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geant4/source/processes/electromagnetic/standard/src/G4GSMottCorrection.cc
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Gabriele Cosmo dd1f179cda Import Geant4 11.2.0.beta source tree
2023-06-30 09:09:57 +02:00

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//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
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// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
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// * any work based on the software) you agree to acknowledge its *
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// ********************************************************************
//
//
// ----------------------------------------------------------------------------
//
//
// File name: G4GSMottCorrection
//
// Author: Mihaly Novak
//
// Creation date: 23.08.2017
//
// Modifications:
// 02.02.2018 M.Novak: fixed initialization of first moment correction.
//
// Class description: see the header file.
//
// -----------------------------------------------------------------------------
#include "G4GSMottCorrection.hh"
#include "G4PhysicalConstants.hh"
#include "zlib.h"
#include "Randomize.hh"
#include "G4Log.hh"
#include "G4Exp.hh"
#include "G4ProductionCutsTable.hh"
#include "G4MaterialCutsCouple.hh"
#include "G4Material.hh"
#include "G4ElementVector.hh"
#include "G4Element.hh"
#include "G4EmParameters.hh"
#include <iostream>
#include <fstream>
#include <cmath>
#include <algorithm>
const std::string G4GSMottCorrection::gElemSymbols[] = {"H","He","Li","Be","B" ,
"C" ,"N" ,"O" ,"F" ,"Ne","Na","Mg","Al","Si","P" , "S","Cl","Ar","K" ,"Ca","Sc",
"Ti","V" ,"Cr","Mn","Fe","Co","Ni","Cu","Zn","Ga","Ge","As","Se","Br","Kr","Rb",
"Sr","Y" ,"Zr","Nb","Mo","Tc","Ru","Rh","Pd","Ag","Cd","In","Sn","Sb","Te","I" ,
"Xe","Cs","Ba","La","Ce","Pr","Nd","Pm","Sm","Eu","Gd","Tb","Dy","Ho","Er","Tm",
"Yb","Lu","Hf","Ta","W" ,"Re","Os","Ir","Pt","Au","Hg","Tl","Pb","Bi","Po","At",
"Rn","Fr","Ra","Ac","Th","Pa","U" ,"Np","Pu","Am","Cm","Bk","Cf"};
G4GSMottCorrection::G4GSMottCorrection(G4bool iselectron) : fIsElectron(iselectron) {
// init grids related data member values
fMaxEkin = CLHEP::electron_mass_c2*(1./std::sqrt(1.-gMaxBeta2)-1.);
fLogMinEkin = G4Log(gMinEkin);
fInvLogDelEkin = (gNumEkin-gNumBeta2)/G4Log(gMidEkin/gMinEkin);
G4double pt2 = gMidEkin*(gMidEkin+2.0*CLHEP::electron_mass_c2);
fMinBeta2 = pt2/(pt2+CLHEP::electron_mass_c2*CLHEP::electron_mass_c2);
fInvDelBeta2 = (gNumBeta2-1.)/(gMaxBeta2-fMinBeta2);
fInvDelDelta = (gNumDelta-1.)/gMaxDelta;
fInvDelAngle = gNumAngle-1.;
}
G4GSMottCorrection::~G4GSMottCorrection() {
ClearMCDataPerElement();
ClearMCDataPerMaterial();
}
void G4GSMottCorrection::GetMottCorrectionFactors(G4double logekin, G4double beta2, G4int matindx, G4double &mcToScr,
G4double &mcToQ1, G4double &mcToG2PerG1) {
G4int ekinIndxLow = 0;
G4double remRfaction = 0.;
if (beta2>=gMaxBeta2) {
ekinIndxLow = gNumEkin - 1;
// remRfaction = -1.
