247 lines
8.1 KiB
C++
247 lines
8.1 KiB
C++
//
|
|
// ********************************************************************
|
|
// * 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. *
|
|
// ********************************************************************
|
|
//
|
|
//
|
|
//
|
|
|
|
#include <time.h>
|
|
|
|
#include "Randomize.hh"
|
|
#include "G4TransportationManager.hh"
|
|
|
|
#include "G4ExplicitEuler.hh"
|
|
#include "G4ImplicitEuler.hh"
|
|
#include "G4SimpleRunge.hh"
|
|
#include "G4SimpleHeum.hh"
|
|
#include "G4ClassicalRK4.hh"
|
|
#include "G4CashKarpRKF45.hh"
|
|
|
|
#include "F04GlobalField.hh"
|
|
|
|
F04GlobalField* F04GlobalField::object = 0;
|
|
|
|
F04GlobalField::F04GlobalField() : G4ElectroMagneticField(),
|
|
minStep(0.01*mm), deltaChord(3.0*mm),
|
|
deltaOneStep(0.01*mm), deltaIntersection(0.1*mm),
|
|
epsMin(2.5e-7*mm), epsMax(0.05*mm),
|
|
fEquation(0), fFieldManager(0),
|
|
fFieldPropagator(0), fStepper(0), fChordFinder(0)
|
|
//F04GlobalField::F04GlobalField() : G4MagneticField(),
|
|
// minStep(0.01*mm), deltaChord(3.0*mm),
|
|
// deltaOneStep(0.01*mm), deltaIntersection(0.1*mm),
|
|
// epsMin(2.5e-7*mm), epsMax(0.05*mm),
|
|
// fEquation(0), fFieldManager(0),
|
|
// fFieldPropagator(0), fStepper(0), fChordFinder(0)
|
|
{
|
|
fFieldMessenger = new F04FieldMessenger(this);
|
|
|
|
fields = new FieldList();
|
|
|
|
fStepperType = 4 ; // ClassicalRK4 is default stepper
|
|
|
|
// set object
|
|
|
|
object = this;
|
|
|
|
updateField();
|
|
}
|
|
|
|
F04GlobalField::~F04GlobalField()
|
|
{
|
|
clear();
|
|
|
|
delete fFieldMessenger;
|
|
|
|
if (fEquation) delete fEquation;
|
|
if (fFieldManager) delete fFieldManager;
|
|
if (fFieldPropagator) delete fFieldPropagator;
|
|
if (fStepper) delete fStepper;
|
|
if (fChordFinder) delete fChordFinder;
|
|
}
|
|
|
|
void F04GlobalField::updateField()
|
|
{
|
|
first = true;
|
|
|
|
nfp = 0;
|
|
fp = 0;
|
|
|
|
clear();
|
|
|
|
// Construct equ. of motion of particles through B fields
|
|
// fEquation = new G4Mag_EqRhs(this);
|
|
// Construct equ. of motion of particles through e.m. fields
|
|
// fEquation = new G4EqMagElectricField(this);
|
|
// Construct equ. of motion of particles including spin through B fields
|
|
// fEquation = new G4Mag_SpinEqRhs(this);
|
|
// Construct equ. of motion of particles including spin through e.m. fields
|
|
fEquation = new G4EqEMFieldWithSpin(this);
|
|
|
|
// Get transportation, field, and propagator managers
|
|
G4TransportationManager* fTransportManager =
|
|
G4TransportationManager::GetTransportationManager();
|
|
|
|
fFieldManager = GetGlobalFieldManager();
|
|
|
|
fFieldPropagator = fTransportManager->GetPropagatorInField();
|
|
|
|
// Need to SetFieldChangesEnergy to account for a time varying electric
|
|
// field (r.f. fields)
|
|
fFieldManager->SetFieldChangesEnergy(true);
|
|
|
|
// Set the field
|
|
fFieldManager->SetDetectorField(this);
|
|
|
|
// Choose a stepper for integration of the equation of motion
|
|
SetStepper();
|
|
|
|
// Create a cord finder providing the (global field, min step length,
|
|
// a pointer to the stepper)
|
|
fChordFinder = new G4ChordFinder((G4MagneticField*)this,minStep,fStepper);
|
|
|
|
// Set accuracy parameters
|
|
fChordFinder->SetDeltaChord( deltaChord );
|
|
|
|
fFieldManager->SetAccuraciesWithDeltaOneStep(deltaOneStep);
|
|
|
|
fFieldManager->SetDeltaIntersection(deltaIntersection);
|
|
|
|
fFieldPropagator->SetMinimumEpsilonStep(epsMin);
