// // ******************************************************************** // * License and Disclaimer * // * * // * The Geant4 software is copyright of the Copyright Holders of * // * the Geant4 Collaboration. It is provided under the terms and * // * conditions of the Geant4 Software License, included in the file * // * LICENSE and available at http://cern.ch/geant4/license . These * // * include a list of copyright holders. * // * * // * Neither the authors of this software system, nor their employing * // * institutes,nor the agencies providing financial support for this * // * work make any representation or warranty, express or implied, * // * regarding this software system or assume any liability for its * // * use. Please see the license in the file LICENSE and URL above * // * for the full disclaimer and the limitation of liability. * // * * // * This code implementation is the result of the scientific and * // * technical work of the GEANT4 collaboration. * // * By using, copying, modifying or distributing the software (or * // * any work based on the software) you agree to acknowledge its * // * use in resulting scientific publications, and indicate your * // * acceptance of all terms of the Geant4 Software license. * // ******************************************************************** // //$Id: G4AnalyticalEcpssrLiCrossSection.cc,v 1.4 2010/11/22 17:25:45 mantero Exp $ // GEANT4 tag $Name: geant4-09-04-ref-00 $ #include "globals.hh" #include "G4AnalyticalEcpssrLiCrossSection.hh" #include "G4AtomicTransitionManager.hh" #include "G4NistManager.hh" #include "G4Proton.hh" #include "G4Alpha.hh" #include #include #include "G4LinLogInterpolation.hh" //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... G4AnalyticalEcpssrLiCrossSection::G4AnalyticalEcpssrLiCrossSection() { // Storing FLi data needed for 0.2 to 3.0 velocities region char *path = getenv("G4LEDATA"); if (!path) G4Exception("G4ecpssrLCrossSection::G4AnalyticalEcpssrLiCrossSection() G4LEDDATA environment variable not set"); std::ostringstream fileName1; std::ostringstream fileName2; fileName1 << path << "/pixe/uf/FL1.dat"; fileName2 << path << "/pixe/uf/FL2.dat"; // Reading of FL1.dat std::ifstream FL1(fileName1.str().c_str()); if (!FL1) G4Exception("G4ecpssrLCrossSection::G4AnalyticalEcpssrLiCrossSection() error opening FL1 data file"); dummyVec1.push_back(0.); while(!FL1.eof()) { double x1; double y1; FL1>>x1>>y1; // Mandatory vector initialization if (x1 != dummyVec1.back()) { dummyVec1.push_back(x1); aVecMap1[x1].push_back(-1.); } FL1>>FL1Data[x1][y1]; if (y1 != aVecMap1[x1].back()) aVecMap1[x1].push_back(y1); } // Reading of FL2.dat std::ifstream FL2(fileName2.str().c_str()); if (!FL2) G4Exception("G4ecpssrLCrossSection::G4AnalyticalEcpssrLiCrossSection() error opening FL2 data file"); dummyVec2.push_back(0.); while(!FL2.eof()) { double x2; double y2; FL2>>x2>>y2; // Mandatory vector initialization if (x2 != dummyVec2.back()) { dummyVec2.push_back(x2); aVecMap2[x2].push_back(-1.); } FL2>>FL2Data[x2][y2]; if (y2 != aVecMap2[x2].back()) aVecMap2[x2].push_back(y2); } // Verbose level verboseLevel=0; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... G4AnalyticalEcpssrLiCrossSection::~G4AnalyticalEcpssrLiCrossSection() {} //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... G4double G4AnalyticalEcpssrLiCrossSection::ExpIntFunction(G4int n,G4double x) { // this function allows fast evaluation of the n order exponential integral function En(x) G4int i; G4int ii; G4int nm1; G4double a; G4double b; G4double c; G4double d; G4double del; G4double fact; G4double h; G4double psi; G4double ans = 0; const G4double euler= 0.5772156649; const G4int maxit= 100; const G4double fpmin = 1.0e-30; const G4double eps = 1.0e-7; nm1=n-1; if (n<0 || x<0.0 || (x==0.0 && (n==0 || n==1))) G4cout << "bad arguments in ExpIntFunction" << G4endl; else { if (n==0) ans=std::exp(-x)/x; else { if (x==0.0) ans=1.0/nm1; else { if (x > 1.0) { b=x+n; c=1.0/fpmin; d=1.0/b; h=d; for (i=1;i<=maxit;i++) { a=-i*(nm1+i); b +=2.0; d=1.0/(a*d+b); c=b+a/c; del=c*d; h *=del; if (std::fabs(del-1.0) < eps) { ans=h*std::exp(-x); return ans; } } } else { ans = (nm1!