#include <LandauFP420.h>
Public Member Functions | |
LandauFP420 () | |
double | SampleFluctuations (const double momentum, const double mass, double &tmax, const double length, const double meanLoss) |
~LandauFP420 () | |
Private Attributes | |
double | alim |
double | chargeSquare |
double | e0 |
double | e1Fluct |
double | e1LogFluct |
double | e2Fluct |
double | e2LogFluct |
double | electronDensity |
double | f1Fluct |
double | f2Fluct |
double | ipotFluct |
double | ipotLogFluct |
double | minLoss |
double | minNumberInteractionsBohr |
int | nmaxCont1 |
int | nmaxCont2 |
double | particleMass |
double | problim |
double | rateFluct |
double | sumalim |
double | theBohrBeta2 |
Definition at line 52 of file LandauFP420.h.
LandauFP420::LandauFP420 | ( | ) |
Definition at line 66 of file LandauFP420.cc.
References chargeSquare, e0, e1Fluct, e1LogFluct, e2Fluct, e2LogFluct, electronDensity, f1Fluct, f2Fluct, ipotFluct, ipotLogFluct, create_public_lumi_plots::log, problim, rateFluct, and sumalim.
:minNumberInteractionsBohr(10.0), theBohrBeta2(50.0*keV/proton_mass_c2), minLoss(0.000001*eV), problim(0.01), alim(10.), nmaxCont1(4), nmaxCont2(16) { sumalim = -log(problim); chargeSquare = 1.; //Assume all particles have charge 1 // Taken from Geant4 printout, HARDWIRED for Silicon. ipotFluct = 0.0001736; //material->GetIonisation()->GetMeanExcitationEnergy(); electronDensity = 6.797E+20; // material->GetElectronDensity(); f1Fluct = 0.8571; // material->GetIonisation()->GetF1fluct(); f2Fluct = 0.1429; //material->GetIonisation()->GetF2fluct(); e1Fluct = 0.000116;// material->GetIonisation()->GetEnergy1fluct(); e2Fluct = 0.00196; //material->GetIonisation()->GetEnergy2fluct(); e1LogFluct = -9.063; //material->GetIonisation()->GetLogEnergy1fluct(); e2LogFluct = -6.235; //material->GetIonisation()->GetLogEnergy2fluct(); rateFluct = 0.4; //material->GetIonisation()->GetRateionexcfluct(); ipotLogFluct = -8.659; //material->GetIonisation()->GetLogMeanExcEnergy(); e0 = 1.E-5; //material->GetIonisation()->GetEnergy0fluct(); }
LandauFP420::~LandauFP420 | ( | ) |
Definition at line 93 of file LandauFP420.cc.
{}
double LandauFP420::SampleFluctuations | ( | const double | momentum, |
const double | mass, | ||
double & | tmax, | ||
const double | length, | ||
const double | meanLoss | ||
) |
Definition at line 99 of file LandauFP420.cc.
References alim, funct::C, chargeSquare, e0, e1Fluct, e1LogFluct, e2Fluct, e2LogFluct, electronDensity, f1Fluct, f2Fluct, i, ipotFluct, ipotLogFluct, gen::k, create_public_lumi_plots::log, max(), minLoss, minNumberInteractionsBohr, nmaxCont1, nmaxCont2, p1, p2, p3, particleMass, rateFluct, mathSSE::sqrt(), sumalim, w(), and w2.
