[819] | 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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[961] | 27 | // $Id: G4Cerenkov.cc,v 1.26 2008/11/14 20:16:51 gum Exp $ |
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[1007] | 28 | // GEANT4 tag $Name: geant4-09-02 $ |
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[819] | 29 | // |
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| 30 | //////////////////////////////////////////////////////////////////////// |
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| 31 | // Cerenkov Radiation Class Implementation |
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| 32 | //////////////////////////////////////////////////////////////////////// |
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| 33 | // |
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| 34 | // File: G4Cerenkov.cc |
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| 35 | // Description: Discrete Process -- Generation of Cerenkov Photons |
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| 36 | // Version: 2.1 |
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| 37 | // Created: 1996-02-21 |
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| 38 | // Author: Juliet Armstrong |
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| 39 | // Updated: 2007-09-30 by Peter Gumplinger |
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| 40 | // > change inheritance to G4VDiscreteProcess |
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| 41 | // GetContinuousStepLimit -> GetMeanFreePath (StronglyForced) |
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| 42 | // AlongStepDoIt -> PostStepDoIt |
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| 43 | // 2005-08-17 by Peter Gumplinger |
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| 44 | // > change variable name MeanNumPhotons -> MeanNumberOfPhotons |
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| 45 | // 2005-07-28 by Peter Gumplinger |
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| 46 | // > add G4ProcessType to constructor |
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| 47 | // 2001-09-17, migration of Materials to pure STL (mma) |
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| 48 | // 2000-11-12 by Peter Gumplinger |
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| 49 | // > add check on CerenkovAngleIntegrals->IsFilledVectorExist() |
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| 50 | // in method GetAverageNumberOfPhotons |
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| 51 | // > and a test for MeanNumberOfPhotons <= 0.0 in DoIt |
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| 52 | // 2000-09-18 by Peter Gumplinger |
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| 53 | // > change: aSecondaryPosition=x0+rand*aStep.GetDeltaPosition(); |
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| 54 | // aSecondaryTrack->SetTouchable(0); |
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| 55 | // 1999-10-29 by Peter Gumplinger |
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| 56 | // > change: == into <= in GetContinuousStepLimit |
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| 57 | // 1997-08-08 by Peter Gumplinger |
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| 58 | // > add protection against /0 |
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| 59 | // > G4MaterialPropertiesTable; new physics/tracking scheme |
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| 60 | // |
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| 61 | // mail: gum@triumf.ca |
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| 62 | // |
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| 63 | //////////////////////////////////////////////////////////////////////// |
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| 64 | |
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| 65 | #include "G4ios.hh" |
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| 66 | #include "G4Poisson.hh" |
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[961] | 67 | #include "G4EmProcessSubType.hh" |
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| 68 | |
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| 69 | #include "G4LossTableManager.hh" |
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| 70 | #include "G4MaterialCutsCouple.hh" |
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| 71 | #include "G4ParticleDefinition.hh" |
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| 72 | |
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[819] | 73 | #include "G4Cerenkov.hh" |
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| 74 | |
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| 75 | using namespace std; |
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| 76 | |
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| 77 | ///////////////////////// |
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| 78 | // Class Implementation |
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| 79 | ///////////////////////// |
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| 80 | |
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| 81 | ////////////// |
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| 82 | // Operators |
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| 83 | ////////////// |
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| 84 | |
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| 85 | // G4Cerenkov::operator=(const G4Cerenkov &right) |
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| 86 | // { |
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| 87 | // } |
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| 88 | |
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| 89 | ///////////////// |
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| 90 | // Constructors |
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| 91 | ///////////////// |
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| 92 | |
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| 93 | G4Cerenkov::G4Cerenkov(const G4String& processName, G4ProcessType type) |
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[961] | 94 | : G4VProcess(processName, type) |
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[819] | 95 | { |
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| 96 | G4cout << "G4Cerenkov::G4Cerenkov constructor" << G4endl; |
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[961] | 97 | G4cout << "NOTE: this is now a G4VProcess!" << G4endl; |
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[819] | 98 | G4cout << "Required change in UserPhysicsList: " << G4endl; |
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| 99 | G4cout << "change: pmanager->AddContinuousProcess(theCerenkovProcess);" << G4endl; |
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| 100 | G4cout << "to: pmanager->AddProcess(theCerenkovProcess);" << G4endl; |