} else if (beta2>=fMinBeta2) { // linear interpolation on \beta^2
remRfaction = (beta2 - fMinBeta2) * fInvDelBeta2;
ekinIndxLow = (G4int)remRfaction;
remRfaction -= ekinIndxLow;
ekinIndxLow += (gNumEkin - gNumBeta2);
} else if (logekin>=fLogMinEkin) {
remRfaction = (logekin - fLogMinEkin) * fInvLogDelEkin;
ekinIndxLow = (G4int)remRfaction;
remRfaction -= ekinIndxLow;
} // the defaults otherwise i.e. use the lowest energy values when ekin is smaller than the minum ekin
//
DataPerEkin *perEkinLow = fMCDataPerMaterial[matindx]->fDataPerEkin[ekinIndxLow];
mcToScr = perEkinLow->fMCScreening;
mcToQ1 = perEkinLow->fMCFirstMoment;
mcToG2PerG1 = perEkinLow->fMCSecondMoment;
if (remRfaction>0.) {
DataPerEkin *perEkinHigh = fMCDataPerMaterial[matindx]->fDataPerEkin[ekinIndxLow+1];
mcToScr += remRfaction*(perEkinHigh->fMCScreening - perEkinLow->fMCScreening);
mcToQ1 += remRfaction*(perEkinHigh->fMCFirstMoment - perEkinLow->fMCFirstMoment);
mcToG2PerG1 += remRfaction*(perEkinHigh->fMCSecondMoment - perEkinLow->fMCSecondMoment);
}
}
// accept cost if rndm [0,1] < return value
double G4GSMottCorrection::GetMottRejectionValue(G4double logekin, G4double beta2, G4double q1, G4double cost,
G4int matindx, G4int &ekindx, G4int &deltindx) {
G4double val = 1.0;
G4double delta = q1/(0.5+q1);
// check if converged to 1 for all angles => accept cost
if (delta>=gMaxDelta) {
return val;
}
//
// check if kinetic energy index needs to be determined
if (ekindx<0) {
G4int ekinIndxLow = 0;
G4double probIndxHigh = 0.; // will be the prob. of taking the ekinIndxLow+1 bin
if (beta2>gMaxBeta2) {
ekinIndxLow = gNumEkin - 1;
// probIndxHigh = -1.
} else if (beta2>=fMinBeta2) { // linear interpolation on \beta^2
probIndxHigh = (beta2 - fMinBeta2) * fInvDelBeta2;
ekinIndxLow = (G4int)probIndxHigh;
probIndxHigh -= ekinIndxLow;
ekinIndxLow += (gNumEkin - gNumBeta2);
} else if (logekin>fLogMinEkin) { // linear interpolation on \ln(E_{kin})
probIndxHigh = (logekin - fLogMinEkin) * fInvLogDelEkin;
ekinIndxLow = (G4int)probIndxHigh;
probIndxHigh -= ekinIndxLow;
} // the defaults otherwise i.e. use the lowest energy values when ekin is smaller than the minum ekin
//
// check if need to take the higher ekin index
if (G4UniformRand()<probIndxHigh) {
++ekinIndxLow;
}
// set kinetic energy grid index
ekindx = ekinIndxLow;
}
// check if delta value index needs to be determined (note: in case of single scattering deltindx will be set to 0 by
// by the caller but the ekindx will be -1: kinetic energy index is not known but the delta index is known)
if (deltindx<0) {
// note: delta is for sure < gMaxDelta at this point ( and minimum delta value is 0)
G4double probIndxHigh = delta*fInvDelDelta; // will be the prob. of taking the deltIndxLow+1 bin
G4int deltIndxLow = (G4int)probIndxHigh;
probIndxHigh -= deltIndxLow;
// check if need to take the higher delta index
if (G4UniformRand()<probIndxHigh) {
++deltIndxLow;
}
// set the delta value grid index
deltindx = deltIndxLow;
}
//
// get the corresponding distribution
DataPerDelta *perDelta = fMCDataPerMaterial[matindx]->fDataPerEkin[ekindx]->fDataPerDelta[deltindx];
//
// determine lower index of the angular bin
G4double ang = std::sqrt(0.5*(1.-cost)); // sin(0.5\theta) in [0,1]