=0 ? 1.0/nm1 : -std::log(x)-euler); fact=1.0; for (i=1;i<=maxit;i++) { fact *=-x/i; if (i !=nm1) del = -fact/(i-nm1); else { psi = -euler; for (ii=1;ii<=nm1;ii++) psi +=1.0/ii; del=fact*(-std::log(x)+psi); } ans += del; if (std::fabs(del) < std::fabs(ans)*eps) return ans; } } } } } return ans; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... G4double G4AnalyticalEcpssrLiCrossSection::CalculateL1CrossSection(G4int zTarget,G4double massIncident, G4double energyIncident) { //this L1-CrossSection calculation method is done according to Werner Brandt and Grzegorz Lapicki, Phys.Rev.A20 N2 (1979), //and using data tables of O. Benka et al. At.Data Nucl.Data Tables Vol.22 No.3 (1978). G4NistManager* massManager = G4NistManager::Instance(); G4AtomicTransitionManager* transitionManager = G4AtomicTransitionManager::Instance(); G4double zIncident = 0; G4Proton* aProtone = G4Proton::Proton(); G4Alpha* aAlpha = G4Alpha::Alpha(); if (massIncident == aProtone->GetPDGMass() ) zIncident = (aProtone->GetPDGCharge())/eplus; else { if (massIncident == aAlpha->GetPDGMass()) zIncident = (aAlpha->GetPDGCharge())/eplus; else { G4cout << "*** WARNING in G4AnalyticalEcpssrLiCrossSection::CalculateL1CrossSection : Proton or Alpha incident particles only. " << G4endl; G4cout << massIncident << ", " << aAlpha->GetPDGMass() << " (alpha)" << aProtone->GetPDGMass() << " (proton)" << G4endl; return 0; } } G4double l1BindingEnergy = transitionManager->Shell(zTarget,1)->BindingEnergy(); //Observed binding energy of L1-subshell G4double massTarget = (massManager->GetAtomicMassAmu(zTarget))*amu_c2; G4double systemMass =((massIncident*massTarget)/(massIncident+massTarget))/electron_mass_c2; //Mass of the system (projectile, target) const G4double zlshell= 4.15; G4double screenedzTarget = zTarget-zlshell; //Effective nuclear charge as seen by electrons in L1-sub shell const G4double rydbergMeV= 13.6056923e-6; const G4double nl= 2.; G4double tetal1 = (l1BindingEnergy*nl*nl)/((screenedzTarget*screenedzTarget)*rydbergMeV); //Screening parameter if (verboseLevel>0) G4cout << " tetal1=" << tetal1<< G4endl; G4double reducedEnergy = (energyIncident*electron_mass_c2)/(massIncident*rydbergMeV*screenedzTarget*screenedzTarget); const G4double bohrPow2Barn=(Bohr_radius*Bohr_radius)/barn ; //Bohr radius of hydrogen G4double sigma0 = 8.*pi*(zIncident*zIncident)*bohrPow2Barn*std::pow(screenedzTarget,-4.); G4double velocityl1 = CalculateVelocity(1, zTarget, massIncident, energyIncident); // Scaled velocity if (verboseLevel>0) G4cout << " velocityl1=" << velocityl1<< G4endl; const G4double l1AnalyticalApproximation= 1.5; G4double x1 =(nl*l1AnalyticalApproximation)/velocityl1; if (verboseLevel>0) G4cout << " x1=" << x1<< G4endl; G4double electrIonizationEnergyl1=0.; if ( x1<=0.035) electrIonizationEnergyl1= 0.75*pi*(std::log(1./(x1*x1))-1.); else { if ( x1<=3.) electrIonizationEnergyl1 =std::exp(-2.*x1)/(0.031+(0.213*std::pow(x1,0.5))+(0.005*x1)-(0.069*std::pow(x1,3./2.))+(0.324*x1*x1)); else {if ( x1<=11.) electrIonizationEnergyl1 =2.*std::exp(-2.*x1)/std::pow(x1,1.6);} } G4double hFunctionl1 =(electrIonizationEnergyl1*2.*nl)/(tetal1*std::pow(velocityl1,3)); //takes into account the polarization effect if (verboseLevel>0) G4cout << " hFunctionl1=" << hFunctionl1<< G4endl; G4double gFunctionl1 = (1.