| 1 | //
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| 2 | // ********************************************************************
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| 3 | // * License and Disclaimer *
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| 4 | // * *
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of *
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and *
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| 7 | // * conditions of the Geant4 Software License, included in the file *
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These *
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| 9 | // * include a list of copyright holders. *
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| 10 | // * *
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| 11 | // * Neither the authors of this software system, nor their employing *
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| 12 | // * institutes,nor the agencies providing financial support for this *
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| 13 | // * work make any representation or warranty, express or implied, *
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| 14 | // * regarding this software system or assume any liability for its *
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| 15 | // * use. Please see the license in the file LICENSE and URL above *
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| 16 | // * for the full disclaimer and the limitation of liability. *
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| 17 | // * *
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| 18 | // * This code implementation is the result of the scientific and *
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| 19 | // * technical work of the GEANT4 collaboration. *
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| 20 | // * By using, copying, modifying or distributing the software (or *
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| 21 | // * any work based on the software) you agree to acknowledge its *
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| 22 | // * use in resulting scientific publications, and indicate your *
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| 23 | // * acceptance of all terms of the Geant4 Software license. *
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| 24 | // ********************************************************************
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| 25 | //
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| 26 | //
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| 27 | // $Id: G4PropagatorInField.hh,v 1.13 2007/06/08 09:49:34 gcosmo Exp $
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| 28 | // GEANT4 tag $Name: $
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| 29 | //
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| 30 | // class G4PropagatorInField
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| 31 | //
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| 32 | // Class description:
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| 33 | //
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| 34 | // This class performs the navigation/propagation of a particle/track
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| 35 | // in a magnetic field. The field is in general non-uniform.
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| 36 | // For the calculation of the path, it relies on the class G4ChordFinder.
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| 37 | //
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| 38 | // Key Method:
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| 39 | // ComputeStep(..)
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| 40 | // History:
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| 41 | // -------
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| 42 | // 25.10.96 John Apostolakis, design and implementation
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| 43 | // 25.03.97 John Apostolakis, adaptation for G4Transportation and cleanup
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| 44 | // 8.11.02 John Apostolakis, changes to enable use of safety in intersecting
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| 45 | // ---------------------------------------------------------------------------
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| 46 |
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| 47 | #ifndef G4PropagatorInField_hh
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| 48 | #define G4PropagatorInField_hh 1
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| 49 |
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| 50 | #include "G4Types.hh"
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| 51 |
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| 52 | #include <vector>
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| 53 |
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| 54 | #include "G4FieldTrack.hh"
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| 55 | #include "G4FieldManager.hh"
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| 56 | class G4ChordFinder;
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| 57 |
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| 58 | class G4Navigator;
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| 59 | class G4VPhysicalVolume;
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| 60 | class G4VCurvedTrajectoryFilter;
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| 61 |
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| 62 | class G4PropagatorInField
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| 63 | {
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| 64 |
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| 65 | public: // with description
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| 66 |
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| 67 | G4PropagatorInField( G4Navigator *theNavigator,
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| 68 | G4FieldManager *detectorFieldMgr );
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| 69 | ~G4PropagatorInField();
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| 70 |
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| 71 | G4double ComputeStep( G4FieldTrack &pFieldTrack,
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| 72 | G4double pCurrentProposedStepLength,
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| 73 | G4double &pNewSafety,
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| 74 | G4VPhysicalVolume *pPhysVol=0 );
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| 75 | // Compute the next geometric Step
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| 76 |
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| 77 | inline G4ThreeVector EndPosition() const;
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| 78 | inline G4ThreeVector EndMomentumDir() const;
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| 79 | inline G4bool IsParticleLooping() const;
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| 80 | // Return the state after the Step
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| 81 |
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| 82 | inline G4double GetEpsilonStep() const;
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| 83 | // Relative accuracy for current Step (Calc.)
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| 84 | inline void SetEpsilonStep(G4double newEps);
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| 85 | // The ratio DeltaOneStep()/h_current_step
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| 86 |
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| 87 | inline void SetChargeMomentumMass( G4double charge, // in e+ units
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| 88 | G4double momentum, // in Geant4 units
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| 89 | G4double pMass );
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| 90 | // Inform this and all associated classes of q, p, m
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| 91 |
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| 92 | G4FieldManager* FindAndSetFieldManager(G4VPhysicalVolume* pCurrentPhysVol);
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| 93 | // Set (and return) the correct field manager (global or local),
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| 94 | // if it exists.
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| 95 | // Should be called before ComputeStep is called;
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| 96 | // - currently, ComputeStep will call it, if it has not been called.