G4double remRfaction = ang*fInvDelAngle;
G4int angIndx = (G4int)remRfaction;
remRfaction -= angIndx;
if (angIndx<gNumAngle-2) { // normal case: linear interpolation
val = remRfaction*(perDelta->fRejFuntion[angIndx+1]-perDelta->fRejFuntion[angIndx]) + perDelta->fRejFuntion[angIndx];
} else { // last bin
G4double dum = ang-1.+1./fInvDelAngle;
val = perDelta->fSA + dum*(perDelta->fSB + dum*(perDelta->fSC + dum*perDelta->fSD));
}
return val;
}
void G4GSMottCorrection::Initialise() {
// load Mott-correction data for each elements that belongs to materials that are used in the detector
InitMCDataPerElement();
// clrea Mott-correction data per material
ClearMCDataPerMaterial();
// initialise Mott-correction data for the materials that are used in the detector
InitMCDataPerMaterials();
}
void G4GSMottCorrection::InitMCDataPerElement() {
// do it only once
if (fMCDataPerElement.size()<gMaxZet+1) {
fMCDataPerElement.resize(gMaxZet+1,nullptr);
}
// loop over all materials, for those that are used check the list of elements and load data from file if the
// corresponding data has not been loaded yet
G4ProductionCutsTable *thePCTable = G4ProductionCutsTable::GetProductionCutsTable();
G4int numMatCuts = (G4int)thePCTable->GetTableSize();
for (G4int imc=0; imc<numMatCuts; ++imc) {
const G4MaterialCutsCouple *matCut = thePCTable->GetMaterialCutsCouple(imc);
if (!matCut->IsUsed()) {
continue;
}
const G4Material *mat = matCut->GetMaterial();
const G4ElementVector *elemVect = mat->GetElementVector();
//
std::size_t numElems = elemVect->size();
for (std::size_t ielem=0; ielem<numElems; ++ielem) {
const G4Element *elem = (*elemVect)[ielem];
G4int izet = G4lrint(elem->GetZ());
if (izet>gMaxZet) {
izet = gMaxZet;
}
if (!fMCDataPerElement[izet]) {
LoadMCDataElement(elem);
}
}
}
}
void G4GSMottCorrection::InitMCDataPerMaterials() {
// prepare size of the container
std::size_t numMaterials = G4Material::GetNumberOfMaterials();
if (fMCDataPerMaterial.size()!=numMaterials) {
fMCDataPerMaterial.resize(numMaterials);
}
// init. Mott-correction data for the Materials that are used in the geometry
G4ProductionCutsTable *thePCTable = G4ProductionCutsTable::GetProductionCutsTable();
G4int numMatCuts = (G4int)thePCTable->GetTableSize();
for (G4int imc=0; imc<numMatCuts; ++imc) {
const G4MaterialCutsCouple *matCut = thePCTable->GetMaterialCutsCouple(imc);
if (!matCut->IsUsed()) {
continue;
}
const G4Material *mat = matCut->GetMaterial();
if (!fMCDataPerMaterial[mat->GetIndex()]) {
InitMCDataMaterial(mat);
}
}
}
// it's called only if data has not been loaded for this element yet
void G4GSMottCorrection::LoadMCDataElement(const G4Element *elem) {
// allocate memory
G4int izet = elem->GetZasInt();
if (izet>gMaxZet) {
izet = gMaxZet;
}
auto perElem = new DataPerMaterial();
AllocateDataPerMaterial(perElem);
fMCDataPerElement[izet] = perElem;
//
// load data from file
std::string path = G4EmParameters::Instance()->GetDirLEDATA();
if (fIsElectron) {
path += "/msc_GS/MottCor/el/";
} else {
path += "/msc_GS/MottCor/pos/";
}
std::string fname = path+"rej_"+gElemSymbols[izet-1];
std::istringstream infile(std::ios::in);
ReadCompressedFile(fname, infile);
// check if file is open !!!