+(9.*velocityl1)+(31.*velocityl1*velocityl1)+(49.*std::pow(velocityl1,3.))+(162.*std::pow(velocityl1,4.))+(63.*std::pow(velocityl1,5.))+(18.*std::pow(velocityl1,6.))+(1.97*std::pow(velocityl1,7.)))/std::pow(1.+velocityl1,9.);//takes into account the reduced binding effect if (verboseLevel>0) G4cout << " gFunctionl1=" << gFunctionl1<< G4endl; G4double sigmaPSS_l1 = 1.+(((2.*zIncident)/(screenedzTarget*tetal1))*(gFunctionl1-hFunctionl1)); //Binding-polarization factor if (verboseLevel>0) G4cout << "sigmaPSS_l1 =" << sigmaPSS_l1<< G4endl; const G4double cNaturalUnit= 137.; G4double yl1Formula=0.4*(screenedzTarget/cNaturalUnit)*(screenedzTarget/cNaturalUnit)/(nl*velocityl1/sigmaPSS_l1); G4double l1relativityCorrection = std::pow((1.+(1.1*yl1Formula*yl1Formula)),0.5)+yl1Formula; // Relativistic correction parameter //G4double reducedVelocity_l1 = velocityl1*std::pow(l1relativityCorrection,0.5); //Reduced velocity parameter G4double L1etaOverTheta2; G4double universalFunction_l1 = 0.; G4double sigmaPSSR_l1; if ( velocityl1 <5. ) { L1etaOverTheta2 =(reducedEnergy* l1relativityCorrection)/((tetal1*sigmaPSS_l1)*(tetal1*sigmaPSS_l1)); if ( ((tetal1*sigmaPSS_l1) >=0.2) && ((tetal1*sigmaPSS_l1) <=2.6670) && (L1etaOverTheta2>=0.1e-3) && (L1etaOverTheta2<=0.866e2) ) universalFunction_l1 = FunctionFL1((tetal1*sigmaPSS_l1),L1etaOverTheta2); if (verboseLevel>0) G4cout << "at low velocity range, universalFunction_l1 =" << universalFunction_l1 << G4endl; sigmaPSSR_l1 = (sigma0/(tetal1*sigmaPSS_l1))*universalFunction_l1;// Plane-wave Born -Aproximation L1-subshell ionisation Cross Section if (verboseLevel>0) G4cout << " at low velocity range, sigma PWBA L1 CS = " << sigmaPSSR_l1<< G4endl; } else { L1etaOverTheta2 = reducedEnergy/(tetal1*tetal1); if ( (tetal1 >=0.2) && (tetal1 <=2.6670) && (L1etaOverTheta2>=0.1e-3) && (L1etaOverTheta2<=0.866e2) ) universalFunction_l1 = FunctionFL1(tetal1,L1etaOverTheta2); if (verboseLevel>0) G4cout << "at medium and high velocity range, universalFunction_l1 =" << universalFunction_l1 << G4endl; sigmaPSSR_l1 = (sigma0/tetal1)*universalFunction_l1;// Plane-wave Born -Aproximation L1-subshell ionisation Cross Section if (verboseLevel>0) G4cout << " sigma PWBA L1 CS at medium and high velocity range = " << sigmaPSSR_l1<< G4endl; } G4double pssDeltal1 = (4./(systemMass *sigmaPSS_l1*tetal1))*(sigmaPSS_l1/velocityl1)*(sigmaPSS_l1/velocityl1); if (verboseLevel>0) G4cout << " pssDeltal1=" << pssDeltal1<< G4endl; G4double energyLossl1 = std::pow(1-pssDeltal1,0.5); if (verboseLevel>0) G4cout << " energyLossl1=" << energyLossl1<< G4endl; G4double coulombDeflectionl1 = (8.*pi*zIncident/systemMass)*std::pow(tetal1*sigmaPSS_l1,-2.)*std::pow(velocityl1/sigmaPSS_l1,-3.)*(zTarget/screenedzTarget); G4double cParameterl1 =2.* coulombDeflectionl1/(energyLossl1*(energyLossl1+1.)); G4double coulombDeflectionFunction_l1 = 9.*ExpIntFunction(10,cParameterl1); //Coulomb-deflection effect correction if (verboseLevel>0) G4cout << " coulombDeflectionFunction_l1 =" << coulombDeflectionFunction_l1 << G4endl; G4double crossSection_L1 = coulombDeflectionFunction_l1 * sigmaPSSR_l1; //ECPSSR L1 -subshell cross section is estimated at perturbed-stationnairy-state(PSS) //and reduced by the energy-loss(E),the Coulomb deflection(C),and the relativity(R) effects if (verboseLevel>0) G4cout << " crossSection_L1 =" << crossSection_L1 << G4endl; if (crossSection_L1 >= 0) { return crossSection_L1 * barn; } else {return 0;} } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... G4double G4AnalyticalEcpssrLiCrossSection::CalculateL2CrossSection(G4int zTarget,G4double massIncident, G4double energyIncident) { // this L2-CrossSection calculation