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| 101 | G4cout << " pmanager->SetProcessOrdering(theCerenkovProcess,idxPostStep);" << G4endl; |
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| 102 | |
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[961] | 103 | SetProcessSubType(fCerenkov); |
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| 104 | |
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[819] | 105 | fTrackSecondariesFirst = false; |
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[961] | 106 | fMaxBetaChange = 0.; |
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[819] | 107 | fMaxPhotons = 0; |
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| 108 | |
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| 109 | thePhysicsTable = NULL; |
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| 110 | |
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| 111 | if (verboseLevel>0) { |
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| 112 | G4cout << GetProcessName() << " is created " << G4endl; |
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| 113 | } |
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| 114 | |
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| 115 | BuildThePhysicsTable(); |
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| 116 | } |
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| 117 | |
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| 118 | // G4Cerenkov::G4Cerenkov(const G4Cerenkov &right) |
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| 119 | // { |
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| 120 | // } |
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| 121 | |
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| 122 | //////////////// |
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| 123 | // Destructors |
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| 124 | //////////////// |
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| 125 | |
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| 126 | G4Cerenkov::~G4Cerenkov() |
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| 127 | { |
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| 128 | if (thePhysicsTable != NULL) { |
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| 129 | thePhysicsTable->clearAndDestroy(); |
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| 130 | delete thePhysicsTable; |
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| 131 | } |
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| 132 | } |
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| 133 | |
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| 134 | //////////// |
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| 135 | // Methods |
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| 136 | //////////// |
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| 137 | |
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| 138 | // PostStepDoIt |
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| 139 | // ------------- |
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| 140 | // |
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| 141 | G4VParticleChange* |
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| 142 | G4Cerenkov::PostStepDoIt(const G4Track& aTrack, const G4Step& aStep) |
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| 143 | |
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| 144 | // This routine is called for each tracking Step of a charged particle |
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| 145 | // in a radiator. A Poisson-distributed number of photons is generated |
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| 146 | // according to the Cerenkov formula, distributed evenly along the track |
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| 147 | // segment and uniformly azimuth w.r.t. the particle direction. The |
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| 148 | // parameters are then transformed into the Master Reference System, and |
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| 149 | // they are added to the particle change. |
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| 150 | |
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| 151 | { |
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| 152 | ////////////////////////////////////////////////////// |
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| 153 | // Should we ensure that the material is dispersive? |
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| 154 | ////////////////////////////////////////////////////// |
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| 155 | |
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| 156 | aParticleChange.Initialize(aTrack); |
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| 157 | |
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| 158 | const G4DynamicParticle* aParticle = aTrack.GetDynamicParticle(); |
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| 159 | const G4Material* aMaterial = aTrack.GetMaterial(); |
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| 160 | |
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| 161 | G4StepPoint* pPreStepPoint = aStep.GetPreStepPoint(); |
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| 162 | G4StepPoint* pPostStepPoint = aStep.GetPostStepPoint(); |
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| 163 | |
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| 164 | G4ThreeVector x0 = pPreStepPoint->GetPosition(); |
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| 165 | G4ThreeVector p0 = aStep.GetDeltaPosition().unit(); |
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| 166 | G4double t0 = pPreStepPoint->GetGlobalTime(); |
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| 167 | |
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| 168 | G4MaterialPropertiesTable* aMaterialPropertiesTable = |
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| 169 | aMaterial->GetMaterialPropertiesTable(); |
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[961] | 170 | if (!aMaterialPropertiesTable) return pParticleChange; |
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[819] | 171 | |
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| 172 | const G4MaterialPropertyVector* Rindex = |
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| 173 | aMaterialPropertiesTable->GetProperty("RINDEX"); |
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[961] | 174 | if (!Rindex) return pParticleChange; |
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[819] | 175 | |
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| 176 | // particle charge |
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| 177 | const G4double charge = aParticle->GetDefinition()->GetPDGCharge(); |
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| 178 | |