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| 97 |
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| 98 | inline G4ChordFinder* GetChordFinder();
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| 99 |
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| 100 | G4int SetVerboseLevel( G4int verbose );
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| 101 | inline G4int GetVerboseLevel() const;
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| 102 | inline G4int Verbose() const;
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| 103 |
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| 104 | inline G4int GetMaxLoopCount() const;
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| 105 | inline void SetMaxLoopCount( G4int new_max );
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| 106 | // A maximum for the number of steps that a (looping) particle can take.
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| 107 |
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| 108 | void printStatus( const G4FieldTrack& startFT,
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| 109 | const G4FieldTrack& currentFT,
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| 110 | G4double requestStep,
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| 111 | G4double safety,
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| 112 | G4int step,
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| 113 | G4VPhysicalVolume* startVolume);
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| 114 | // Print Method - useful mostly for debugging.
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| 115 |
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| 116 | inline G4FieldTrack GetEndState() const;
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| 117 |
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| 118 | // The following methods are now obsolescent but *for now* will work
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| 119 | // They are being replaced by same-name methods in G4FieldManager,
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| 120 | // allowing the specialisation in different volumes.
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| 121 | // Their new behaviour is to change the values for the global field manager.
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| 122 | inline G4double GetMinimumEpsilonStep() const;
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| 123 | inline void SetMinimumEpsilonStep( G4double newEpsMin );
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| 124 | // Minimum for Relative accuracy of any Step
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| 125 |
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| 126 | inline G4double GetMaximumEpsilonStep() const;
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| 127 | inline void SetMaximumEpsilonStep( G4double newEpsMax );
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| 128 |
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| 129 | inline void SetLargestAcceptableStep( G4double newBigDist );
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| 130 | inline G4double GetLargestAcceptableStep();
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| 131 |
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| 132 | public: // with description
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| 133 |
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| 134 | // The following methods are obsolete and will not work --
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| 135 | // as they have been replaced by the same methods in G4FieldManager
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| 136 | // since Geant4 4.0
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| 137 | inline G4double GetDeltaIntersection() const;
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| 138 | inline G4double GetDeltaOneStep() const;
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| 139 | inline void SetAccuraciesWithDeltaOneStep( G4double deltaOneStep );
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| 140 | inline void SetDeltaIntersection( G4double deltaIntersection );
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| 141 | inline void SetDeltaOneStep( G4double deltaOneStep );
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| 142 |
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| 143 | public: // without description
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| 144 |
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| 145 | inline G4FieldManager* GetCurrentFieldManager();
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| 146 | inline void SetNavigatorForPropagating( G4Navigator *SimpleOrMultiNavigator );
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| 147 | inline G4Navigator* GetNavigatorForPropagating();
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| 148 |
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| 149 | public: // no description
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| 150 |
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| 151 | inline void SetThresholdNoZeroStep( G4int noAct,
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| 152 | G4int noHarsh,
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| 153 | G4int noAbandon );
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| 154 | inline G4int GetThresholdNoZeroSteps( G4int i );
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| 155 |
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| 156 | public: // with description
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| 157 | //
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| 158 | void SetTrajectoryFilter(G4VCurvedTrajectoryFilter* filter);
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| 159 | // Set the filter that examines & stores 'intermediate'
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| 160 | // curved trajectory points. Currently only position is stored.
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| 161 |
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| 162 | std::vector<G4ThreeVector>* GimmeTrajectoryVectorAndForgetIt() const;
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| 163 | // Access the points which have passed by the filter.
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| 164 | // Responsibility for deleting the points lies with the client.
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| 165 | // This method MUST BE called exactly ONCE per step.
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| 166 |
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| 167 | void ClearPropagatorState();
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| 168 | // Clear all the State of this class and its current associates
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| 169 | // --> the current field manager & chord finder will also be called
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| 170 |
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| 171 | inline void SetDetectorFieldManager( G4FieldManager* newGlobalFieldManager );
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| 172 | // Update this (dangerous) state -- for the time being
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| 173 |
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| 174 | inline void SetUseSafetyForOptimization( G4bool );
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| 175 | inline G4bool GetUseSafetyForOptimization();
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| 176 | // Toggle & view parameter for using safety to discard
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| 177 | // unneccesary calls to navigator (thus 'optimising' performance)
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| 178 |
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| 179 | protected: // with description
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| 180 |
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| 181 | G4bool LocateIntersectionPoint(
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| 182 | const G4FieldTrack& curveStartPointTangent, // A
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| 183 | const G4FieldTrack& curveEndPointTangent, // B
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| 184 | const G4ThreeVector& trialPoint, // E
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| 185 | G4FieldTrack& intersectPointTangent, // Output
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| 186 | G4bool& recalculatedEndPoint); // Out:
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| 187 |
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| 188 | // If such an intersection exists, this function
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| 189 | // calculate the intersection point of the true path of the particle
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| 190 | // with the surface of the current volume (or of one of its daughters).