method is done according to Werner Brandt and Grzegorz Lapicki, Phys.Rev.A20 N2 (1979), // and using data tables of O. Benka et al. At.Data Nucl.Data Tables Vol.22 No.3 (1978). G4NistManager* massManager = G4NistManager::Instance(); G4AtomicTransitionManager* transitionManager = G4AtomicTransitionManager::Instance(); G4double zIncident = 0; G4Proton* aProtone = G4Proton::Proton(); G4Alpha* aAlpha = G4Alpha::Alpha(); if (massIncident == aProtone->GetPDGMass() ) zIncident = (aProtone->GetPDGCharge())/eplus; else { if (massIncident == aAlpha->GetPDGMass()) zIncident = (aAlpha->GetPDGCharge())/eplus; else { G4cout << "*** WARNING in G4AnalyticalEcpssrLiCrossSection::CalculateL2CrossSection : Proton or Alpha incident particles only. " << G4endl; G4cout << massIncident << ", " << aAlpha->GetPDGMass() << " (alpha)" << aProtone->GetPDGMass() << " (proton)" << G4endl; return 0; } } G4double l2BindingEnergy = transitionManager->Shell(zTarget,2)->BindingEnergy(); //Observed binding energy of L2-subshell G4double massTarget = (massManager->GetAtomicMassAmu(zTarget))*amu_c2; G4double systemMass =((massIncident*massTarget)/(massIncident+massTarget))/electron_mass_c2; //Mass of the system (projectile, target) const G4double zlshell= 4.15; G4double screenedzTarget = zTarget-zlshell; //Effective nuclear charge as seen by electrons in L2-subshell const G4double rydbergMeV= 13.6056923e-6; const G4double nl= 2.; G4double tetal2 = (l2BindingEnergy*nl*nl)/((screenedzTarget*screenedzTarget)*rydbergMeV); //Screening parameter if (verboseLevel>0) G4cout << " tetal2=" << tetal2<< G4endl; G4double reducedEnergy = (energyIncident*electron_mass_c2)/(massIncident*rydbergMeV*screenedzTarget*screenedzTarget); const G4double bohrPow2Barn=(Bohr_radius*Bohr_radius)/barn ; //Bohr radius of hydrogen G4double sigma0 = 8.*pi*(zIncident*zIncident)*bohrPow2Barn*std::pow(screenedzTarget,-4.); G4double velocityl2 = CalculateVelocity(2, zTarget, massIncident, energyIncident); // Scaled velocity if (verboseLevel>0) G4cout << " velocityl2=" << velocityl2<< G4endl; const G4double l23AnalyticalApproximation= 1.25; G4double x2 = (nl*l23AnalyticalApproximation)/velocityl2; if (verboseLevel>0) G4cout << " x2=" << x2<< G4endl; G4double electrIonizationEnergyl2=0.; if ( x2<=0.035) electrIonizationEnergyl2= 0.75*pi*(std::log(1./(x2*x2))-1.); else { if ( x2<=3.) electrIonizationEnergyl2 =std::exp(-2.*x2)/(0.031+(0.210*std::pow(x2,0.5))+(0.005*x2)-(0.069*std::pow(x2,3./2.))+(0.324*x2*x2)); else {if ( x2<=11.) electrIonizationEnergyl2 =2.*std::exp(-2.*x2)/std::pow(x2,1.6); } } G4double hFunctionl2 =(electrIonizationEnergyl2*2.*nl)/(tetal2*std::pow(velocityl2,3)); //takes into account the polarization effect if (verboseLevel>0) G4cout << " hFunctionl2=" << hFunctionl2<< G4endl; G4double gFunctionl2 = (1.+(10.*velocityl2)+(45.*velocityl2*velocityl2)+(102.*std::pow(velocityl2,3.))+(331.*std::pow(velocityl2,4.))+(6.7*std::pow(velocityl2,5.))+(58.*std::pow(velocityl2,6.))+(7.8*std::pow(velocityl2,7.))+ (0.888*std::pow(velocityl2,8.)) )/std::pow(1.+velocityl2,10.); //takes into account the reduced binding effect if (verboseLevel>0) G4cout << " gFunctionl2=" << gFunctionl2<< G4endl; G4double sigmaPSS_l2 = 1.+(((2.*zIncident)/(screenedzTarget*tetal2))*(gFunctionl2-hFunctionl2)); //Binding-polarization factor if (verboseLevel>0) G4cout << " sigmaPSS_l2=" << sigmaPSS_l2<< G4endl; const G4double cNaturalUnit= 137.; G4double yl2Formula=0.15*(screenedzTarget/cNaturalUnit)*(screenedzTarget/cNaturalUnit)/(velocityl2/sigmaPSS_l2); G4double l2relativityCorrection = std::pow((1.