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| 179 | // particle beta |
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| 180 | const G4double beta = (pPreStepPoint ->GetBeta() + |
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| 181 | pPostStepPoint->GetBeta())/2.; |
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| 182 | |
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| 183 | G4double MeanNumberOfPhotons = |
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| 184 | GetAverageNumberOfPhotons(charge,beta,aMaterial,Rindex); |
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| 185 | |
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| 186 | if (MeanNumberOfPhotons <= 0.0) { |
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| 187 | |
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| 188 | // return unchanged particle and no secondaries |
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| 189 | |
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| 190 | aParticleChange.SetNumberOfSecondaries(0); |
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| 191 | |
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[961] | 192 | return pParticleChange; |
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[819] | 193 | |
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| 194 | } |
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| 195 | |
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| 196 | G4double step_length; |
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| 197 | step_length = aStep.GetStepLength(); |
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| 198 | |
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| 199 | MeanNumberOfPhotons = MeanNumberOfPhotons * step_length; |
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| 200 | |
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| 201 | G4int NumPhotons = (G4int) G4Poisson(MeanNumberOfPhotons); |
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| 202 | |
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| 203 | if (NumPhotons <= 0) { |
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| 204 | |
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| 205 | // return unchanged particle and no secondaries |
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| 206 | |
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| 207 | aParticleChange.SetNumberOfSecondaries(0); |
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| 208 | |
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[961] | 209 | return pParticleChange; |
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[819] | 210 | } |
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| 211 | |
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| 212 | //////////////////////////////////////////////////////////////// |
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| 213 | |
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| 214 | aParticleChange.SetNumberOfSecondaries(NumPhotons); |
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| 215 | |
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| 216 | if (fTrackSecondariesFirst) { |
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| 217 | if (aTrack.GetTrackStatus() == fAlive ) |
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| 218 | aParticleChange.ProposeTrackStatus(fSuspend); |
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| 219 | } |
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| 220 | |
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| 221 | //////////////////////////////////////////////////////////////// |
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| 222 | |
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[961] | 223 | G4double Pmin = Rindex->GetMinPhotonEnergy(); |
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| 224 | G4double Pmax = Rindex->GetMaxPhotonEnergy(); |
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[819] | 225 | G4double dp = Pmax - Pmin; |
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| 226 | |
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| 227 | G4double nMax = Rindex->GetMaxProperty(); |
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| 228 | |
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| 229 | G4double BetaInverse = 1./beta; |
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| 230 | |
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| 231 | G4double maxCos = BetaInverse / nMax; |
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| 232 | G4double maxSin2 = (1.0 - maxCos) * (1.0 + maxCos); |
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| 233 | |
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[961] | 234 | const G4double beta1 = pPreStepPoint ->GetBeta(); |
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| 235 | const G4double beta2 = pPostStepPoint->GetBeta(); |
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| 236 | |
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| 237 | G4double MeanNumberOfPhotons1 = |
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| 238 | GetAverageNumberOfPhotons(charge,beta1,aMaterial,Rindex); |
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| 239 | G4double MeanNumberOfPhotons2 = |
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| 240 | GetAverageNumberOfPhotons(charge,beta2,aMaterial,Rindex); |
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| 241 | |
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[819] | 242 | for (G4int i = 0; i < NumPhotons; i++) { |
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| 243 | |
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[961] | 244 | // Determine photon energy |
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[819] | 245 | |
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| 246 | G4double rand; |
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[961] | 247 | G4double sampledEnergy, sampledRI; |
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[819] | 248 | G4double cosTheta, sin2Theta; |
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| 249 | |
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[961] | 250 | // sample an energy |
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[819] | 251 | |
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| 252 | do { |
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| 253 | rand = G4UniformRand(); |
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[961] | 254 | sampledEnergy = Pmin + rand * dp; |
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| 255 | sampledRI = Rindex->GetProperty(sampledEnergy); |
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[819] | 256 | cosTheta = BetaInverse / sampledRI; |
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| 257 | |
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| 258 | sin2Theta = (1.0 - cosTheta)*(1.0 + cosTheta); |
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| 259 | rand = G4UniformRand(); |
