#include <SiG4UniversalFluctuation.h>

Public Member Functions
SiG4UniversalFluctuation &	operator= (const SiG4UniversalFluctuation &right)=delete

double	SampleFluctuations (const double momentum, const double mass, double &tmax, const double length, const double meanLoss, CLHEP::HepRandomEngine *)

	SiG4UniversalFluctuation ()

	SiG4UniversalFluctuation (const SiG4UniversalFluctuation &)=delete

	~SiG4UniversalFluctuation ()

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

double	nmaxCont1

double	nmaxCont2

double	particleMass

double	problim

double	rateFluct

double	sumalim

double	theBohrBeta2

Detailed Description

Definition at line 25 of file SiG4UniversalFluctuation.h.

Constructor & Destructor Documentation

◆ SiG4UniversalFluctuation() [1/2]

SiG4UniversalFluctuation::SiG4UniversalFluctuation ( )

explicit

Definition at line 18 of file SiG4UniversalFluctuation.cc.

References chargeSquare, e0, e1Fluct, e1LogFluct, e2Fluct, e2LogFluct, electronDensity, f1Fluct, f2Fluct, ipotFluct, ipotLogFluct, dqm-mbProfile::log, problim, rateFluct, and sumalim.

     : minNumberInteractionsBohr(10.0),
       theBohrBeta2(50.0 * keV / proton_mass_c2),
       minLoss(10. * eV),
       problim(5.e-3),
       alim(10.),
       nmaxCont1(4.),
       nmaxCont2(16.) {
   sumalim = -log(problim);
 
   // Add these definitions d.k.
   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();
 
   // cout << " init new fluct +++++++++++++++++++++++++++++++++++++++++"<<endl;
 }

◆ SiG4UniversalFluctuation() [2/2]

SiG4UniversalFluctuation::SiG4UniversalFluctuation ( const SiG4UniversalFluctuation & )

delete

◆ ~SiG4UniversalFluctuation()

SiG4UniversalFluctuation::~SiG4UniversalFluctuation ( )

Definition at line 51 of file SiG4UniversalFluctuation.cc.

51 {}

Member Function Documentation

◆ operator=()

SiG4UniversalFluctuation& SiG4UniversalFluctuation::operator= ( const SiG4UniversalFluctuation & right )

delete

◆ SampleFluctuations()

double SiG4UniversalFluctuation::SampleFluctuations	(	const double	momentum,
		const double	mass,
		double &	tmax,
		const double	length,
		const double	meanLoss,
		CLHEP::HepRandomEngine *	engine
	)

Definition at line 53 of file SiG4UniversalFluctuation.cc.

References testProducerWithPsetDescEmpty_cfi::a2, alim, correctionTermsCaloMet_cff::C, chargeSquare, e0, e1Fluct, e1LogFluct, e2Fluct, e2LogFluct, electronDensity, f1Fluct, f2Fluct, mps_fire::i, createfilelist::int, ipotFluct, ipotLogFluct, dqmdumpme::k, EgHLTOffHistBins_cfi::mass, SiStripPI::max, minLoss, minNumberInteractionsBohr, nmaxCont1, nmaxCont2, LaserDQM_cfg::p1, SiStripOfflineCRack_cfg::p2, chargedHadronTrackResolutionFilter_cfi::p3, particleMass, RPCpg::rate(), rateFluct, mathSSE::sqrt(), sumalim, tmax, w(), w1, w2, and x.

Referenced by RPixLinearChargeDivider::FluctuateEloss().

                                                                                   {
   // Calculate actual loss from the mean loss.
   // The model used to get the fluctuations is essentially the same
   // as in Glandz in Geant3 (Cern program library W5013, phys332).
   // L. Urban et al. NIM A362, p.416 (1995) and Geant4 Physics Reference Manual
 
   // shortcut for very very small loss (out of validity of the model)
   //
   if (meanLoss < minLoss)
     return meanLoss;
 
   particleMass = mass;
   double gam2 = (momentum * momentum) / (particleMass * particleMass) + 1.0;
   double beta2 = 1.0 - 1.0 / gam2;
   double gam = sqrt(gam2);
 
   double loss(0.), siga(0.);
 
   // Gaussian regime
   // for heavy particles only and conditions
   // for Gauusian fluct. has been changed
   //
   if ((particleMass > electron_mass_c2) && (meanLoss >= minNumberInteractionsBohr * tmax)) {
     double massrate = electron_mass_c2 / particleMass;
     double tmaxkine = 2. * electron_mass_c2 * beta2 * gam2 / (1. + massrate * (2. * gam + massrate));
     if (tmaxkine <= 2. * tmax) {
       siga = (1.0 / beta2 - 0.5) * twopi_mc2_rcl2 * tmax * length * electronDensity * chargeSquare;
       siga = sqrt(siga);
       double twomeanLoss = meanLoss + meanLoss;
       if (twomeanLoss < siga) {
         double x;
         do {
           loss = twomeanLoss * CLHEP::RandFlat::shoot(engine);
           x = (loss - meanLoss) / siga;
         } while (1.0 - 0.5 * x * x < CLHEP::RandFlat::shoot(engine));
       } else {
         do {
           loss = CLHEP::RandGaussQ::shoot(engine, meanLoss, siga);
         } while (loss < 0. || loss > twomeanLoss);
       }
       return loss;
     }
   }
 
