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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. * // ******************************************************************** // // // ------------------------------------------------------------------- // GEANT 4 class implementation file // // CERN, Geneva, Switzerland // // File name: G4RKPropagation.cc // // Author: Alessandro Brunengo (Alessandro.Brunengo@ge.infn.it) // // Creation date: 6 June 2000 // ------------------------------------------------------------------- #include "G4RKPropagation.hh" // nuclear fields #include "G4VNuclearField.hh" #include "G4ProtonField.hh" #include "G4NeutronField.hh" #include "G4AntiProtonField.hh" #include "G4KaonPlusField.hh" #include "G4KaonMinusField.hh" #include "G4KaonZeroField.hh" #include "G4PionPlusField.hh" #include "G4PionMinusField.hh" #include "G4PionZeroField.hh" #include "G4SigmaPlusField.hh" #include "G4SigmaMinusField.hh" #include "G4SigmaZeroField.hh" // particles properties #include "G4Proton.hh" #include "G4Neutron.hh" #include "G4AntiProton.hh" #include "G4KaonPlus.hh" #include "G4KaonMinus.hh" #include "G4KaonZero.hh" #include "G4PionPlus.hh" #include "G4PionMinus.hh" #include "G4PionZero.hh" #include "G4SigmaPlus.hh" #include "G4SigmaMinus.hh" #include "G4SigmaZero.hh" #include "globals.hh" #include "G4KM_OpticalEqRhs.hh" #include "G4KM_NucleonEqRhs.hh" #include "G4ClassicalRK4.hh" #include "G4MagIntegratorDriver.hh" #include "G4LorentzRotation.hh" // unsigned EncodingHashFun(const G4int& aEncoding); G4RKPropagation::G4RKPropagation() : theNucleus(0), theFieldMap(0), theEquationMap(0), theField(0) { } G4RKPropagation::G4RKPropagation(const G4RKPropagation &) : G4VFieldPropagation() { } G4RKPropagation::~G4RKPropagation() { // free theFieldMap memory if(theFieldMap) delete_FieldsAndMap(theFieldMap); // free theEquationMap memory if(theEquationMap) delete_EquationsAndMap(theEquationMap); if (theField) delete theField; } const G4RKPropagation & G4RKPropagation::operator=(const G4RKPropagation &) { throw G4HadronicException(__FILE__, __LINE__, "G4RKPropagation::operator= meant not to be accessible"); return *this; } G4int G4RKPropagation::operator==(const G4RKPropagation &) const { throw G4HadronicException(__FILE__, __LINE__, "G4RKPropagation::operator== meant not to be accessible"); return 0; } G4int G4RKPropagation::operator!=(const G4RKPropagation &) const { throw G4HadronicException(__FILE__, __LINE__, "G4RKPropagation::operator!= meant not to be accessible"); return 1; } //---------------------------------------------------------------------------- //---------------------------------------------------------------------------- void G4RKPropagation::Init(G4V3DNucleus * nucleus) //---------------------------------------------------------------------------- { // free theFieldMap memory if(theFieldMap) delete_FieldsAndMap(theFieldMap); // free theEquationMap memory if(theEquationMap) delete_EquationsAndMap(theEquationMap); if (theField) delete theField; // Initialize the nuclear field map. theNucleus = nucleus; theOuterRadius = theNucleus->GetOuterRadius(); theFieldMap = new std::map >; (*theFieldMap)[G4Proton::Proton()->GetPDGEncoding()] = new G4ProtonField(theNucleus); (*theFieldMap)[G4Neutron::Neutron()->GetPDGEncoding()] = new G4NeutronField(theNucleus); (*theFieldMap)[G4AntiProton::AntiProton()->GetPDGEncoding()] = new G4AntiProtonField(theNucleus); (*theFieldMap)[G4KaonPlus::KaonPlus()->GetPDGEncoding()] = new G4KaonPlusField(theNucleus); (*theFieldMap)[G4KaonMinus::KaonMinus()->GetPDGEncoding()] = new G4KaonMinusField(theNucleus); (*theFieldMap)[G4KaonZero::KaonZero()->GetPDGEncoding()] = new