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| 260 | |
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| 261 | } while (rand*maxSin2 > sin2Theta); |
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| 262 | |
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| 263 | // Generate random position of photon on cone surface |
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| 264 | // defined by Theta |
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| 265 | |
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| 266 | rand = G4UniformRand(); |
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| 267 | |
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| 268 | G4double phi = twopi*rand; |
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| 269 | G4double sinPhi = sin(phi); |
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| 270 | G4double cosPhi = cos(phi); |
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| 271 | |
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[961] | 272 | // calculate x,y, and z components of photon energy |
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[819] | 273 | // (in coord system with primary particle direction |
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| 274 | // aligned with the z axis) |
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| 275 | |
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| 276 | G4double sinTheta = sqrt(sin2Theta); |
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| 277 | G4double px = sinTheta*cosPhi; |
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| 278 | G4double py = sinTheta*sinPhi; |
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| 279 | G4double pz = cosTheta; |
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| 280 | |
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| 281 | // Create photon momentum direction vector |
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| 282 | // The momentum direction is still with respect |
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| 283 | // to the coordinate system where the primary |
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| 284 | // particle direction is aligned with the z axis |
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| 285 | |
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| 286 | G4ParticleMomentum photonMomentum(px, py, pz); |
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| 287 | |
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| 288 | // Rotate momentum direction back to global reference |
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| 289 | // system |
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| 290 | |
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| 291 | photonMomentum.rotateUz(p0); |
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| 292 | |
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| 293 | // Determine polarization of new photon |
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| 294 | |
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| 295 | G4double sx = cosTheta*cosPhi; |
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| 296 | G4double sy = cosTheta*sinPhi; |
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| 297 | G4double sz = -sinTheta; |
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| 298 | |
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| 299 | G4ThreeVector photonPolarization(sx, sy, sz); |
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| 300 | |
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| 301 | // Rotate back to original coord system |
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| 302 | |
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| 303 | photonPolarization.rotateUz(p0); |
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| 304 | |
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| 305 | // Generate a new photon: |
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| 306 | |
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| 307 | G4DynamicParticle* aCerenkovPhoton = |
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| 308 | new G4DynamicParticle(G4OpticalPhoton::OpticalPhoton(), |
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| 309 | photonMomentum); |
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| 310 | aCerenkovPhoton->SetPolarization |
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| 311 | (photonPolarization.x(), |
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| 312 | photonPolarization.y(), |
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| 313 | photonPolarization.z()); |
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| 314 | |
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[961] | 315 | aCerenkovPhoton->SetKineticEnergy(sampledEnergy); |
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[819] | 316 | |
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| 317 | // Generate new G4Track object: |
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| 318 | |
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[961] | 319 | G4double delta, NumberOfPhotons, N; |
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[819] | 320 | |
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[961] | 321 | do { |
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| 322 | rand = G4UniformRand(); |
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| 323 | delta = rand * aStep.GetStepLength(); |
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| 324 | NumberOfPhotons = MeanNumberOfPhotons1 - delta * |
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| 325 | (MeanNumberOfPhotons1-MeanNumberOfPhotons2)/ |
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| 326 | aStep.GetStepLength(); |
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| 327 | N = G4UniformRand() * |
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| 328 | std::max(MeanNumberOfPhotons1,MeanNumberOfPhotons2); |
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| 329 | } while (N > NumberOfPhotons); |
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| 330 | |
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[819] | 331 | G4double deltaTime = delta / |
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| 332 | ((pPreStepPoint->GetVelocity()+ |
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| 333 | pPostStepPoint->GetVelocity())/2.); |
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| 334 | |
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| 335 | G4double aSecondaryTime = t0 + deltaTime; |
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| 336 | |
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| 337 | G4ThreeVector aSecondaryPosition = |
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| 338 | x0 + rand * aStep.GetDeltaPosition(); |
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| 339 | |
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| 340 | G4Track* aSecondaryTrack = |