+(1.1*yl2Formula*yl2Formula)),0.5)+yl2Formula; // Relativistic correction parameter G4double L2etaOverTheta2; G4double universalFunction_l2 = 0.; G4double sigmaPSSR_l2 ; if ( velocityl2 < 5. ) { L2etaOverTheta2 = (reducedEnergy*l2relativityCorrection)/((sigmaPSS_l2*tetal2)*(sigmaPSS_l2*tetal2)); if ( (tetal2*sigmaPSS_l2>=0.2) && (tetal2*sigmaPSS_l2<=2.6670) && (L2etaOverTheta2>=0.1e-3) && (L2etaOverTheta2<=0.866e2) ) universalFunction_l2 = FunctionFL2((tetal2*sigmaPSS_l2),L2etaOverTheta2); sigmaPSSR_l2 = (sigma0/(tetal2*sigmaPSS_l2))*universalFunction_l2; if (verboseLevel>0) G4cout << " sigma PWBA L2 CS at low velocity range = " << sigmaPSSR_l2<< G4endl; } else { L2etaOverTheta2 = reducedEnergy /(tetal2*tetal2); if ( (tetal2>=0.2) && (tetal2<=2.6670) && (L2etaOverTheta2>=0.1e-3) && (L2etaOverTheta2<=0.866e2) ) universalFunction_l2 = FunctionFL2((tetal2),L2etaOverTheta2); sigmaPSSR_l2 = (sigma0/tetal2)*universalFunction_l2; if (verboseLevel>0) G4cout << " sigma PWBA L2 CS at medium and high velocity range = " << sigmaPSSR_l2<< G4endl; } G4double pssDeltal2 = (4./(systemMass*sigmaPSS_l2*tetal2))*(sigmaPSS_l2/velocityl2)*(sigmaPSS_l2/velocityl2); G4double energyLossl2 = std::pow(1-pssDeltal2,0.5); if (verboseLevel>0) G4cout << " energyLossl2=" << energyLossl2<< G4endl; G4double coulombDeflectionl2 =(8.*pi*zIncident/systemMass)*std::pow(tetal2*sigmaPSS_l2,-2.)*std::pow(velocityl2/sigmaPSS_l2,-3.)*(zTarget/screenedzTarget); G4double cParameterl2 = 2.*coulombDeflectionl2/(energyLossl2*(energyLossl2+1.)); G4double coulombDeflectionFunction_l2 = 11.*ExpIntFunction(12,cParameterl2); //Coulomb-deflection effect correction if (verboseLevel>0) G4cout << " coulombDeflectionFunction_l2 =" << coulombDeflectionFunction_l2 << G4endl; G4double crossSection_L2 = coulombDeflectionFunction_l2 * sigmaPSSR_l2; //ECPSSR L2 -subshell cross section is estimated at perturbed-stationnairy-state(PSS) //and reduced by the energy-loss(E),the Coulomb deflection(C),and the relativity(R) effects if (verboseLevel>0) G4cout << " crossSection_L2 =" << crossSection_L2 << G4endl; if (crossSection_L2 >= 0) { return crossSection_L2 * barn; } else {return 0;} } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... G4double G4AnalyticalEcpssrLiCrossSection::CalculateL3CrossSection(G4int zTarget,G4double massIncident, G4double energyIncident) { //this L3-CrossSection calculation method is done according to Werner Brandt and Grzegorz Lapicki, Phys.Rev.A20 N2 (1979), //and using data tables of O. Benka et al. At.Data Nucl.Data Tables Vol.22 No.3 (1978). G4NistManager* massManager = G4NistManager::Instance(); G4AtomicTransitionManager* transitionManager = G4AtomicTransitionManager::Instance(); G4double zIncident = 0; G4Proton* aProtone = G4Proton::Proton(); G4Alpha* aAlpha = G4Alpha::Alpha(); if (massIncident == aProtone->GetPDGMass() ) zIncident = (aProtone->GetPDGCharge())/eplus; else { if (massIncident == aAlpha->GetPDGMass()) zIncident = (aAlpha->GetPDGCharge())/eplus; else { G4cout << "*** WARNING in G4AnalyticalEcpssrLiCrossSection::CalculateL3CrossSection : Proton or Alpha incident particles only. " << G4endl; G4cout << massIncident << ", " << aAlpha->GetPDGMass() << " (alpha)" << aProtone->GetPDGMass() << " (proton)" << G4endl; return 0; } } G4double l3BindingEnergy = transitionManager->Shell(zTarget,3)->BindingEnergy(); G4double massTarget = (massManager->GetAtomicMassAmu(zTarget))*amu_c2; G4double systemMass =((massIncident*massTarget)/(massIncident+massTarget))/electron_mass_c2;//Mass of the system (projectile, target) const G4double zlshell= 4.15; G4double screenedzTarget = zTarget-zlshell;//Effective nuclear charge as seen by electrons in L3-subshell const G4double rydbergMeV= 13.6056923e-6; const G4double nl= 2.; G4double tetal3 = (l3BindingEnergy*nl*nl)/((screenedzTarget*screenedzTarget)*rydbergMeV);//Screening parameter if (verboseLevel>0) G4cout << " tetal3=" << tetal3<< G4endl; G4double reducedEnergy = (energyIncident*electron_mass_c2)/(massIncident*rydbergMeV*screenedzTarget*screenedzTarget); const G4double bohrPow2Barn=(Bohr_radius*Bohr_radius)/barn ;//Bohr radius of hydrogen G4double sigma0 = 8.