G4KaonZeroField(theNucleus); (*theFieldMap)[G4PionPlus::PionPlus()->GetPDGEncoding()] = new G4PionPlusField(theNucleus); (*theFieldMap)[G4PionMinus::PionMinus()->GetPDGEncoding()] = new G4PionMinusField(theNucleus); (*theFieldMap)[G4PionZero::PionZero()->GetPDGEncoding()] = new G4PionZeroField(theNucleus); (*theFieldMap)[G4SigmaPlus::SigmaPlus()->GetPDGEncoding()] = new G4SigmaPlusField(theNucleus); (*theFieldMap)[G4SigmaMinus::SigmaMinus()->GetPDGEncoding()] = new G4SigmaMinusField(theNucleus); (*theFieldMap)[G4SigmaZero::SigmaZero()->GetPDGEncoding()] = new G4SigmaZeroField(theNucleus); theEquationMap = new std::map >; // theField needed by the design of G4Mag_eqRhs theField = new G4KM_DummyField; //Field not needed for integration G4KM_OpticalEqRhs * opticalEq; G4KM_NucleonEqRhs * nucleonEq; G4double mass; G4double opticalCoeff; nucleonEq = new G4KM_NucleonEqRhs(theField, theNucleus); mass = G4Proton::Proton()->GetPDGMass(); nucleonEq->SetMass(mass); (*theEquationMap)[G4Proton::Proton()->GetPDGEncoding()] = nucleonEq; nucleonEq = new G4KM_NucleonEqRhs(theField, theNucleus); mass = G4Neutron::Neutron()->GetPDGMass(); nucleonEq->SetMass(mass); (*theEquationMap)[G4Neutron::Neutron()->GetPDGEncoding()] = nucleonEq; opticalEq = new G4KM_OpticalEqRhs(theField, theNucleus); mass = G4AntiProton::AntiProton()->GetPDGMass(); opticalCoeff = (*theFieldMap)[G4AntiProton::AntiProton()->GetPDGEncoding()]->GetCoeff(); opticalEq->SetFactor(mass,opticalCoeff); (*theEquationMap)[G4AntiProton::AntiProton()->GetPDGEncoding()] = opticalEq; opticalEq = new G4KM_OpticalEqRhs(theField, theNucleus); mass = G4KaonPlus::KaonPlus()->GetPDGMass(); opticalCoeff = (*theFieldMap)[G4KaonPlus::KaonPlus()->GetPDGEncoding()]->GetCoeff(); opticalEq->SetFactor(mass,opticalCoeff); (*theEquationMap)[G4KaonPlus::KaonPlus()->GetPDGEncoding()] = opticalEq; opticalEq = new G4KM_OpticalEqRhs(theField, theNucleus); mass = G4KaonMinus::KaonMinus()->GetPDGMass(); opticalCoeff = (*theFieldMap)[G4KaonMinus::KaonMinus()->GetPDGEncoding()]->GetCoeff(); opticalEq->SetFactor(mass,opticalCoeff); (*theEquationMap)[G4KaonMinus::KaonMinus()->GetPDGEncoding()] = opticalEq; opticalEq = new G4KM_OpticalEqRhs(theField, theNucleus); mass = G4KaonZero::KaonZero()->GetPDGMass(); opticalCoeff = (*theFieldMap)[G4KaonZero::KaonZero()->GetPDGEncoding()]->GetCoeff(); opticalEq->SetFactor(mass,opticalCoeff); (*theEquationMap)[G4KaonZero::KaonZero()->GetPDGEncoding()] = opticalEq; opticalEq = new G4KM_OpticalEqRhs(theField, theNucleus); mass = G4PionPlus::PionPlus()->GetPDGMass(); opticalCoeff = (*theFieldMap)[G4PionPlus::PionPlus()->GetPDGEncoding()]->GetCoeff(); opticalEq->SetFactor(mass,opticalCoeff); (*theEquationMap)[G4PionPlus::PionPlus()->GetPDGEncoding()] = opticalEq; opticalEq = new G4KM_OpticalEqRhs(theField, theNucleus); mass = G4PionMinus::PionMinus()->GetPDGMass(); opticalCoeff = (*theFieldMap)[G4PionMinus::PionMinus()->GetPDGEncoding()]->GetCoeff(); opticalEq->SetFactor(mass,opticalCoeff); (*theEquationMap)[G4PionMinus::PionMinus()->GetPDGEncoding()] = opticalEq; opticalEq = new G4KM_OpticalEqRhs(theField, theNucleus); mass = G4PionZero::PionZero()->GetPDGMass(); opticalCoeff = (*theFieldMap)[G4PionZero::PionZero()->GetPDGEncoding()]->GetCoeff(); opticalEq->SetFactor(mass,opticalCoeff); (*theEquationMap)[G4PionZero::PionZero()->GetPDGEncoding()] = opticalEq; opticalEq = new G4KM_OpticalEqRhs(theField, theNucleus); mass = G4SigmaPlus::SigmaPlus()->GetPDGMass(); opticalCoeff = (*theFieldMap)[G4SigmaPlus::SigmaPlus()->GetPDGEncoding()]->GetCoeff(); opticalEq->SetFactor(mass,opticalCoeff); (*theEquationMap)[G4SigmaPlus::SigmaPlus()->GetPDGEncoding()] = opticalEq; opticalEq = new G4KM_OpticalEqRhs(theField, theNucleus); mass = G4SigmaMinus::SigmaMinus()->GetPDGMass(); opticalCoeff = (*theFieldMap)[G4SigmaMinus::SigmaMinus()->GetPDGEncoding()]->GetCoeff(); opticalEq->SetFactor(mass,opticalCoeff); (*theEquationMap)[G4SigmaMinus::SigmaMinus()->GetPDGEncoding()] = opticalEq; opticalEq = new G4KM_OpticalEqRhs(theField, theNucleus); mass = G4SigmaZero::SigmaZero()->GetPDGMass(); opticalCoeff = (*theFieldMap)[G4SigmaZero::SigmaZero()->GetPDGEncoding()]->GetCoeff(); opticalEq->SetFactor(mass,opticalCoeff); (*theEquationMap)[G4SigmaZero::SigmaZero()->GetPDGEncoding()] = opticalEq; } //#define debug_1_RKPropagation 1 //---------------------------------------------------------------------------- void G4RKPropagation::Transport(G4KineticTrackVector & active, //---------------------------------------------------------------------------- const G4KineticTrackVector &, G4double timeStep) { // reset momentum transfer to field theMomentumTranfer=G4ThreeVector(0,0,0); // Loop over tracks std::vector::iterator i; for(i = active.begin(); i != active.end(); ++i) { G4double currTimeStep = timeStep; G4KineticTrack * kt = *i; G4int encoding = kt->GetDefinition()->GetPDGEncoding(); std::map >::iterator fieldIter= theFieldMap->find(encoding); G4VNuclearField* currentField=0; if ( fieldIter != theFieldMap->end() ) currentField=fieldIter->second; // debug // if ( timeStep > 1e30 ) { // G4cout << " Name :" << kt->GetDefinition()->GetParticleName() << G4endl; // } // Get the time of intersections with the nucleus surface. G4double t_enter, t_leave; // if the particle does not intersecate with the nucleus go to next particle if(!GetSphereIntersectionTimes(kt, t_enter, t_leave)) { kt->SetState(G4KineticTrack::miss_nucleus); continue; } #ifdef debug_1_RKPropagation G4cout <<" kt,timeStep, Intersection times tenter, tleave " <= t_leave ) { if ( kt->GetState() == G4KineticTrack::inside ) { kt->SetState(G4KineticTrack::gone_out); } else { kt->SetState(G4KineticTrack::miss_nucleus);} } continue; } if(t_enter > 0) // the particle is out. Transport free to the surface { if(t_enter > currTimeStep) // the particle won't enter the nucleus { FreeTransport(kt, currTimeStep); continue; } else { FreeTransport(kt, t_enter); // go to surface currTimeStep -= t_enter; t_leave -= t_enter; // time left to leave nucleus // on the surface the particle loose the barrier energy // G4double newE = mom.e()-(*theFieldMap)[encoding]->GetBarrier(); // GetField = Barrier + FermiPotential G4double newE = kt->GetTrackingMomentum().e()-currentField->GetField(kt->GetPosition()); if(newE <= kt->GetActualMass()) // the particle cannot enter the nucleus { // FixMe: should be "pushed back?" // for the moment take it past the nucleus, so we'll not worry next time.. FreeTransport(kt, 1.1*t_leave); // take past nucleus kt->SetState(G4KineticTrack::miss_nucleus); // G4cout << "G4RKPropagation: Warning particle cannot enter Nucleus :" << G4endl; // G4cout << " enter nucleus, E out/in: " << kt->GetTrackingMomentum().e() << " / " << newE <GetField(kt->GetPosition()) << " "<< kt->GetPosition()<GetDefinition()->GetParticleName()<GetActualMass())); G4LorentzVector new4Mom(newP*kt->GetTrackingMomentum().vect().unit(), newE); G4ThreeVector transfer(kt->GetTrackingMomentum().vect()-new4Mom.vect()); G4ThreeVector boost= transfer / std::sqrt(transfer.mag2() + sqr(theNucleus->GetMass())); new4Mom*=G4LorentzRotation(boost); kt->SetTrackingMomentum(new4Mom); kt->SetState(G4KineticTrack::inside); /* G4cout <<" Enter Nucleus - E/Field/Sum: " <GetTrackingMomentum().e() << " / " << (*theFieldMap)[encoding]->GetField(kt->GetPosition()) << " / " << kt->GetTrackingMomentum().e()-currentField->GetField(kt->GetPosition()) << G4endl << " Barrier / field just inside nucleus (0.9999*kt->GetPosition())" << (*theFieldMap)[encoding]->GetBarrier() << " / " << (*theFieldMap)[encoding]->GetField(0.9999*kt->GetPosition()) << G4endl; */ } } // FixMe: should I add a control on theCutOnP here? // Transport the particle into the nucleus // G4cerr << "RKPropagation t_leave, curTimeStep " < t_leave) // particle will exit from the nucleus { currTimeStep = t_leave; is_exiting=true; } #ifdef debug_1_RKPropagation G4cerr << "RKPropagation is_exiting?, t_leave, curTimeStep " <GetTrackingMomentum().e() - kt->GetTrackingMomentum().mag() << " " << kt->GetPosition()<<" " << G4endl << currentField->GetField(kt->GetPosition()) << " " << kt->GetProjectilePotential()<< G4endl << kt->GetTrackingMomentum() << G4endl; #endif G4LorentzVector momold=kt->GetTrackingMomentum(); G4ThreeVector posold=kt->GetPosition(); // if (currentField->GetField(kt->GetPosition()) > kt->GetProjectilePotential() || if (currTimeStep > 0 && ! FieldTransport(kt, currTimeStep)) { FreeTransport(kt,currTimeStep); } #ifdef debug_1_RKPropagation G4cout << "RKPropagation Ekin, field, p " << kt->GetTrackingMomentum().e() - kt->GetTrackingMomentum().mag() << " " << G4endl << currentField->GetField(kt->GetPosition())<< G4endl << kt->GetTrackingMomentum() << G4endl << "delta p " << momold-kt->GetTrackingMomentum() << G4endl << "del pos " << posold-kt->GetPosition() << G4endl; #endif // complete the transport // FixMe: in some cases there could be a significant // part to do still in the nucleus, or we stepped to far... depending on // slope of potential G4double t_in=-1, t_out=0; // set onto boundary. // should go out, or are already out by a too long step.. if(is_exiting || (GetSphereIntersectionTimes(kt, t_in, t_out) &&t_in<0 && t_out<=0 )) // particle is exiting { if(t_in < 0 && t_out >= 0) //still inside, transport safely out. { // transport free to a position that is surely out of the nucleus, to avoid // a new transportation and a new adding the barrier next loop. G4ThreeVector savePos = kt->GetPosition(); FreeTransport(kt, t_out); // and evaluate the right the energy G4double newE=kt->GetTrackingMomentum().e(); // G4cout << " V pos/savePos << " // << (*theFieldMap)[encoding]->GetField(kt->GetPosition())<< " / " // << (*theFieldMap)[encoding]->GetField(savePos) // << G4endl; if ( std::abs(currentField->GetField(savePos)) > 0. && std::abs(currentField->GetField(kt->GetPosition())) > 0.) { // FixMe GF: savePos/pos may be out of nucleus, where GetField(..)=0 // This wrongly adds or subtracts the Barrier here while // this is done later. newE += currentField->GetField(savePos) - currentField->GetField(kt->GetPosition()); } // G4cout << " go border nucleus, E in/border: " << kt->GetTrackingMomentum() << " / " << newE <GetActualMass()) { #ifdef debug_1_RKPropagation G4cout << "RKPropagation-Transport: problem with particle exiting - ignored" << G4endl; G4cout << " cannot leave nucleus, E in/out: " << kt->GetTrackingMomentum() << " / " << newE <GetDefinition() == G4Proton::Proton() || kt->GetDefinition() == G4Neutron::Neutron() ) { kt->SetState(G4KineticTrack::captured); } else { kt->SetState(G4KineticTrack::gone_out); //@@GF tofix } continue; // the particle cannot exit the nucleus } G4double newP = std::sqrt(newE*newE- sqr(kt->GetActualMass())); G4LorentzVector new4Mom(newP*kt->GetTrackingMomentum().vect().unit(), newE); G4ThreeVector transfer(kt->GetTrackingMomentum().vect()-new4Mom.vect()); G4ThreeVector boost= transfer / std::sqrt(transfer.mag2() + sqr(theNucleus->GetMass())); new4Mom*=G4LorentzRotation(boost); kt->SetTrackingMomentum(new4Mom); } // add