for (G4int iek=0; iek<gNumEkin; ++iek) {
DataPerEkin *perEkin = perElem->fDataPerEkin[iek];
// 1. get the 3 Mott-correction factors for the current kinetic energy
infile >> perEkin->fMCScreening;
infile >> perEkin->fMCFirstMoment;
infile >> perEkin->fMCSecondMoment;
// 2. load each data per delta:
for (G4int idel=0; idel<gNumDelta; ++idel) {
DataPerDelta *perDelta = perEkin->fDataPerDelta[idel];
// 2./a. : first the rejection function values
for (G4int iang=0; iang<gNumAngle; ++iang) {
infile >> perDelta->fRejFuntion[iang];
}
// 2./b. : then the 4 spline parameter for the last bin
infile >> perDelta->fSA;
infile >> perDelta->fSB;
infile >> perDelta->fSC;
infile >> perDelta->fSD;
}
}
}
// uncompress one data file into the input string stream
void G4GSMottCorrection::ReadCompressedFile(std::string fname, std::istringstream &iss) {
std::string *dataString = nullptr;
std::string compfilename(fname+".z");
// create input stream with binary mode operation and positioning at the end of the file
std::ifstream in(compfilename, std::ios::binary | std::ios::ate);
if (in.good()) {
// get current position in the stream (was set to the end)
std::streamoff fileSize = in.tellg();
// set current position being the beginning of the stream
in.seekg(0,std::ios::beg);
// create (zlib) byte buffer for the data
Bytef *compdata = new Bytef[fileSize];
while(in) {
in.read((char*)compdata, fileSize);
}
// create (zlib) byte buffer for the uncompressed data
uLongf complen = (uLongf)(fileSize*4);
Bytef *uncompdata = new Bytef[complen];
while (Z_OK!=uncompress(uncompdata, &complen, compdata, fileSize)) {
// increase uncompressed byte buffer
delete[] uncompdata;
complen *= 2;
uncompdata = new Bytef[complen];
}
// delete the compressed data buffer
delete [] compdata;
// create a string from the uncompressed data (will be deallocated by the caller)
dataString = new std::string((char*)uncompdata, (long)complen);
// delete the uncompressed data buffer
delete [] uncompdata;
} else {
std::string msg = " Problem while trying to read " + compfilename + " data file.\n";
G4Exception("G4GSMottCorrection::ReadCompressedFile","em0006", FatalException,msg.c_str());
return;
}
// create the input string stream from the data string
if (dataString) {
iss.str(*dataString);
in.close();
delete dataString;
}
}
void G4GSMottCorrection::InitMCDataMaterial(const G4Material *mat) {
constexpr G4double const1 = 7821.6; // [cm2/g]
constexpr G4double const2 = 0.1569; // [cm2 MeV2 / g]
constexpr G4double finstrc2 = 5.325135453E-5; // fine-structure const. square
G4double constFactor = CLHEP::electron_mass_c2*CLHEP::fine_structure_const/0.88534;
constFactor *= constFactor; // (mc^2)^2\alpha^2/( C_{TF}^2)
// allocate memory
auto perMat = new DataPerMaterial();
AllocateDataPerMaterial(perMat);
fMCDataPerMaterial[mat->GetIndex()] = perMat;
//
const G4ElementVector* elemVect = mat->GetElementVector();
const G4int numElems = (G4int)mat->GetNumberOfElements();
const G4double* nbAtomsPerVolVect = mat->GetVecNbOfAtomsPerVolume();
G4double totNbAtomsPerVol = mat->GetTotNbOfAtomsPerVolume();
//
// 1. Compute material dependent part of Moliere's b_c \chi_c^2
// (with \xi=1 (i.e. total sub-threshold scattering power correction)
G4double moliereBc = 0.0;
G4double moliereXc2 = 0.0;
G4double zs = 0.0;
G4double ze = 0.0;
G4double zx = 0.0;
G4double sa = 0.0;
G4double xi = 1.0;
for (G4int ielem=0; ielem<numElems; ++ielem) {
G4double zet = (*elemVect)[ielem]->GetZ();
if (zet>gMaxZet) {
zet = (G4double)gMaxZet;
}
G4double iwa = (*elemVect)[ielem]->GetN();