*pi*(zIncident*zIncident)*bohrPow2Barn*std::pow(screenedzTarget,-4.); G4double velocityl3 = CalculateVelocity(3, zTarget, massIncident, energyIncident);// Scaled velocity if (verboseLevel>0) G4cout << " velocityl3=" << velocityl3<< G4endl; const G4double l23AnalyticalApproximation= 1.25; G4double x3 = (nl*l23AnalyticalApproximation)/velocityl3; if (verboseLevel>0) G4cout << " x3=" << x3<< G4endl; G4double electrIonizationEnergyl3=0.; if ( x3<=0.035) electrIonizationEnergyl3= 0.75*pi*(std::log(1./(x3*x3))-1.); else { if ( x3<=3.) electrIonizationEnergyl3 =std::exp(-2.*x3)/(0.031+(0.210*std::pow(x3,0.5))+(0.005*x3)-(0.069*std::pow(x3,3./2.))+(0.324*x3*x3)); else { if ( x3<=11.) electrIonizationEnergyl3 =2.*std::exp(-2.*x3)/std::pow(x3,1.6);} } G4double hFunctionl3 =(electrIonizationEnergyl3*2.*nl)/(tetal3*std::pow(velocityl3,3));//takes into account the polarization effect if (verboseLevel>0) G4cout << " hFunctionl3=" << hFunctionl3<< G4endl; G4double gFunctionl3 = (1.+(10.*velocityl3)+(45.*velocityl3*velocityl3)+(102.*std::pow(velocityl3,3.))+(331.*std::pow(velocityl3,4.))+(6.7*std::pow(velocityl3,5.))+(58.*std::pow(velocityl3,6.))+(7.8*std::pow(velocityl3,7.))+ (0.888*std::pow(velocityl3,8.)) )/std::pow(1.+velocityl3,10.); //takes into account the reduced binding effect if (verboseLevel>0) G4cout << " gFunctionl3=" << gFunctionl3<< G4endl; G4double sigmaPSS_l3 = 1.+(((2.*zIncident)/(screenedzTarget*tetal3))*(gFunctionl3-hFunctionl3));//Binding-polarization factor if (verboseLevel>0) G4cout << "sigmaPSS_l3 =" << sigmaPSS_l3<< G4endl; const G4double cNaturalUnit= 137.; G4double yl3Formula=0.15*(screenedzTarget/cNaturalUnit)*(screenedzTarget/cNaturalUnit)/(velocityl3/sigmaPSS_l3); G4double l3relativityCorrection = std::pow((1.+(1.1*yl3Formula*yl3Formula)),0.5)+yl3Formula; // Relativistic correction parameter G4double L3etaOverTheta2; G4double universalFunction_l3 = 0.; G4double sigmaPSSR_l3; if ( velocityl3 < 5. ) { L3etaOverTheta2 = (reducedEnergy* l3relativityCorrection)/((sigmaPSS_l3*tetal3)*(sigmaPSS_l3*tetal3)); if ( (tetal3*sigmaPSS_l3>=0.2) && (tetal3*sigmaPSS_l3<=2.6670) && (L3etaOverTheta2>=0.1e-3) && (L3etaOverTheta2<=0.866e2) ) universalFunction_l3 = 2.*FunctionFL2((tetal3*sigmaPSS_l3), L3etaOverTheta2 ); sigmaPSSR_l3 = (sigma0/(tetal3*sigmaPSS_l3))*universalFunction_l3; if (verboseLevel>0) G4cout << " sigma PWBA L3 CS at low velocity range = " << sigmaPSSR_l3<< G4endl; } else { L3etaOverTheta2 = reducedEnergy/(tetal3*tetal3); if ( (tetal3>=0.2) && (tetal3<=2.6670) && (L3etaOverTheta2>=0.1e-3) && (L3etaOverTheta2<=0.866e2) ) universalFunction_l3 = 2.*FunctionFL2(tetal3, L3etaOverTheta2 ); sigmaPSSR_l3 = (sigma0/tetal3)*universalFunction_l3; if (verboseLevel>0) G4cout << " sigma PWBA L3 CS at medium and high velocity range = " << sigmaPSSR_l3<< G4endl; } G4double pssDeltal3 = (4./(systemMass*sigmaPSS_l3*tetal3))*(sigmaPSS_l3/velocityl3)*(sigmaPSS_l3/velocityl3); if (verboseLevel>0) G4cout << " pssDeltal3=" << pssDeltal3<< G4endl; G4double energyLossl3 = std::pow(1-pssDeltal3,0.5); if (verboseLevel>0) G4cout << " energyLossl3=" << energyLossl3<< G4endl; G4double coulombDeflectionl3 = (8.*pi*zIncident/systemMass)*std::pow(tetal3*sigmaPSS_l3,-2.)*std::pow(velocityl3/sigmaPSS_l3,-3.)*(zTarget/screenedzTarget); G4double cParameterl3 = 2.*coulombDeflectionl3/(energyLossl3*(energyLossl3+1.)); G4double coulombDeflectionFunction_l3 = 11.