
384 G4double z0 = (0.0 == sa) ? 0.0 : zs/sa;
385 G4double z1 = (0.0 == zs) ? 0.0 : (ze - zx)/zs;
386
387 moliereBc = const1*density*z0*G4Exp(z1); //[1/cm]
388 moliereXc2 = const2*density*z0; // [MeV2/cm]
389 // change to Geant4 internal units of 1/length and energ2/length
390 moliereBc *= 1.0/CLHEP::cm;
391 moliereXc2 *= CLHEP::MeV*CLHEP::MeV/CLHEP::cm;
392 //
393 // 2. loop over the kinetic energy grid
394 for (G4int iek=0; iek<gNumEkin; ++iek) {
395 // 2./a. set current kinetic energy and pt2 value
396 G4double ekin = G4Exp(fLogMinEkin+iek/fInvLogDelEkin);
397 G4double pt2 = ekin*(ekin+2.0*CLHEP::electron_mass_c2);
398 if (ekin>gMidEkin) {
399 G4double b2 = fMinBeta2+(iek-(gNumEkin-gNumBeta2))/fInvDelBeta2;
400 ekin = CLHEP::electron_mass_c2*(1./std::sqrt(1.-b2)-1.);
401 pt2 = ekin*(ekin+2.0*CLHEP::electron_mass_c2);
402 }
403 // 2./b. loop over the elements at the current kinetic energy point
404 for (G4int ielem=0; ielem<numElems; ++ielem) {
405 const G4Element *elem = (*elemVect)[ielem];
406 G4double zet = elem->GetZ();
407 if (zet>gMaxZet) {
408 zet = (G4double)gMaxZet;
409 }
410 G4int izet = G4lrint(zet);
411 // xi should be one i.e. z(z+1) since total sub-threshold scattering power correction
412 G4double nZZPlus1 = nbAtomsPerVolVect[ielem]*zet*(zet+1.0)/totNbAtomsPerVol;
413 G4double Z23 = std::pow(zet,2./3.);
414 //
415 DataPerEkin *perElemPerEkin = fMCDataPerElement[izet]->fDataPerEkin[iek];
416 DataPerEkin *perMatPerEkin = perMat->fDataPerEkin[iek];
417 //
418 // 2./b./(i) Add the 3 Mott-correction factors
419 G4double mcScrCF = perElemPerEkin->fMCScreening; // \kappa_i[1.13+3.76(\alpha Z_i)^2] with \kappa_i=scr_mc/scr_sr
420 // compute the screening parameter correction factor (Z_i contribution to the material)
421 // src_{mc} = C \exp\left[ \frac{ \sum_i n_i Z_i(Z_i+1)\ln[Z_{i}^{2/3}\kappa_i(1.13+3.76(\alpha Z_i)^2)] } {\sum_i n_i Z_i(Z_i+1)}
422 // with C = \frac{(mc^2)^\alpha^2} {4(pc)^2 C_{TF}^2} = constFactor/(4*(pc)^2)
423 // here we compute the \sum_i n_i Z_i(Z_i+1)\ln[Z_{i}^{2/3}\kappa_i(1.13+3.76(\alpha Z_i)^2)] part
424 perMatPerEkin->fMCScreening += nZZPlus1*G4Log(Z23*mcScrCF);
425 // compute the corrected screening parameter for the current Z_i and E_{kin}
426 // src(Z_i)_{mc} = \frac{(mc^2)^\alpha^2 Z_i^{2/3}} {4(pc)^2 C_{TF}^2} \kappa_i[1.13+3.76(\alpha Z_i)^2]
427 mcScrCF *= constFactor*Z23/(4.*pt2);
428 // compute first moment correction factor
429 // q1_{mc} = \frac{ \sum_i n_i Z_i(Z_i+1) A_i B_i } {\sum_i n_i Z_i(Z_i+1)} \frac{1}{C}
430 // where:
431 // A_i(src(Z_i)_{mc}) = [\ln(1+1/src(Z_i)_{mc}) - 1/(1+src(Z_i)_{mc})]; where \sigma(Z_i)_{tr1}^(sr) = A_i(src(Z_i)_{mc}) [2\pi r_0 Z_i mc^2/(pc)\beta]^2