{ // calculate actual loss from the mean loss // The model used to get the fluctuation is essentially the same // as in Glandz in Geant3. // shortcut for very very small loss if(meanLoss < minLoss) return meanLoss; //if(dp->GetDefinition() != particle) { particleMass = mass; // dp->GetMass(); //G4double q = dp->GetCharge(); //chargeSquare = q*q; //} //double gam = (dp->GetKineticEnergy())/particleMass + 1.0; //double gam2 = gam*gam; double gam2 = (momentum*momentum)/(particleMass*particleMass) + 1.0; double beta2 = 1.0 - 1.0/gam2; // Validity range for delta electron cross section double loss, siga; // Gaussian fluctuation if(meanLoss >= minNumberInteractionsBohr*tmax || tmax <= ipotFluct*minNumberInteractionsBohr) { siga = (1.0/beta2 - 0.5) * twopi_mc2_rcl2 * tmax * length * electronDensity * chargeSquare ; siga = sqrt(siga); do { //loss = G4RandGauss::shoot(meanLoss,siga); loss = CLHEP::RandGaussQ::shoot(meanLoss,siga); } while (loss < 0. || loss > 2.*meanLoss); return loss; } // Non Gaussian fluctuation double suma,w1,w2,C,lossc,w; double a1,a2,a3; int p1,p2,p3; int nb; double corrfac, na,alfa,rfac,namean,sa,alfa1,ea,sea; double dp3; w1 = tmax/ipotFluct; w2 = log(2.*electron_mass_c2*(gam2 - 1.0)); C = meanLoss*(1.-rateFluct)/(w2-ipotLogFluct-beta2); a1 = C*f1Fluct*(w2-e1LogFluct-beta2)/e1Fluct; a2 = C*f2Fluct*(w2-e2LogFluct-beta2)/e2Fluct; a3 = rateFluct*meanLoss*(tmax-ipotFluct)/(ipotFluct*tmax*log(w1)); if(a1 < 0.) a1 = 0.; if(a2 < 0.) a2 = 0.; if(a3 < 0.) a3 = 0.; suma = a1+a2+a3; loss = 0. ; if(suma < sumalim) // very small Step { //e0 = material->GetIonisation()->GetEnergy0fluct();//Hardwired in const if(tmax == ipotFluct) { a3 = meanLoss/e0; if(a3>alim) { siga=sqrt(a3) ; //p3 = G4std::max(0,int(G4RandGauss::shoot(a3,siga)+0.5)); p3 = std::max(0,int(CLHEP::RandGaussQ::shoot(a3,siga)+0.5)); } else p3 = CLHEP::RandPoisson::shoot(a3); //p3 = G4Poisson(a3); loss = p3*e0 ; if(p3 > 0) //loss += (1.-2.*G4UniformRand())*e0 ; loss += (1.-2.*CLHEP::RandFlat::shoot())*e0 ; } else { tmax = tmax-ipotFluct+e0 ; a3 = meanLoss*(tmax-e0)/(tmax*e0*log(tmax/e0)); if(a3>alim) { siga=sqrt(a3) ; //p3 = G4std::max(0,int(G4RandGauss::shoot(a3,siga)+0.5)); p3 = std::max(0,int(CLHEP::RandGaussQ::shoot(a3,siga)+0.5)); } else p3 = CLHEP::RandPoisson::shoot(a3); //p3 = G4Poisson(a3); if(p3 > 0) { w = (tmax-e0)/tmax ; if(p3 > nmaxCont2) { dp3 = float(p3) ; corrfac = dp3/float(nmaxCont2) ; p3 = nmaxCont2 ; } else corrfac = 1. ; //for(int i=0; i<p3; i++) loss += 1./(1.-w*G4UniformRand()) ; for(int i=0; i<p3; i++) loss += 1./(1.-w*CLHEP::RandFlat::shoot()) ; loss *= e0*corrfac ; } } } else // not so small Step { // excitation type 1 if(a1>alim) { siga=sqrt(a1) ; //p1 = std::max(0,int(G4RandGauss::shoot(a1,siga)+0.5)); p1 = std::max(0,int(CLHEP::RandGaussQ::shoot(a1,siga)+0.5)); } else p1 = CLHEP::RandPoisson::shoot(a1); //p1 = G4Poisson(a1); // excitation type 2 if(a2>alim) { siga=sqrt(a2) ; //p2 = std::max(0,int(G4RandGauss::shoot(a2,siga)+0.5)); p2 = std::max(0,int(CLHEP::RandGaussQ::shoot(a2,siga)+0.5)); } else p2 = CLHEP::RandPoisson::shoot(a2); //p2 = G4Poisson(a2); loss = p1*e1Fluct+p2*e2Fluct; // smearing to avoid unphysical peaks if(p2 > 0) //loss += (1.-2.*G4UniformRand())*e2Fluct; loss += (1.-2.*CLHEP::RandFlat::shoot())*e2Fluct; else if (loss>0.) loss += (1.-2.*CLHEP::RandFlat::shoot())*e1Fluct; // ionisation ....................................... if(a3 > 0.) { if(a3>alim) { siga=sqrt(a3) ; p3 = std::max(0,int(CLHEP::RandGaussQ::shoot(a3,siga)+0.5)); } else p3 = CLHEP::RandPoisson::shoot(a3); lossc = 0.; if(p3 > 0) { na = 0.; alfa = 1.; if (p3 > nmaxCont2) { dp3 = float(p3); rfac = dp3/(float(nmaxCont2)+dp3); namean = float(p3)*rfac; sa = float(nmaxCont1)*rfac; na = CLHEP::RandGaussQ::shoot(namean,sa); if (na > 0.) { alfa = w1*float(nmaxCont2+p3)/ (w1*float(nmaxCont2)+float(p3)); alfa1 = alfa*log(alfa)/(alfa-1.); ea = na*ipotFluct*alfa1; sea = ipotFluct*sqrt(na*(alfa-alfa1*alfa1)); lossc += CLHEP::RandGaussQ::shoot(ea,sea); } } nb = int(float(p3)-na); if (nb > 0) { w2 = alfa*ipotFluct; w = (tmax-w2)/tmax; for (int k=0; k<nb; k++) lossc += w2/(1.-w*CLHEP::RandFlat::shoot()); } } loss += lossc; } } return loss; }
double LandauFP420::alim [private] |
Definition at line 107 of file LandauFP420.h.