*ExpIntFunction(12,cParameterl3);//Coulomb-deflection effect correction if (verboseLevel>0) G4cout << " coulombDeflectionFunction_l3 =" << coulombDeflectionFunction_l3 << G4endl; G4double crossSection_L3 = coulombDeflectionFunction_l3 * sigmaPSSR_l3; //ECPSSR L3 -subshell cross section is estimated at perturbed-stationnairy-state(PSS) //and reduced by the energy-loss(E),the Coulomb deflection(C),and the relativity(R) effects if (verboseLevel>0) G4cout << " crossSection_L3 =" << crossSection_L3 << G4endl; if (crossSection_L3 >= 0) { return crossSection_L3 * barn; } else {return 0;} } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... G4double G4AnalyticalEcpssrLiCrossSection::CalculateVelocity(G4int subShell, G4int zTarget, G4double massIncident, G4double energyIncident) { G4AtomicTransitionManager* transitionManager = G4AtomicTransitionManager::Instance(); G4double liBindingEnergy = transitionManager->Shell(zTarget,subShell)->BindingEnergy(); G4Proton* aProtone = G4Proton::Proton(); G4Alpha* aAlpha = G4Alpha::Alpha(); if (!((massIncident == aProtone->GetPDGMass()) || (massIncident == aAlpha->GetPDGMass()))) { G4cout << "*** WARNING in G4AnalyticalEcpssrLiCrossSection::CalculateVelocity : Proton or Alpha incident particles only. " << G4endl; G4cout << massIncident << ", " << aAlpha->GetPDGMass() << " (alpha)" << aProtone->GetPDGMass() << " (proton)" << G4endl; return 0; } const G4double zlshell= 4.15; G4double screenedzTarget = zTarget- zlshell; const G4double rydbergMeV= 13.6056923e-6; const G4double nl= 2.; G4double tetali = (liBindingEnergy*nl*nl)/(screenedzTarget*screenedzTarget*rydbergMeV); G4double reducedEnergy = (energyIncident*electron_mass_c2)/(massIncident*rydbergMeV*screenedzTarget*screenedzTarget); G4double velocity = 2.*nl*std::pow(reducedEnergy,0.5)/tetali; return velocity; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... G4double G4AnalyticalEcpssrLiCrossSection::FunctionFL1(G4double k, G4double theta) { G4double sigma = 0.; G4double valueT1 = 0; G4double valueT2 = 0; G4double valueE21 = 0; G4double valueE22 = 0; G4double valueE12 = 0; G4double valueE11 = 0; G4double xs11 = 0; G4double xs12 = 0; G4double xs21 = 0; G4double xs22 = 0; // PROTECTION TO ALLOW INTERPOLATION AT MINIMUM AND MAXIMUM Eta/Theta2 values if ( theta==8.66e-4 || theta==8.66e-3 || theta==8.66e-2 || theta==8.66e-1 || theta==8.66e+00 || theta==8.66e+01 ) theta=theta-1e-12; if ( theta==1.e-4 || theta==1.e-3 || theta==1.e-2 || theta==1.e-1 || theta==1.e+00 || theta==1.e+01 ) theta=theta+1e-12; // END PROTECTION std::vector::iterator t2 = std::upper_bound(dummyVec1.begin(),dummyVec1.end(), k); std::vector::iterator t1 = t2-1; std::vector::iterator e12 = std::upper_bound(aVecMap1[(*t1)].begin(),aVecMap1[(*t1)].end(), theta); std::vector::iterator e11 = e12-1; std::vector::iterator e22 = std::upper_bound(aVecMap1[(*t2)].begin(),aVecMap1[(*t2)].end(), theta); std::vector::iterator e21 = e22-1; valueT1 =*t1; valueT2 =*t2; valueE21 =*e21; valueE22 =*e22; valueE12 =*e12; valueE11 =*e11; xs11 = FL1Data[valueT1][valueE11]; xs12 = FL1Data[valueT1][valueE12]; xs21 = FL1Data[valueT2][valueE21]; xs22 = FL1Data[valueT2][valueE22]; if (verboseLevel>0) G4cout << valueT1 << " " << valueT2 << " " << valueE11 << " " << valueE12 << " " << valueE21 << " " << valueE22 << " " << xs11 << " " << xs12 << " " << xs21 << " " << xs22 << " " << G4endl; G4double xsProduct = xs11 * xs12 * xs21 * xs22; if (xs11==0 || xs12==0 ||xs21==0 ||xs22==0) return (0.); if (xsProduct != 0.) { sigma = QuadInterpolator( valueE11, valueE12, valueE21, valueE22, xs11, xs12, xs21, xs22, valueT1, valueT2, k, theta ); } return sigma; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... G4double G4AnalyticalEcpssrLiCrossSection::FunctionFL2(G4double k, G4double