source: trunk/source/geometry/navigation/include/G4PropagatorInField.icc @ 847

//
// ********************************************************************
// * 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: G4PropagatorInField.icc,v 1.10 2006/11/13 17:34:08 gcosmo Exp $
// GEANT4 tag $Name:  $
//
// 
// ------------------------------------------------------------------------
//  GEANT 4  inline implementation
//
// ------------------------------------------------------------------------
// 
// 25.10.96 John Apostolakis, design and implementation 
// 25.03.97 John Apostolakis, adaptation for G4Transportation and cleanup
//
//  To create an object of this type, must have:
//  - an object that calculates the Curved paths 
//  - the navigator to find (linear) intersections
//  - and ?? also must know the value of the maximum displacement allowed
// ------------------------------------------------------------------------

inline
G4ChordFinder* G4PropagatorInField::GetChordFinder()
{
  // The "Chord Finder" of the current Field Mgr is used
  //    -- this could be of the global field manager
  //        or that of another, from the current volume 
  return fCurrentFieldMgr->GetChordFinder(); 
}

inline
void G4PropagatorInField::SetChargeMomentumMass( 
            G4double Charge,            // in e+ units
            G4double Momentum,          // in GeV/c 
            G4double Mass)              // in ? units
{
  // GetChordFinder()->SetChargeMomentumMass(Charge, Momentum, Mass);
  //  --> Not needed anymore, as it is done in ComputeStep for the 
  //       ChordFinder of the current step (which is known only then).
  fCharge = Charge;
  fInitialMomentumModulus = Momentum;
  fMass = Mass; 
}

//  Obtain the final space-point and velocity (normal) at the end of the Step
//
inline
G4ThreeVector  G4PropagatorInField::EndPosition() const
{
  return   End_PointAndTangent.GetPosition(); 
}

inline
G4ThreeVector  G4PropagatorInField::EndMomentumDir() const
{
  return   End_PointAndTangent.GetMomentumDir(); 
}

inline
G4double G4PropagatorInField::GetEpsilonStep() const
{ 
  return fEpsilonStep; 
}

inline
void     G4PropagatorInField::SetEpsilonStep( G4double newEps )
{
  fEpsilonStep=newEps;
}

inline
G4bool   G4PropagatorInField::IsParticleLooping() const
{
  return fParticleIsLooping;
}

inline
G4int    G4PropagatorInField::GetMaxLoopCount() const
{
  return fMax_loop_count;
}

inline
void     G4PropagatorInField::SetMaxLoopCount( G4int new_max ) 
{
  fMax_loop_count = new_max;
}

inline
G4double G4PropagatorInField::GetDeltaIntersection() const
{
  return fCurrentFieldMgr->GetDeltaIntersection();
} 

inline
G4double G4PropagatorInField::GetDeltaOneStep() const
{
  return fCurrentFieldMgr->GetDeltaOneStep();
}

inline
void
G4PropagatorInField::SetAccuraciesWithDeltaOneStep( G4double valDeltaOneStep )
{ 
  fDetectorFieldMgr->SetAccuraciesWithDeltaOneStep(valDeltaOneStep);
}

inline
void G4PropagatorInField::SetDeltaOneStep( G4double valDeltaOneStep )
{ 
  fDetectorFieldMgr->SetDeltaOneStep(valDeltaOneStep); 
}

inline
void G4PropagatorInField::SetDeltaIntersection( G4double valDeltaIntersection )
{
  fDetectorFieldMgr->SetDeltaIntersection(valDeltaIntersection);
}

inline
G4int G4PropagatorInField::GetVerboseLevel() const
{
  return fVerboseLevel;
}

inline
G4int G4PropagatorInField::Verbose() const     // Obsolete
{
  return GetVerboseLevel();
}

inline
G4FieldTrack G4PropagatorInField::GetEndState() const
{
  return End_PointAndTangent;
}

// Minimum for Relative accuracy of a Step in volumes of global field
inline 
G4double  G4PropagatorInField::GetMinimumEpsilonStep() const
{
  return fDetectorFieldMgr->GetMinimumEpsilonStep();
}

inline 
void      G4PropagatorInField::SetMinimumEpsilonStep( G4double newEpsMin )
{
  fDetectorFieldMgr->SetMinimumEpsilonStep(newEpsMin);
}

// Maximum for Relative accuracy of any Step 
inline 
G4double  G4PropagatorInField::GetMaximumEpsilonStep() const
{
  return fDetectorFieldMgr->GetMaximumEpsilonStep();
}

inline 
void      G4PropagatorInField::SetMaximumEpsilonStep( G4double newEpsMax )
{
  fDetectorFieldMgr->SetMaximumEpsilonStep( newEpsMax );
}

inline
void G4PropagatorInField::SetLargestAcceptableStep( G4double newBigDist )
{
  if( fLargestAcceptableStep>0.0 )
  {
    fLargestAcceptableStep = newBigDist;
  }
}

inline
G4double  G4PropagatorInField::GetLargestAcceptableStep()
{
  return fLargestAcceptableStep;
}

inline
G4FieldManager*  G4PropagatorInField::GetCurrentFieldManager()
{
  return fCurrentFieldMgr;
} 

inline
void G4PropagatorInField::SetThresholdNoZeroStep( G4int noAct,
                                                  G4int noHarsh,
                                                  G4int noAbandon )
{
  if( noAct>0 ) 
    fActionThreshold_NoZeroSteps = noAct; 

  if( noHarsh > fActionThreshold_NoZeroSteps )
    fSevereActionThreshold_NoZeroSteps = noHarsh; 
  else
    fSevereActionThreshold_NoZeroSteps = 2*(fActionThreshold_NoZeroSteps+1);

  if( noAbandon > fSevereActionThreshold_NoZeroSteps+5 )
    fAbandonThreshold_NoZeroSteps = noAbandon; 
  else
    fAbandonThreshold_NoZeroSteps = 2*(fSevereActionThreshold_NoZeroSteps+3); 
}

inline
G4int G4PropagatorInField::GetThresholdNoZeroSteps( G4int i )
{
   G4int t=0;
   if( i==0 )     { t = 3; }     // No of parameters
   else if (i==1) { t = fActionThreshold_NoZeroSteps; }
   else if (i==2) { t = fSevereActionThreshold_NoZeroSteps; }
   else if (i==3) { t = fAbandonThreshold_NoZeroSteps; }

   return t;
}

inline
void G4PropagatorInField::SetDetectorFieldManager(G4FieldManager* newDetectorFieldManager)
{
   fDetectorFieldMgr = newDetectorFieldManager; 
}

  
inline
void  G4PropagatorInField:: SetUseSafetyForOptimization( G4bool value )
{
   fUseSafetyForOptimisation= value;
}

inline 
G4bool G4PropagatorInField::GetUseSafetyForOptimization() 
{ 
   return fUseSafetyForOptimisation; 
}

inline 
void G4PropagatorInField::
SetNavigatorForPropagating( G4Navigator *SimpleOrMultiNavigator )
{
  if(SimpleOrMultiNavigator)  { fNavigator= SimpleOrMultiNavigator; }
}

inline
G4Navigator* G4PropagatorInField::GetNavigatorForPropagating()
{
  return fNavigator;
}