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| 341 | new G4Track(aCerenkovPhoton,aSecondaryTime,aSecondaryPosition); |
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| 342 | |
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[961] | 343 | aSecondaryTrack->SetTouchableHandle( |
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| 344 | aStep.GetPreStepPoint()->GetTouchableHandle()); |
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[819] | 345 | |
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| 346 | aSecondaryTrack->SetParentID(aTrack.GetTrackID()); |
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| 347 | |
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| 348 | aParticleChange.AddSecondary(aSecondaryTrack); |
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| 349 | } |
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| 350 | |
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| 351 | if (verboseLevel>0) { |
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| 352 | G4cout << "\n Exiting from G4Cerenkov::DoIt -- NumberOfSecondaries = " |
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| 353 | << aParticleChange.GetNumberOfSecondaries() << G4endl; |
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| 354 | } |
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| 355 | |
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[961] | 356 | return pParticleChange; |
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[819] | 357 | } |
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| 358 | |
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| 359 | // BuildThePhysicsTable for the Cerenkov process |
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| 360 | // --------------------------------------------- |
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| 361 | // |
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| 362 | |
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| 363 | void G4Cerenkov::BuildThePhysicsTable() |
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| 364 | { |
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| 365 | if (thePhysicsTable) return; |
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| 366 | |
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| 367 | const G4MaterialTable* theMaterialTable= |
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| 368 | G4Material::GetMaterialTable(); |
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| 369 | G4int numOfMaterials = G4Material::GetNumberOfMaterials(); |
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| 370 | |
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| 371 | // create new physics table |
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| 372 | |
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| 373 | thePhysicsTable = new G4PhysicsTable(numOfMaterials); |
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| 374 | |
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| 375 | // loop for materials |
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| 376 | |
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| 377 | for (G4int i=0 ; i < numOfMaterials; i++) |
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| 378 | { |
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| 379 | G4PhysicsOrderedFreeVector* aPhysicsOrderedFreeVector = |
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| 380 | new G4PhysicsOrderedFreeVector(); |
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| 381 | |
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| 382 | // Retrieve vector of refraction indices for the material |
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| 383 | // from the material's optical properties table |
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| 384 | |
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| 385 | G4Material* aMaterial = (*theMaterialTable)[i]; |
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| 386 | |
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| 387 | G4MaterialPropertiesTable* aMaterialPropertiesTable = |
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| 388 | aMaterial->GetMaterialPropertiesTable(); |
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| 389 | |
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| 390 | if (aMaterialPropertiesTable) { |
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| 391 | |
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| 392 | G4MaterialPropertyVector* theRefractionIndexVector = |
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| 393 | aMaterialPropertiesTable->GetProperty("RINDEX"); |
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| 394 | |
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| 395 | if (theRefractionIndexVector) { |
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| 396 | |
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| 397 | // Retrieve the first refraction index in vector |
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[961] | 398 | // of (photon energy, refraction index) pairs |
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[819] | 399 | |
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| 400 | theRefractionIndexVector->ResetIterator(); |
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| 401 | ++(*theRefractionIndexVector); // advance to 1st entry |
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| 402 | |
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| 403 | G4double currentRI = theRefractionIndexVector-> |
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| 404 | GetProperty(); |
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| 405 | |
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| 406 | if (currentRI > 1.0) { |
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| 407 | |
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[961] | 408 | // Create first (photon energy, Cerenkov Integral) |
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[819] | 409 | // pair |
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| 410 | |
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| 411 | G4double currentPM = theRefractionIndexVector-> |
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[961] | 412 | GetPhotonEnergy(); |
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[819] | 413 | G4double currentCAI = 0.0; |
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| 414 | |
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| 415 | aPhysicsOrderedFreeVector-> |
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| 416 | InsertValues(currentPM , currentCAI); |
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| 417 | |
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| 418 | // Set previous values to current ones prior to loop |
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| 419 | |
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| 420 | G4double prevPM = currentPM; |