the potential barrier // FixMe the Coulomb field is not parallel to mom, this is simple approximation G4double newE = kt->GetTrackingMomentum().e()+currentField->GetField(kt->GetPosition()); if(newE < kt->GetActualMass()) { // the particle cannot exit the nucleus @@@ GF check. #ifdef debug_1_RKPropagation G4cout << " cannot leave nucleus, E in/out: " << kt->GetTrackingMomentum() << " / " << newE <GetDefinition() == G4Proton::Proton() || kt->GetDefinition() == G4Neutron::Neutron() ) { kt->SetState(G4KineticTrack::captured); } else { kt->SetState(G4KineticTrack::gone_out); //@@GF tofix } continue; } G4double newP = std::sqrt(newE*newE- sqr(kt->GetActualMass())); G4LorentzVector new4Mom(newP*kt->GetTrackingMomentum().vect().unit(), newE); G4ThreeVector transfer(kt->GetTrackingMomentum().vect()-new4Mom.vect()); G4ThreeVector boost= transfer / std::sqrt(transfer.mag2() + sqr(theNucleus->GetMass())); new4Mom*=G4LorentzRotation(boost); kt->SetTrackingMomentum(new4Mom); kt->SetState(G4KineticTrack::gone_out); } } } //---------------------------------------------------------------------------- G4ThreeVector G4RKPropagation::GetMomentumTransfer() const //---------------------------------------------------------------------------- { return theMomentumTranfer; } //---------------------------------------------------------------------------- G4bool G4RKPropagation::FieldTransport(G4KineticTrack * kt, const G4double timeStep) //---------------------------------------------------------------------------- { theMomentumTranfer=G4ThreeVector(0,0,0); // G4cout <<"Stepper input"<GetTrackingMomentum()<second; G4Mag_EqRhs * equation = (*theEquationMap)[kt->GetDefinition()->GetPDGEncoding()]; G4MagIntegratorStepper * stepper = new G4ClassicalRK4(equation); // create the integrator driver G4double hMin = 1.0e-25*second; // arbitrary choice. Means 0.03 fm at c G4MagInt_Driver * driver = new G4MagInt_Driver(hMin, stepper); // Temporary: use driver->AccurateAdvance() // create the G4FieldTrack needed by AccurateAdvance G4double curveLength = 0; G4FieldTrack track(kt->GetPosition(), kt->GetTrackingMomentum().vect().unit(), // momentum direction curveLength, // curvelength kt->GetTrackingMomentum().e()-kt->GetActualMass(), // kinetic energy kt->GetActualMass(), // restmass kt->GetTrackingMomentum().beta()*c_light); // velocity // integrate G4double eps = 0.01; // G4cout << "currTimeStep = " << currTimeStep << G4endl; if(!driver->AccurateAdvance(track, timeStep, eps)) { // cannot track this particle #ifdef debug_1_RKPropagation std::cerr << "G4RKPropagation::FieldTransport() warning: integration error." << G4endl << "position " << kt->GetPosition() << " 4mom " <GetTrackingMomentum() <GetField(pos) << " / " << mom.e()+(*theFieldMap)[encoding]->GetField(pos) << G4endl; */ // Correct for momentum ( thus energy) transfered to nucleus, boost particle into moving nuclues frame. G4ThreeVector MomentumTranfer = kt->GetTrackingMomentum().vect() - track.GetMomentum(); G4ThreeVector boost= MomentumTranfer / std::sqrt (MomentumTranfer.mag2() +sqr(theNucleus->GetMass())); // update the kt kt->SetPosition(track.GetPosition()); G4LorentzVector mom(track.GetMomentum(),std::sqrt(track.GetMomentum().mag2() + sqr(kt->GetActualMass()))); mom *= G4LorentzRotation( boost ); theMomentumTranfer += ( kt->GetTrackingMomentum() - mom ).vect(); kt->SetTrackingMomentum(mom); // G4cout <<"Stepper output"<GetTrackingMomentum()<<" "<GetPosition()<GetTrackingMomentum().vect() - mom.vect(); * G4cout << " MomentumTransfer/corrected" << MomentumTranfer << " " << MomentumTranfer.mag() * << " " << MomentumTranfer2 << " " << MomentumTranfer2.mag() << " " * << MomentumTranfer-MomentumTranfer2 << " "<< * MomentumTranfer-MomentumTranfer2.mag() << " " << G4endl; * G4cout <<" E/Field/Sum aft : " <GetField(pos)<< " / " * << mom.e()+(*theFieldMap)[encoding]->GetField(pos) * << G4endl; */ delete driver; delete stepper; return true; } //---------------------------------------------------------------------------- G4bool G4RKPropagation::FreeTransport(G4KineticTrack * kt, const G4double timeStep) //---------------------------------------------------------------------------- { G4ThreeVector newpos = kt->GetPosition() + timeStep*c_light/kt->GetTrackingMomentum().e() * kt->GetTrackingMomentum().vect(); kt->SetPosition(newpos); return true; } /* G4bool G4RKPropagation::WillBeCaptured(const G4KineticTrack * kt) { G4double radius = theOuterRadius; // evaluate the final energy. Il will be captured if newE or newP < 0 G4ParticleDefinition * definition = kt->GetDefinition(); G4double mass = definition->GetPDGMass(); G4ThreeVector pos = kt->GetPosition(); G4LorentzVector mom = kt->GetTrackingMomentum(); G4VNuclearField * field = (*theFieldMap)[definition->GetPDGEncoding()]; G4ThreeVector newPos(0, 0, radius); // to get the field on the surface G4double newE = mom.e()+field->GetField(pos)-field->GetField(newPos); return ((newE < mass) ? false : true); } */ //---------------------------------------------------------------------------- G4bool G4RKPropagation::GetSphereIntersectionTimes(const G4double radius, //---------------------------------------------------------------------------- const G4ThreeVector & currentPos, const G4LorentzVector & momentum, G4double & t1, G4double & t2) { G4ThreeVector speed = momentum.vect()/momentum.e(); // boost vector G4double scalarProd = currentPos.dot(speed); G4double speedMag = speed.mag(); G4double sqrtArg = scalarProd*scalarProd - speedMag*speedMag*(currentPos.mag2()-radius*radius); if(sqrtArg <= 0.) // particle will not intersect the sphere { // G4cout << " GetSphereIntersectionTimes sqrtArg negative: " << sqrtArg << G4endl; return false; } t1 = (-scalarProd - std::sqrt(sqrtArg))/speedMag/speedMag/c_light; t2 = (-scalarProd + std::sqrt(sqrtArg))/speedMag/speedMag/c_light; return true; } //---------------------------------------------------------------------------- G4bool G4RKPropagation::GetSphereIntersectionTimes(const G4KineticTrack * kt, G4double & t1, G4double & t2) { G4double radius = theOuterRadius + 3*fermi; // "safety" of 3 fermi G4ThreeVector speed = kt->GetTrackingMomentum().vect()/kt->GetTrackingMomentum().e(); // bost vector G4double scalarProd = kt->GetPosition().dot(speed); G4double speedMag2 = speed.mag2(); G4double sqrtArg = scalarProd*scalarProd - speedMag2*(kt->GetPosition().mag2()-radius*radius); if(sqrtArg <= 0.) // particle will not intersect the sphere { return false; } t1 = (-scalarProd - std::sqrt(sqrtArg))/speedMag2/c_light; t2 = (-scalarProd + std::sqrt(sqrtArg))/speedMag2/c_light; return true; } // Implementation methods //---------------------------------------------------------------------------- void G4RKPropagation::delete_FieldsAndMap( //---------------------------------------------------------------------------- std::map > * aMap) { if(aMap) { std::map >::iterator cur; for(cur = aMap->begin(); cur != aMap->end(); ++cur) delete (*cur).second; aMap->clear(); delete aMap; } } //---------------------------------------------------------------------------- void G4RKPropagation::delete_EquationsAndMap( //---------------------------------------------------------------------------- std::map > * aMap) { if(aMap) { std::map >::iterator cur; for(cur = aMap->begin(); cur != aMap->end(); ++cur) delete (*cur).second; aMap->clear(); delete aMap; } }