|
|
fFieldPropagator->SetMaximumEpsilonStep(epsMax);
|
|
|
|
G4cout << "Accuracy Parameters:" <<
|
|
" MinStep=" << minStep <<
|
|
" DeltaChord=" << deltaChord <<
|
|
" DeltaOneStep=" << deltaOneStep << G4endl;
|
|
G4cout << " " <<
|
|
" DeltaIntersection=" << deltaIntersection <<
|
|
" EpsMin=" << epsMin <<
|
|
" EpsMax=" << epsMax << G4endl;
|
|
|
|
fFieldManager->SetChordFinder(fChordFinder);
|
|
|
|
}
|
|
|
|
F04GlobalField* F04GlobalField::getObject()
|
|
{
|
|
if (!object) new F04GlobalField();
|
|
return object;
|
|
}
|
|
|
|
void F04GlobalField::SetStepper()
|
|
{
|
|
if(fStepper) delete fStepper;
|
|
|
|
switch ( fStepperType )
|
|
{
|
|
case 0:
|
|
// fStepper = new G4ExplicitEuler( fEquation, 8 ); // no spin tracking
|
|
fStepper = new G4ExplicitEuler( fEquation, 12 ); // with spin tracking
|
|
G4cout << "G4ExplicitEuler is called" << G4endl;
|
|
break;
|
|
case 1:
|
|
// fStepper = new G4ImplicitEuler( fEquation, 8 ); // no spin tracking
|
|
fStepper = new G4ImplicitEuler( fEquation, 12 ); // with spin tracking
|
|
G4cout << "G4ImplicitEuler is called" << G4endl;
|
|
break;
|
|
case 2:
|
|
// fStepper = new G4SimpleRunge( fEquation, 8 ); // no spin tracking
|
|
fStepper = new G4SimpleRunge( fEquation, 12 ); // with spin tracking
|
|
G4cout << "G4SimpleRunge is called" << G4endl;
|
|
break;
|
|
case 3:
|
|
// fStepper = new G4SimpleHeum( fEquation, 8 ); // no spin tracking
|
|
fStepper = new G4SimpleHeum( fEquation, 12 ); // with spin tracking
|
|
G4cout << "G4SimpleHeum is called" << G4endl;
|
|
break;
|
|
case 4:
|
|
// fStepper = new G4ClassicalRK4( fEquation, 8 ); // no spin tracking
|
|
fStepper = new G4ClassicalRK4( fEquation, 12 ); // with spin tracking
|
|
G4cout << "G4ClassicalRK4 (default) is called" << G4endl;
|
|
break;
|
|
case 5:
|
|
// fStepper = new G4CashKarpRKF45( fEquation, 8 ); // no spin tracking
|
|
fStepper = new G4CashKarpRKF45( fEquation, 12 ); // with spin tracking
|
|
G4cout << "G4CashKarpRKF45 is called" << G4endl;
|
|
break;
|
|
default: fStepper = 0;
|
|
}
|
|
}
|
|
|
|
G4FieldManager* F04GlobalField::GetGlobalFieldManager()
|
|
{
|
|
return G4TransportationManager::GetTransportationManager()
|
|
->GetFieldManager();
|
|
}
|
|
|
|
void F04GlobalField::GetFieldValue(const G4double* point, G4double* field) const
|
|
{
|
|
// NOTE: this routine dominates the CPU time for tracking.
|
|
// Using the simple array fp[] instead of fields[]
|
|
// directly sped it up
|
|
|
|
field[0] = field[1] = field[2] = field[3] = field[4] = field[5] = 0.0;
|
|
|
|
// protect against Geant4 bug that calls us with point[] NaN.
|
|
if(point[0] != point[0]) return;
|
|
|
|
// (can't use nfp or fp, as they may change)
|
|
if (first) ((F04GlobalField*)this)->setupArray(); // (cast away const)
|
|
|
|
for (int i=0; i<nfp; ++i) {
|
|
const F04ElementField* p = fp[i];
|
|
if (p->isInBoundingBox(point)) {
|
|
p->addFieldValue(point,field);
|
|
}
|
|
}
|
|
|
|
}
|
|
|
|
void F04GlobalField::clear()
|
|
{
|
|
if (fields) {
|
|
if (fields->size()>0) {
|
|
FieldList::iterator i;
|
|
for (i=fields->begin(); i!=fields->end(); ++i) delete *i;
|
|
fields->clear();
|
|
}
|
|
}
|
|
|
|
if (fp) delete[] fp;
|
|
|
|
first = true;
|
|
|
|
nfp = 0;
|
|
fp = NULL;
|
|
}
|
|
|
|
void F04GlobalField::setupArray()
|
|
{
|
|
first = false;
|
|
nfp = fields->size();
|
|
fp = new const F04ElementField* [nfp+1]; // add 1 so it's never 0
|
|
for (int i=0; i<nfp; ++i) fp[i] = (*fields)[i];
|
|
}
|