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| 421 | G4double prevCAI = currentCAI; |
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| 422 | G4double prevRI = currentRI; |
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| 423 | |
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[961] | 424 | // loop over all (photon energy, refraction index) |
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[819] | 425 | // pairs stored for this material |
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| 426 | |
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| 427 | while(++(*theRefractionIndexVector)) |
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| 428 | { |
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| 429 | currentRI=theRefractionIndexVector-> |
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| 430 | GetProperty(); |
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| 431 | |
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| 432 | currentPM = theRefractionIndexVector-> |
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[961] | 433 | GetPhotonEnergy(); |
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[819] | 434 | |
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| 435 | currentCAI = 0.5*(1.0/(prevRI*prevRI) + |
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| 436 | 1.0/(currentRI*currentRI)); |
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| 437 | |
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| 438 | currentCAI = prevCAI + |
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| 439 | (currentPM - prevPM) * currentCAI; |
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| 440 | |
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| 441 | aPhysicsOrderedFreeVector-> |
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| 442 | InsertValues(currentPM, currentCAI); |
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| 443 | |
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| 444 | prevPM = currentPM; |
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| 445 | prevCAI = currentCAI; |
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| 446 | prevRI = currentRI; |
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| 447 | } |
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| 448 | |
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| 449 | } |
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| 450 | } |
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| 451 | } |
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| 452 | |
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| 453 | // The Cerenkov integral for a given material |
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| 454 | // will be inserted in thePhysicsTable |
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| 455 | // according to the position of the material in |
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| 456 | // the material table. |
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| 457 | |
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| 458 | thePhysicsTable->insertAt(i,aPhysicsOrderedFreeVector); |
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| 459 | |
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| 460 | } |
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| 461 | } |
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| 462 | |
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| 463 | // GetMeanFreePath |
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| 464 | // --------------- |
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| 465 | // |
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| 466 | |
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[961] | 467 | G4double G4Cerenkov::GetMeanFreePath(const G4Track&, |
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[819] | 468 | G4double, |
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[961] | 469 | G4ForceCondition*) |
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| 470 | { |
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| 471 | return 1.; |
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| 472 | } |
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| 473 | |
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| 474 | G4double G4Cerenkov::PostStepGetPhysicalInteractionLength( |
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| 475 | const G4Track& aTrack, |
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| 476 | G4double, |
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[819] | 477 | G4ForceCondition* condition) |
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| 478 | { |
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[961] | 479 | *condition = NotForced; |
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| 480 | G4double StepLimit = DBL_MAX; |
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[819] | 481 | |
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| 482 | const G4DynamicParticle* aParticle = aTrack.GetDynamicParticle(); |
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| 483 | const G4Material* aMaterial = aTrack.GetMaterial(); |
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[961] | 484 | const G4MaterialCutsCouple* couple = aTrack.GetMaterialCutsCouple(); |
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[819] | 485 | |
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[961] | 486 | const G4double kineticEnergy = aParticle->GetKineticEnergy(); |
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| 487 | const G4ParticleDefinition* particleType = aParticle->GetDefinition(); |
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| 488 | const G4double mass = particleType->GetPDGMass(); |
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[819] | 489 | |
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| 490 | // particle beta |
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| 491 | const G4double beta = aParticle->GetTotalMomentum() / |
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| 492 | aParticle->GetTotalEnergy(); |
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[961] | 493 | // particle gamma |
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| 494 | const G4double gamma = 1./std::sqrt(1.-beta*beta); |
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[819] | 495 | |
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[961] | 496 | G4MaterialPropertiesTable* aMaterialPropertiesTable = |
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| 497 | aMaterial->GetMaterialPropertiesTable(); |
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[819] | 498 | |
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[961] | 499 | const G4MaterialPropertyVector* Rindex = NULL; |
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[819] | 500 | |
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[961] | 501 | if (aMaterialPropertiesTable) |