G4double ipz = nbAtomsPerVolVect[ielem]/totNbAtomsPerVol;
G4double dum = ipz*zet*(zet+xi);
zs += dum;
ze += dum*(-2.0/3.0)*G4Log(zet);
zx += dum*G4Log(1.0+3.34*finstrc2*zet*zet);
sa += ipz*iwa;
}
G4double density = mat->GetDensity()*CLHEP::cm3/CLHEP::g; // [g/cm3]
//
moliereBc = const1*density*zs/sa*G4Exp(ze/zs)/G4Exp(zx/zs); //[1/cm]
moliereXc2 = const2*density*zs/sa; // [MeV2/cm]
// change to Geant4 internal units of 1/length and energ2/length
moliereBc *= 1.0/CLHEP::cm;
moliereXc2 *= CLHEP::MeV*CLHEP::MeV/CLHEP::cm;
//
// 2. loop over the kinetic energy grid
for (G4int iek=0; iek<gNumEkin; ++iek) {
// 2./a. set current kinetic energy and pt2 value
G4double ekin = G4Exp(fLogMinEkin+iek/fInvLogDelEkin);
G4double pt2 = ekin*(ekin+2.0*CLHEP::electron_mass_c2);
if (ekin>gMidEkin) {
G4double b2 = fMinBeta2+(iek-(gNumEkin-gNumBeta2))/fInvDelBeta2;
ekin = CLHEP::electron_mass_c2*(1./std::sqrt(1.-b2)-1.);
pt2 = ekin*(ekin+2.0*CLHEP::electron_mass_c2);
}
// 2./b. loop over the elements at the current kinetic energy point
for (G4int ielem=0; ielem<numElems; ++ielem) {
const G4Element *elem = (*elemVect)[ielem];
G4double zet = elem->GetZ();
if (zet>gMaxZet) {
zet = (G4double)gMaxZet;
}
G4int izet = G4lrint(zet);
// xi should be one i.e. z(z+1) since total sub-threshold scattering power correction
G4double nZZPlus1 = nbAtomsPerVolVect[ielem]*zet*(zet+1.0)/totNbAtomsPerVol;
G4double Z23 = std::pow(zet,2./3.);
//
DataPerEkin *perElemPerEkin = fMCDataPerElement[izet]->fDataPerEkin[iek];
DataPerEkin *perMatPerEkin = perMat->fDataPerEkin[iek];
//
// 2./b./(i) Add the 3 Mott-correction factors
G4double mcScrCF = perElemPerEkin->fMCScreening; // \kappa_i[1.13+3.76(\alpha Z_i)^2] with \kappa_i=scr_mc/scr_sr
// compute the screening parameter correction factor (Z_i contribution to the material)
// 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)}
// with C = \frac{(mc^2)^\alpha^2} {4(pc)^2 C_{TF}^2} = constFactor/(4*(pc)^2)
// 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
perMatPerEkin->fMCScreening += nZZPlus1*G4Log(Z23*mcScrCF);
// compute the corrected screening parameter for the current Z_i and E_{kin}
// 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]
mcScrCF *= constFactor*Z23/(4.*pt2);
// compute first moment correction factor
// 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}
// where:
// 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
// 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)
// and \gamma_i = \sigma(Z_i)_{el}^(MC-DCS)/\sigma(Z_i,src(Z_i)_{mc})_{el}^(sr)
// 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
// A_i x B_i is stored in file per e-/e+, E_{kin} and Z_i
// here we compute the \sum_i n_i Z_i(Z_i+1) A_i B_i part
perMatPerEkin->fMCFirstMoment += nZZPlus1*(G4Log(1.+1./mcScrCF)-1./(1.+mcScrCF))*perElemPerEkin->fMCFirstMoment;
// compute the second moment correction factor
// [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}
// 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}}
// here we compute the \sum_i n_i Z_i(Z_i+1) A_i part
perMatPerEkin->fMCSecondMoment += nZZPlus1*perElemPerEkin->fMCSecondMoment;
//
// 2./b./(ii) Go for the rejection funtion part
// I. loop over delta values
for (G4int idel=0; idel<gNumDelta; ++idel) {
DataPerDelta *perMatPerDelta = perMatPerEkin->fDataPerDelta[idel];
DataPerDelta *perElemPerDelta = perElemPerEkin->fDataPerDelta[idel];
// I./a. loop over angles (i.e. the \sin(0.5\theta) values) and add the rejection function
for (G4int iang=0; iang<gNumAngle; ++iang) {