432 // B_i = \beta_i \gamma_i with beta_i(Z_i) = \sigma(Z_i)_{tr1}^(PWA)/\sigma(Z_i,src(Z_i)_{mc})_{tr1}^(sr)
433 // and \gamma_i = \sigma(Z_i)_{el}^(MC-DCS)/\sigma(Z_i,src(Z_i)_{mc})_{el}^(sr)
434 // C(src_{mc}) = [\ln(1+1/src_{mc}) - 1/(1+src_{mc})]; where \sigma_{tr1}^(sr) = C(src_{mc}) [2\pi r_0 Z_i mc^2/(pc)\beta]^2
435 // A_i x B_i is stored in file per e-/e+, E_{kin} and Z_i
436 // here we compute the \sum_i n_i Z_i(Z_i+1) A_i B_i part
437 perMatPerEkin->fMCFirstMoment += nZZPlus1*(G4Log(1.+1./mcScrCF)-1./(1.+mcScrCF))*perElemPerEkin->fMCFirstMoment;
438 // compute the second moment correction factor
439 // [G2/G1]_{mc} = \frac{ \sum_i n_i Z_i(Z_i+1) A_i } {\sum_i n_i Z_i(Z_i+1)} \frac{1}{C}
440 // with A_i(Z_i) = G2(Z_i)^{PWA}/G1(Z_i)^{PWA} and C=G2(Z_i,scr_{mc})^{sr}/G1(Z_i,scr_{mc})^{sr}}
441 // here we compute the \sum_i n_i Z_i(Z_i+1) A_i part
442 perMatPerEkin->fMCSecondMoment += nZZPlus1*perElemPerEkin->fMCSecondMoment;
443 //
444 // 2./b./(ii) Go for the rejection funtion part
445 // I. loop over delta values
446 for (G4int idel=0; idel<gNumDelta; ++idel) {
447 DataPerDelta *perMatPerDelta = perMatPerEkin->fDataPerDelta[idel];
448 DataPerDelta *perElemPerDelta = perElemPerEkin->fDataPerDelta[idel];
449 // I./a. loop over angles (i.e. the \sin(0.5\theta) values) and add the rejection function
450 for (G4int iang=0; iang<gNumAngle; ++iang) {
451 perMatPerDelta->fRejFuntion[iang] += nZZPlus1*perElemPerDelta->fRejFuntion[iang];
452 }
453 // I./b. get the last bin spline parameters and add them (a+bx+cx^2+dx^3)
454 perMatPerDelta->fSA += nZZPlus1*perElemPerDelta->fSA;
455 perMatPerDelta->fSB += nZZPlus1*perElemPerDelta->fSB;
456 perMatPerDelta->fSC += nZZPlus1*perElemPerDelta->fSC;
457 perMatPerDelta->fSD += nZZPlus1*perElemPerDelta->fSD;
458 }
459 //
460 // 2./b./(iii) When the last element has been added:
461 if (ielem==numElems-1) {
462 //
463 // 1. the remaining part of the sreening correction and divide the corrected screening par. with Moliere's one:
464 // (Moliere screening parameter = moliereXc2/(4(pc)^2 moliereBc) )
465 G4double dumScr = G4Exp(perMatPerEkin->fMCScreening/zs);
466 perMatPerEkin->fMCScreening = constFactor*dumScr*moliereBc/moliereXc2;
467 //
468 // 2. the remaining part of the first moment correction and divide by the one computed by using the corrected
469 // screening parameter (= (mc^2)^\alpha^2/(4(pc)^2C_{TF}^2) dumScr
470 G4double scrCorTed = constFactor*dumScr/(4.*pt2);
471 G4double dum0 = G4Log(1.+1./scrCorTed);
472 perMatPerEkin->fMCFirstMoment = perMatPerEkin->fMCFirstMoment/(zs*(dum0-1./(1.+scrCorTed)));
473 //