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| 502 | Rindex = aMaterialPropertiesTable->GetProperty("RINDEX"); |
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[819] | 503 | |
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[961] | 504 | G4double nMax; |
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| 505 | if (Rindex) { |
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| 506 | nMax = Rindex->GetMaxProperty(); |
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| 507 | } else { |
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| 508 | return StepLimit; |
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| 509 | } |
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| 510 | |
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| 511 | G4double BetaMin = 1./nMax; |
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| 512 | if ( BetaMin >= 1. ) return StepLimit; |
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| 513 | |
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| 514 | G4double GammaMin = 1./std::sqrt(1.-BetaMin*BetaMin); |
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| 515 | |
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| 516 | if (gamma < GammaMin ) return StepLimit; |
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| 517 | |
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| 518 | G4double kinEmin = mass*(GammaMin-1.); |
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| 519 | |
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| 520 | G4double RangeMin = G4LossTableManager::Instance()-> |
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| 521 | GetRange(particleType, |
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| 522 | kinEmin, |
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| 523 | couple); |
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| 524 | G4double Range = G4LossTableManager::Instance()-> |
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| 525 | GetRange(particleType, |
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| 526 | kineticEnergy, |
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| 527 | couple); |
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| 528 | |
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| 529 | G4double Step = Range - RangeMin; |
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| 530 | if (Step < 1.*um ) return StepLimit; |
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| 531 | |
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| 532 | if (Step > 0. && Step < StepLimit) StepLimit = Step; |
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| 533 | |
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| 534 | // If user has defined an average maximum number of photons to |
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| 535 | // be generated in a Step, then calculate the Step length for |
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| 536 | // that number of photons. |
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| 537 | |
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| 538 | if (fMaxPhotons > 0) { |
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| 539 | |
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| 540 | // particle charge |
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| 541 | const G4double charge = aParticle-> |
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| 542 | GetDefinition()->GetPDGCharge(); |
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| 543 | |
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| 544 | G4double MeanNumberOfPhotons = |
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| 545 | GetAverageNumberOfPhotons(charge,beta,aMaterial,Rindex); |
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| 546 | |
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| 547 | G4double Step = 0.; |
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| 548 | if (MeanNumberOfPhotons > 0.0) Step = fMaxPhotons / |
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| 549 | MeanNumberOfPhotons; |
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| 550 | |
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| 551 | if (Step > 0. && Step < StepLimit) StepLimit = Step; |
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| 552 | } |
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| 553 | |
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| 554 | // If user has defined an maximum allowed change in beta per step |
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| 555 | if (fMaxBetaChange > 0.) { |
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| 556 | |
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| 557 | G4double dedx = G4LossTableManager::Instance()-> |
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| 558 | GetDEDX(particleType, |
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| 559 | kineticEnergy, |
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| 560 | couple); |
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| 561 | |
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| 562 | G4double deltaGamma = gamma - |
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| 563 | 1./std::sqrt(1.-beta*beta* |
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| 564 | (1.-fMaxBetaChange)* |
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| 565 | (1.-fMaxBetaChange)); |
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| 566 | |
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| 567 | G4double Step = mass * deltaGamma / dedx; |
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| 568 | |
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| 569 | if (Step > 0. && Step < StepLimit) StepLimit = Step; |
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| 570 | |
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| 571 | } |
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| 572 | |
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| 573 | *condition = StronglyForced; |
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| 574 | return StepLimit; |
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[819] | 575 | } |
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| 576 | |
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| 577 | // GetAverageNumberOfPhotons |
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| 578 | // ------------------------- |
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| 579 | // This routine computes the number of Cerenkov photons produced per |
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| 580 | // GEANT-unit (millimeter) in the current medium. |
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| 581 | // ^^^^^^^^^^ |
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| 582 | |
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| 583 | G4double |
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| 584 | G4Cerenkov::GetAverageNumberOfPhotons(const G4double charge, |