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| 191 | // (Should use lateral displacement as measure of convergence).
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| 192 |
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| 193 | G4bool IntersectChord( G4ThreeVector StartPointA,
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| 194 | G4ThreeVector EndPointB,
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| 195 | G4double &NewSafety,
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| 196 | G4double &LinearStepLength,
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| 197 | G4ThreeVector &IntersectionPoint);
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| 198 | // Intersect the chord from StartPointA to EndPointB
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| 199 | // and return whether an intersection occurred
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| 200 |
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| 201 | G4FieldTrack ReEstimateEndpoint( const G4FieldTrack &CurrentStateA,
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| 202 | const G4FieldTrack &EstimtdEndStateB,
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| 203 | G4double linearDistSq,
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| 204 | G4double curveDist);
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| 205 | // Return new estimate for state after curveDist
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| 206 | // starting from CurrentStateA, to replace EstimtdEndStateB,
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| 207 | // (and report displacement -- if field is compiled verbose.)
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| 208 |
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| 209 | void PrintStepLengthDiagnostic( G4double currentProposedStepLength,
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| 210 | G4double decreaseFactor,
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| 211 | G4double stepTrial,
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| 212 | const G4FieldTrack& aFieldTrack);
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| 213 | private:
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| 214 |
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| 215 | // ----------------------------------------------------------------------
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| 216 | // DATA Members
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| 217 | // ----------------------------------------------------------------------
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| 218 |
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| 219 | G4FieldManager *fDetectorFieldMgr;
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| 220 | // The Field Manager of the whole Detector. (default)
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| 221 |
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| 222 | G4FieldManager *fCurrentFieldMgr;
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| 223 | // The Field Manager of the current volume (may be the one above.)
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| 224 |
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| 225 | G4Navigator *fNavigator;
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| 226 |
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| 227 | // STATE information
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| 228 | // -----------------
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| 229 |
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| 230 | G4double fEpsilonStep;
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| 231 | // Relative accuracy for current Step (Calc.)
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| 232 |
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| 233 | G4FieldTrack End_PointAndTangent;
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| 234 | // End point storage
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| 235 |
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| 236 | G4bool fParticleIsLooping;
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| 237 |
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| 238 | G4int fVerboseLevel;
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| 239 | // For debuging purposes
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| 240 |
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| 241 | G4int fMax_loop_count;
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| 242 | // Limit for the number of sub-steps taken in one call to ComputeStep
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| 243 |
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| 244 | // Variables to keep track of "abnormal" case - which causes loop
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| 245 | //
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| 246 | G4int fNoZeroStep; // Counter of zeroStep
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| 247 | G4int fActionThreshold_NoZeroSteps; // Threshold: above this - act
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| 248 | G4int fSevereActionThreshold_NoZeroSteps; // Threshold to act harshly
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| 249 | G4int fAbandonThreshold_NoZeroSteps; // Threshold to abandon
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| 250 |
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| 251 | G4double fFull_CurveLen_of_LastAttempt;
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| 252 | G4double fLast_ProposedStepLength;
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| 253 | G4double fLargestAcceptableStep;
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| 254 |
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| 255 | G4double fCharge, fInitialMomentumModulus, fMass;
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| 256 |
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| 257 | G4ThreeVector fPreviousSftOrigin;
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| 258 | G4double fPreviousSafety;
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| 259 | G4bool fUseSafetyForOptimisation;
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| 260 | // Last safety origin & value: for optimisation
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| 261 |
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| 262 | G4bool fSetFieldMgr;
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| 263 | // Flag whether field manager has been set for the current step
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| 264 |
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| 265 | G4double kCarTolerance;
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| 266 | // Geometrical tolerance defining surface thickness
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| 267 |
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| 268 | private:
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| 269 |
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| 270 | static const G4int max_depth=4;
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| 271 | G4FieldTrack* ptrInterMedFT[max_depth+1];
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| 272 | // Used to store intermediate values of tracks in case of
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| 273 | // too slow progress
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| 274 |
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| 275 | private:
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| 276 |
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| 277 | G4VCurvedTrajectoryFilter* fpTrajectoryFilter;
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| 278 | // The filter encapsulates the algorithm which selects which
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| 279 | // intermediate points should be stored in a trajectory.
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| 280 | // When it is NULL, no intermediate points will be stored.
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| 281 | // Else PIF::ComputeStep must submit (all) intermediate
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| 282 | // points it calculates, to this filter. (jacek 04/11/2002)
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| 283 | };
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| 284 |
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| 285 | // ********************************************************************
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| 286 | // Inline methods.
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| 287 | // ********************************************************************
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| 288 |
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| 289 | #include "G4PropagatorInField.icc"
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| 290 |
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| 291 | #endif
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