474 // 3. the remaining part of the second moment correction and divide by the one computed by using the corrected
475 // screening parameter
476 G4double G2PerG1 = 3.*(1.+scrCorTed)*((1.+2.*scrCorTed)*dum0-2.)/((1.+scrCorTed)*dum0-1.);
477 perMatPerEkin->fMCSecondMoment = perMatPerEkin->fMCSecondMoment/(zs*G2PerG1);
478 //
479 // 4. scale the maximum of the rejection function to unity and correct the last bin spline parameters as well
480 // I. loop over delta values
481 for (G4int idel=0; idel<gNumDelta; ++idel) {
482 DataPerDelta *perMatPerDelta = perMatPerEkin->fDataPerDelta[idel];
483 G4double maxVal = -1.;
484 // II. llop over angles
485 for (G4int iang=0; iang<gNumAngle; ++iang) {
486 if (perMatPerDelta->fRejFuntion[iang]>maxVal)
487 maxVal = perMatPerDelta->fRejFuntion[iang];
488 }
489 for (G4int iang=0; iang<gNumAngle; ++iang) {
490 perMatPerDelta->fRejFuntion[iang] /=maxVal;
491 }
492 perMatPerDelta->fSA /= maxVal;
493 perMatPerDelta->fSB /= maxVal;
494 perMatPerDelta->fSC /= maxVal;
495 perMatPerDelta->fSD /= maxVal;
496 }
497 }
498 }
499 }
500 }
501
502
503 void G4GSMottCorrection::AllocateDataPerMaterial(DataPerMaterial *data) {
504 data->fDataPerEkin = new DataPerEkin*[gNumEkin]();
505 for (G4int iek=0; iek<gNumEkin; ++iek) {
506 auto perEkin = new DataPerEkin();
507 perEkin->fDataPerDelta = new DataPerDelta*[gNumDelta]();
508 for (G4int idel=0; idel<gNumDelta; ++idel) {
509 auto perDelta = new DataPerDelta();
510 perDelta->fRejFuntion = new double[gNumAngle]();
511 perEkin->fDataPerDelta[idel] = perDelta;
512 }
513 data->fDataPerEkin[iek] = perEkin;
514 }
515 }
516
517 void G4GSMottCorrection::DeAllocateDataPerMaterial(DataPerMaterial *data) {
518 for (G4int iek=0; iek<gNumEkin; ++iek) {
519 DataPerEkin *perEkin = data->fDataPerEkin[iek]; //new DataPerEkin();
520 for (G4int idel=0; idel<gNumDelta; ++idel) {
521 DataPerDelta *perDelta = perEkin->fDataPerDelta[idel];
522 delete [] perDelta->fRejFuntion;
523 delete perDelta;
524 }
525 delete [] perEkin->fDataPerDelta;
526 delete perEkin;
527 }
528 delete [] data->fDataPerEkin;
529 }
530
531
532 void G4GSMottCorrection::ClearMCDataPerElement() {
533 for (std::size_t i=0; i<fMCDataPerElement.size(); ++i) {
534 if (fMCDataPerElement[i]) {
535 DeAllocateDataPerMaterial(fMCDataPerElement[i]);
536 delete fMCDataPerElement[i];
537 }
538 }
539 fMCDataPerElement.clear();
540 }
541
542 void G4GSMottCorrection::ClearMCDataPerMaterial() {
543 for (std::size_t i=0; i<fMCDataPerMaterial.size(); ++i) {
544 if (fMCDataPerMaterial[i]) {
545 DeAllocateDataPerMaterial(fMCDataPerMaterial[i]);
546 delete fMCDataPerMaterial[i];
547 }
548 }
549 fMCDataPerMaterial.clear();
550 }
551