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| 585 | const G4double beta, |
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| 586 | const G4Material* aMaterial, |
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| 587 | const G4MaterialPropertyVector* Rindex) const |
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| 588 | { |
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| 589 | const G4double Rfact = 369.81/(eV * cm); |
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| 590 | |
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| 591 | if(beta <= 0.0)return 0.0; |
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| 592 | |
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| 593 | G4double BetaInverse = 1./beta; |
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| 594 | |
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| 595 | // Vectors used in computation of Cerenkov Angle Integral: |
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| 596 | // - Refraction Indices for the current material |
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| 597 | // - new G4PhysicsOrderedFreeVector allocated to hold CAI's |
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| 598 | |
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| 599 | G4int materialIndex = aMaterial->GetIndex(); |
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| 600 | |
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| 601 | // Retrieve the Cerenkov Angle Integrals for this material |
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| 602 | |
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| 603 | G4PhysicsOrderedFreeVector* CerenkovAngleIntegrals = |
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| 604 | (G4PhysicsOrderedFreeVector*)((*thePhysicsTable)(materialIndex)); |
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| 605 | |
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| 606 | if(!(CerenkovAngleIntegrals->IsFilledVectorExist()))return 0.0; |
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| 607 | |
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[961] | 608 | // Min and Max photon energies |
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| 609 | G4double Pmin = Rindex->GetMinPhotonEnergy(); |
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| 610 | G4double Pmax = Rindex->GetMaxPhotonEnergy(); |
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[819] | 611 | |
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| 612 | // Min and Max Refraction Indices |
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| 613 | G4double nMin = Rindex->GetMinProperty(); |
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| 614 | G4double nMax = Rindex->GetMaxProperty(); |
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| 615 | |
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| 616 | // Max Cerenkov Angle Integral |
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| 617 | G4double CAImax = CerenkovAngleIntegrals->GetMaxValue(); |
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| 618 | |
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| 619 | G4double dp, ge; |
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| 620 | |
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| 621 | // If n(Pmax) < 1/Beta -- no photons generated |
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| 622 | |
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| 623 | if (nMax < BetaInverse) { |
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| 624 | dp = 0; |
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| 625 | ge = 0; |
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| 626 | } |
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| 627 | |
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| 628 | // otherwise if n(Pmin) >= 1/Beta -- photons generated |
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| 629 | |
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| 630 | else if (nMin > BetaInverse) { |
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| 631 | dp = Pmax - Pmin; |
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| 632 | ge = CAImax; |
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| 633 | } |
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| 634 | |
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| 635 | // If n(Pmin) < 1/Beta, and n(Pmax) >= 1/Beta, then |
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| 636 | // we need to find a P such that the value of n(P) == 1/Beta. |
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[961] | 637 | // Interpolation is performed by the GetPhotonEnergy() and |
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[819] | 638 | // GetProperty() methods of the G4MaterialPropertiesTable and |
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| 639 | // the GetValue() method of G4PhysicsVector. |
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| 640 | |
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| 641 | else { |
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[961] | 642 | Pmin = Rindex->GetPhotonEnergy(BetaInverse); |
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[819] | 643 | dp = Pmax - Pmin; |
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| 644 | |
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| 645 | // need boolean for current implementation of G4PhysicsVector |
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| 646 | // ==> being phased out |
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| 647 | G4bool isOutRange; |
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| 648 | G4double CAImin = CerenkovAngleIntegrals-> |
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| 649 | GetValue(Pmin, isOutRange); |
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| 650 | ge = CAImax - CAImin; |
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| 651 | |
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| 652 | if (verboseLevel>0) { |
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| 653 | G4cout << "CAImin = " << CAImin << G4endl; |
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| 654 | G4cout << "ge = " << ge << G4endl; |
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| 655 | } |
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| 656 | } |
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| 657 | |
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| 658 | // Calculate number of photons |
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| 659 | G4double NumPhotons = Rfact * charge/eplus * charge/eplus * |
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| 660 | (dp - ge * BetaInverse*BetaInverse); |
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| 661 | |
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| 662 | return NumPhotons; |
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| 663 | } |
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