perMatPerDelta->fRejFuntion[iang] += nZZPlus1*perElemPerDelta->fRejFuntion[iang];
}
// I./b. get the last bin spline parameters and add them (a+bx+cx^2+dx^3)
perMatPerDelta->fSA += nZZPlus1*perElemPerDelta->fSA;
perMatPerDelta->fSB += nZZPlus1*perElemPerDelta->fSB;
perMatPerDelta->fSC += nZZPlus1*perElemPerDelta->fSC;
perMatPerDelta->fSD += nZZPlus1*perElemPerDelta->fSD;
}
//
// 2./b./(iii) When the last element has been added:
if (ielem==numElems-1) {
//
// 1. the remaining part of the sreening correction and divide the corrected screening par. with Moliere's one:
// (Moliere screening parameter = moliereXc2/(4(pc)^2 moliereBc) )
G4double dumScr = G4Exp(perMatPerEkin->fMCScreening/zs);
perMatPerEkin->fMCScreening = constFactor*dumScr*moliereBc/moliereXc2;
//
// 2. the remaining part of the first moment correction and divide by the one computed by using the corrected
// screening parameter (= (mc^2)^\alpha^2/(4(pc)^2C_{TF}^2) dumScr
G4double scrCorTed = constFactor*dumScr/(4.*pt2);
G4double dum0 = G4Log(1.+1./scrCorTed);
perMatPerEkin->fMCFirstMoment = perMatPerEkin->fMCFirstMoment/(zs*(dum0-1./(1.+scrCorTed)));
//
// 3. the remaining part of the second moment correction and divide by the one computed by using the corrected
// screening parameter
G4double G2PerG1 = 3.*(1.+scrCorTed)*((1.+2.*scrCorTed)*dum0-2.)/((1.+scrCorTed)*dum0-1.);
perMatPerEkin->fMCSecondMoment = perMatPerEkin->fMCSecondMoment/(zs*G2PerG1);
//
// 4. scale the maximum of the rejection function to unity and correct the last bin spline parameters as well
// I. loop over delta values
for (G4int idel=0; idel<gNumDelta; ++idel) {
DataPerDelta *perMatPerDelta = perMatPerEkin->fDataPerDelta[idel];
G4double maxVal = -1.;
// II. llop over angles
for (G4int iang=0; iang<gNumAngle; ++iang) {
if (perMatPerDelta->fRejFuntion[iang]>maxVal)
maxVal = perMatPerDelta->fRejFuntion[iang];
}
for (G4int iang=0; iang<gNumAngle; ++iang) {
perMatPerDelta->fRejFuntion[iang] /=maxVal;
}
perMatPerDelta->fSA /= maxVal;
perMatPerDelta->fSB /= maxVal;
perMatPerDelta->fSC /= maxVal;
perMatPerDelta->fSD /= maxVal;
}
}
}
}
}
void G4GSMottCorrection::AllocateDataPerMaterial(DataPerMaterial *data) {
data->fDataPerEkin = new DataPerEkin*[gNumEkin]();
for (G4int iek=0; iek<gNumEkin; ++iek) {
auto perEkin = new DataPerEkin();
perEkin->fDataPerDelta = new DataPerDelta*[gNumDelta]();
for (G4int idel=0; idel<gNumDelta; ++idel) {
auto perDelta = new DataPerDelta();
perDelta->fRejFuntion = new double[gNumAngle]();
perEkin->fDataPerDelta[idel] = perDelta;
}
data->fDataPerEkin[iek] = perEkin;
}
}
void G4GSMottCorrection::DeAllocateDataPerMaterial(DataPerMaterial *data) {
for (G4int iek=0; iek<gNumEkin; ++iek) {
DataPerEkin *perEkin = data->fDataPerEkin[iek]; //new DataPerEkin();
for (G4int idel=0; idel<gNumDelta; ++idel) {
DataPerDelta *perDelta = perEkin->fDataPerDelta[idel];
delete [] perDelta->fRejFuntion;
delete perDelta;
}
delete [] perEkin->fDataPerDelta;
delete perEkin;
}
delete [] data->fDataPerEkin;
}
void G4GSMottCorrection::ClearMCDataPerElement() {
for (std::size_t i=0; i<fMCDataPerElement.size(); ++i) {
if (fMCDataPerElement[i]) {
DeAllocateDataPerMaterial(fMCDataPerElement[i]);
delete fMCDataPerElement[i];
}
}
fMCDataPerElement.clear();
}
void G4GSMottCorrection::ClearMCDataPerMaterial() {
for (std::size_t i=0; i<fMCDataPerMaterial.size(); ++i) {
if (fMCDataPerMaterial[i]) {
DeAllocateDataPerMaterial(fMCDataPerMaterial[i]);
delete fMCDataPerMaterial[i];
}
}
fMCDataPerMaterial.clear();
}
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