   double a1 = 0., a2 = 0., a3 = 0.;
   double p3;
   double rate = rateFluct;
 
   double w1 = tmax / ipotFluct;
   double w2 = vdt::fast_log(2. * electron_mass_c2 * beta2 * gam2) - beta2;
 
   if (w2 > ipotLogFluct) {
     double C = meanLoss * (1. - rateFluct) / (w2 - ipotLogFluct);
     a1 = C * f1Fluct * (w2 - e1LogFluct) / e1Fluct;
     a2 = C * f2Fluct * (w2 - e2LogFluct) / e2Fluct;
     if (a2 < 0.) {
       a1 = 0.;
       a2 = 0.;
       rate = 1.;
     }
   } else {
     rate = 1.;
   }
 
   // added
   if (tmax > ipotFluct) {
     a3 = rate * meanLoss * (tmax - ipotFluct) / (ipotFluct * tmax * vdt::fast_log(w1));
   }
   double suma = a1 + a2 + a3;
 
   // Glandz regime
   //
   if (suma > sumalim) {
     if ((a1 + a2) > 0.) {
       double p1, p2;
       // excitation type 1
       if (a1 > alim) {
         siga = sqrt(a1);
         p1 = max(0., CLHEP::RandGaussQ::shoot(engine, a1, siga) + 0.5);
       } else {
         p1 = double(CLHEP::RandPoissonQ::shoot(engine, a1));
       }
 
       // excitation type 2
       if (a2 > alim) {
         siga = sqrt(a2);
         p2 = max(0., CLHEP::RandGaussQ::shoot(engine, a2, siga) + 0.5);
       } else {
         p2 = double(CLHEP::RandPoissonQ::shoot(engine, a2));
       }
 
       loss = p1 * e1Fluct + p2 * e2Fluct;
 
       // smearing to avoid unphysical peaks
       if (p2 > 0.)
         loss += (1. - 2. * CLHEP::RandFlat::shoot(engine)) * e2Fluct;
       else if (loss > 0.)
         loss += (1. - 2. * CLHEP::RandFlat::shoot(engine)) * e1Fluct;
       if (loss < 0.)
         loss = 0.0;
     }
 
     // ionisation
     if (a3 > 0.) {
       if (a3 > alim) {
         siga = sqrt(a3);
         p3 = max(0., CLHEP::RandGaussQ::shoot(engine, a3, siga) + 0.5);
       } else {
         p3 = double(CLHEP::RandPoissonQ::shoot(engine, a3));
       }
       double lossc = 0.;
       if (p3 > 0) {
         double na = 0.;
         double alfa = 1.;
         if (p3 > nmaxCont2) {
           double rfac = p3 / (nmaxCont2 + p3);
           double namean = p3 * rfac;
           double sa = nmaxCont1 * rfac;
           na = CLHEP::RandGaussQ::shoot(engine, namean, sa);
           if (na > 0.) {
             alfa = w1 * (nmaxCont2 + p3) / (w1 * nmaxCont2 + p3);
             double alfa1 = alfa * vdt::fast_log(alfa) / (alfa - 1.);
             double ea = na * ipotFluct * alfa1;
             double sea = ipotFluct * sqrt(na * (alfa - alfa1 * alfa1));
             lossc += CLHEP::RandGaussQ::shoot(engine, ea, sea);
           }
         }
 
         if (p3 > na) {
           w2 = alfa * ipotFluct;
           double w = (tmax - w2) / tmax;
           int nb = int(p3 - na);
           for (int k = 0; k < nb; k++)
             lossc += w2 / (1. - w * CLHEP::RandFlat::shoot(engine));
         }
       }
       loss += lossc;
     }
     return loss;
   }
 
   // suma < sumalim;  very small energy loss;
   a3 = meanLoss * (tmax - e0) / (tmax * e0 * vdt::fast_log(tmax / e0));
   if (a3 > alim) {
     siga = sqrt(a3);
     p3 = max(0., CLHEP::RandGaussQ::shoot(engine, a3, siga) + 0.5);
   } else {
     p3 = double(CLHEP::RandPoissonQ::shoot(engine, a3));
   }
   if (p3 > 0.) {
     double w = (tmax - e0) / tmax;
     double corrfac = 1.;
     if (p3 > nmaxCont2) {
       corrfac = p3 / nmaxCont2;
       p3 = nmaxCont2;
     }
     int ip3 = (int)p3;
     for (int i = 0; i < ip3; i++)
       loss += 1. / (1. - w * CLHEP::RandFlat::shoot(engine));
     loss *= e0 * corrfac;
     // smearing for losses near to e0
     if (p3 <= 2.)
       loss += e0 * (1. - 2. * CLHEP::RandFlat::shoot(engine));
   }
 
   return loss;
 }