Referenced by SampleFluctuations().
double LandauFP420::chargeSquare [private] |
Definition at line 85 of file LandauFP420.h.
Referenced by LandauFP420(), and SampleFluctuations().
double LandauFP420::e0 [private] |
Definition at line 100 of file LandauFP420.h.
Referenced by LandauFP420(), and SampleFluctuations().
double LandauFP420::e1Fluct [private] |
Definition at line 94 of file LandauFP420.h.
Referenced by LandauFP420(), and SampleFluctuations().
double LandauFP420::e1LogFluct [private] |
Definition at line 97 of file LandauFP420.h.
Referenced by LandauFP420(), and SampleFluctuations().
double LandauFP420::e2Fluct [private] |
Definition at line 95 of file LandauFP420.h.
Referenced by LandauFP420(), and SampleFluctuations().
double LandauFP420::e2LogFluct [private] |
Definition at line 98 of file LandauFP420.h.
Referenced by LandauFP420(), and SampleFluctuations().
double LandauFP420::electronDensity [private] |
Definition at line 89 of file LandauFP420.h.
Referenced by LandauFP420(), and SampleFluctuations().
double LandauFP420::f1Fluct [private] |
Definition at line 92 of file LandauFP420.h.
Referenced by LandauFP420(), and SampleFluctuations().
double LandauFP420::f2Fluct [private] |
Definition at line 93 of file LandauFP420.h.
Referenced by LandauFP420(), and SampleFluctuations().
double LandauFP420::ipotFluct [private] |
Definition at line 88 of file LandauFP420.h.
Referenced by LandauFP420(), and SampleFluctuations().
double LandauFP420::ipotLogFluct [private] |
Definition at line 99 of file LandauFP420.h.
Referenced by LandauFP420(), and SampleFluctuations().
double LandauFP420::minLoss [private] |
Definition at line 104 of file LandauFP420.h.
Referenced by SampleFluctuations().
double LandauFP420::minNumberInteractionsBohr [private] |
Definition at line 102 of file LandauFP420.h.
Referenced by SampleFluctuations().
int LandauFP420::nmaxCont1 [private] |
Definition at line 108 of file LandauFP420.h.
Referenced by SampleFluctuations().
int LandauFP420::nmaxCont2 [private] |
Definition at line 109 of file LandauFP420.h.
Referenced by SampleFluctuations().
double LandauFP420::particleMass [private] |
Definition at line 84 of file LandauFP420.h.
Referenced by SampleFluctuations().
double LandauFP420::problim [private] |
Definition at line 105 of file LandauFP420.h.
Referenced by LandauFP420().
double LandauFP420::rateFluct [private] |
Definition at line 96 of file LandauFP420.h.
Referenced by LandauFP420(), and SampleFluctuations().
double LandauFP420::sumalim [private] |
Definition at line 106 of file LandauFP420.h.
Referenced by LandauFP420(), and SampleFluctuations().
double LandauFP420::theBohrBeta2 [private] |
Definition at line 103 of file LandauFP420.h.