theta) { G4double sigma = 0.; G4double valueT1 = 0; G4double valueT2 = 0; G4double valueE21 = 0; G4double valueE22 = 0; G4double valueE12 = 0; G4double valueE11 = 0; G4double xs11 = 0; G4double xs12 = 0; G4double xs21 = 0; G4double xs22 = 0; // PROTECTION TO ALLOW INTERPOLATION AT MINIMUM AND MAXIMUM Eta/Theta2 values if ( theta==8.66e-4 || theta==8.66e-3 || theta==8.66e-2 || theta==8.66e-1 || theta==8.66e+00 || theta==8.66e+01 ) theta=theta-1e-12; if ( theta==1.e-4 || theta==1.e-3 || theta==1.e-2 || theta==1.e-1 || theta==1.e+00 || theta==1.e+01 ) theta=theta+1e-12; // END PROTECTION std::vector::iterator t2 = std::upper_bound(dummyVec2.begin(),dummyVec2.end(), k); std::vector::iterator t1 = t2-1; std::vector::iterator e12 = std::upper_bound(aVecMap2[(*t1)].begin(),aVecMap2[(*t1)].end(), theta); std::vector::iterator e11 = e12-1; std::vector::iterator e22 = std::upper_bound(aVecMap2[(*t2)].begin(),aVecMap2[(*t2)].end(), theta); std::vector::iterator e21 = e22-1; valueT1 =*t1; valueT2 =*t2; valueE21 =*e21; valueE22 =*e22; valueE12 =*e12; valueE11 =*e11; xs11 = FL2Data[valueT1][valueE11]; xs12 = FL2Data[valueT1][valueE12]; xs21 = FL2Data[valueT2][valueE21]; xs22 = FL2Data[valueT2][valueE22]; if (verboseLevel>0) G4cout << valueT1 << " " << valueT2 << " " << valueE11 << " " << valueE12 << " " << valueE21 << " " << valueE22 << " " << xs11 << " " << xs12 << " " << xs21 << " " << xs22 << " " << G4endl; G4double xsProduct = xs11 * xs12 * xs21 * xs22; if (xs11==0 || xs12==0 ||xs21==0 ||xs22==0) return (0.); if (xsProduct != 0.) { sigma = QuadInterpolator( valueE11, valueE12, valueE21, valueE22, xs11, xs12, xs21, xs22, valueT1, valueT2, k, theta ); } return sigma; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... G4double G4AnalyticalEcpssrLiCrossSection::LinLinInterpolate(G4double e1, G4double e2, G4double e, G4double xs1, G4double xs2) { G4double value = xs1 + (xs2 - xs1)*(e - e1)/ (e2 - e1); return value; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... G4double G4AnalyticalEcpssrLiCrossSection::LinLogInterpolate(G4double e1, G4double e2, G4double e, G4double xs1, G4double xs2) { G4double d1 = std::log(xs1); G4double d2 = std::log(xs2); G4double value = std::exp(d1 + (d2 - d1)*(e - e1)/ (e2 - e1)); return value; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... G4double G4AnalyticalEcpssrLiCrossSection::LogLogInterpolate(G4double e1, G4double e2, G4double e, G4double xs1, G4double xs2) { G4double a = (std::log10(xs2)-std::log10(xs1)) / (std::log10(e2)-std::log10(e1)); G4double b = std::log10(xs2) - a*std::log10(e2); G4double sigma = a*std::log10(e) + b; G4double value = (std::pow(10.,sigma)); return value; } //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... G4double G4AnalyticalEcpssrLiCrossSection::QuadInterpolator(G4double e11, G4double e12, G4double e21, G4double e22, G4double xs11, G4double xs12, G4double xs21, G4double xs22, G4double t1, G4double t2, G4double t, G4double e) { // Log-Log G4double interpolatedvalue1 = LogLogInterpolate(e11, e12, e, xs11, xs12); G4double interpolatedvalue2 = LogLogInterpolate(e21, e22, e, xs21, xs22); G4double value = LogLogInterpolate(t1, t2, t, interpolatedvalue1, interpolatedvalue2); /* // Lin-Log G4double interpolatedvalue1 = LinLogInterpolate(e11, e12, e, xs11, xs12); G4double interpolatedvalue2 = LinLogInterpolate(e21, e22, e, xs21, xs22); G4double value = LinLogInterpolate(t1, t2, t, interpolatedvalue1, interpolatedvalue2); */ /* // Lin-Lin G4double interpolatedvalue1 = LinLinInterpolate(e11, e12, e, xs11, xs12); G4double interpolatedvalue2 = LinLinInterpolate(e21, e22, e, xs21, xs22); G4double value = LinLinInterpolate(t1, t2, t, interpolatedvalue1, interpolatedvalue2); */ return value; }