| 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 | // $Id: G4LowEnergyPolarizedRayleigh.cc,v 1.10 2009/06/11 15:47:08 mantero Exp $
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| 27 | // GEANT4 tag $Name: geant4-09-03-cand-01 $
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| 28 | //
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| 29 | // --------------------------------------------------------------
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| 30 | //
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| 31 | // File name: G4LowEnergyPolarizedRayleigh.cc
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| 32 | //
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| 33 | // Author: Capra Riccardo
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| 34 | //
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| 35 | // Creation date: May 2005
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| 36 | //
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| 37 | // History:
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| 38 | // -----------
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| 39 | // 02 May 2005 R. Capra 1st implementation
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| 40 | // 20 May 2005 MGP Changed name of a local variable hiding
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| 41 | // a data member of the base class
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| 42 | //
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| 43 | //----------------------------------------------------------------
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| 44 |
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| 45 |
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| 46 | #include "G4LowEnergyPolarizedRayleigh.hh"
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| 47 |
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| 48 | #include "G4LogLogInterpolation.hh"
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| 49 | #include "G4VCrossSectionHandler.hh"
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| 50 | #include "G4VEMDataSet.hh"
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| 51 | #include "globals.hh" //G4Exception
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| 52 |
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| 53 |
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| 54 | G4LowEnergyPolarizedRayleigh::G4LowEnergyPolarizedRayleigh(const G4String& processName)
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| 55 | :
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| 56 | G4VLowEnergyDiscretePhotonProcess(processName, "rayl/re-cs-", "rayl/re-ff-", new G4LogLogInterpolation, 250*eV, 100*GeV),
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| 57 | intrinsicLowEnergyLimit(10*eV),
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| 58 | intrinsicHighEnergyLimit(100*GeV)
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| 59 | {
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| 60 | if (GetLowEnergyLimit() < intrinsicLowEnergyLimit ||
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| 61 | GetHighEnergyLimit() > intrinsicHighEnergyLimit)
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| 62 | G4Exception("G4LowEnergyPolarizedRayleigh::G4LowEnergyPolarizedRayleigh - Energy limit outside intrinsic process validity range");
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| 63 |
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| 64 |
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| 65 | G4cout << G4endl;
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| 66 | G4cout << "*******************************************************************************" << G4endl;
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| 67 | G4cout << "*******************************************************************************" << G4endl;
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| 68 | G4cout << " The class G4LowEnergyPolarizedRayleigh is NOT SUPPORTED ANYMORE. " << G4endl;
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| 69 | G4cout << " It will be REMOVED with the next major release of Geant4. " << G4endl;
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| 70 | G4cout << " Please consult: https://twiki.cern.ch/twiki/bin/view/Geant4/LoweProcesses" << G4endl;
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| 71 | G4cout << "*******************************************************************************" << G4endl;
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| 72 | G4cout << "*******************************************************************************" << G4endl;
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| 73 | G4cout << G4endl;
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| 74 | }
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| 75 |
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| 76 |
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| 77 | G4VParticleChange* G4LowEnergyPolarizedRayleigh::PostStepDoIt(const G4Track& aTrack, const G4Step& aStep)
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| 78 | {
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| 79 | // aParticleChange comes from G4VProcess
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| 80 | aParticleChange.Initialize(aTrack);
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| 81 |
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| 82 | const G4DynamicParticle* incomingPhoton = aTrack.GetDynamicParticle();
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| 83 | G4double incomingPhotonEnergy = incomingPhoton->GetKineticEnergy();
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| 84 |
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| 85 | if (incomingPhotonEnergy <= GetLowEnergyLimit())
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| 86 | {
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| 87 | aParticleChange.ProposeTrackStatus(fStopAndKill);
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| 88 | aParticleChange.ProposeEnergy(0.);
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| 89 | aParticleChange.ProposeLocalEnergyDeposit(incomingPhotonEnergy);
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| 90 |
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| 91 | return G4VLowEnergyDiscretePhotonProcess::PostStepDoIt(aTrack, aStep);
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| 92 | }
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| 93 |
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| 94 | const G4VCrossSectionHandler* crossSectionHandle = GetCrossSectionHandler();
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| 95 | const G4MaterialCutsCouple* couple = aTrack.GetMaterialCutsCouple();
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| 96 | G4int zAtom = crossSectionHandle->SelectRandomAtom(couple, incomingPhotonEnergy);
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| 97 |
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| 98 | G4double outcomingPhotonCosTheta = GenerateCosTheta(incomingPhotonEnergy, zAtom);
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| 99 | G4double outcomingPhotonPhi = GeneratePhi(outcomingPhotonCosTheta);
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| 100 | G4double beta=GeneratePolarizationAngle();
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| 101 |
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| 102 | // incomingPhoton reference frame:
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| 103 | // z = versor parallel to the incomingPhotonDirection
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| 104 | // x = versor parallel to the incomingPhotonPolarization
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| 105 | // y = defined as z^x
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| 106 |
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| 107 | // outgoingPhoton reference frame:
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| 108 | // z' = versor parallel to the outgoingPhotonDirection
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| 109 | // x' = defined as x-x*z'z' normalized
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| 110 | // y' = defined as z'^x'
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| 111 |
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| 112 | G4ThreeVector z(incomingPhoton->GetMomentumDirection().unit());
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| 113 | G4ThreeVector x(GetPhotonPolarization(*incomingPhoton));
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| 114 | G4ThreeVector y(z.cross(x));
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| 115 |
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| 116 | // z' = std::cos(phi)*std::sin(theta) x + std::sin(phi)*std::sin(theta) y + std::cos(theta) z
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| 117 | G4double xDir;
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| 118 | G4double yDir;
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| 119 | G4double zDir;
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| 120 | zDir=outcomingPhotonCosTheta;
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| 121 | xDir=std::sqrt(1-outcomingPhotonCosTheta*outcomingPhotonCosTheta);
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| 122 | yDir=xDir;
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| 123 | xDir*=std::cos(outcomingPhotonPhi);
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| 124 | yDir*=std::sin(outcomingPhotonPhi);
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| 125 |
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| 126 | G4ThreeVector zPrime((xDir*x + yDir*y + zDir*z).unit());
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| 127 | G4ThreeVector xPrime(x.perpPart(zPrime).unit());
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| 128 | G4ThreeVector yPrime(zPrime.cross(xPrime));
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| 129 |
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| 130 | // outgoingPhotonPolarization is directed as x' std::cos(beta) + y' std::sin(beta)
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| 131 | G4ThreeVector outcomingPhotonPolarization(xPrime*std::cos(beta) + yPrime*std::sin(beta));
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| 132 |
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| 133 | aParticleChange.ProposeEnergy(incomingPhotonEnergy);
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| 134 | aParticleChange.ProposeMomentumDirection(zPrime);
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| 135 | aParticleChange.ProposePolarization(outcomingPhotonPolarization);
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| 136 | aParticleChange.SetNumberOfSecondaries(0);
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| 137 |
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| 138 | // returns aParticleChange though pParticleChange and G4VProcess::PostStepDoIt
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| 139 | return G4VLowEnergyDiscretePhotonProcess::PostStepDoIt(aTrack, aStep);
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| 140 | }
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| 141 |
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| 142 |
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| 143 |
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| 144 |
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| 145 | G4double G4LowEnergyPolarizedRayleigh::GenerateCosTheta(G4double incomingPhotonEnergy, G4int zAtom) const
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| 146 | {
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| 147 | // d sigma k0
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| 148 | // --------- = r0^2 * pi * F^2(x, Z) * ( 2 - sin^2 theta) * std::sin (theta), x = ---- std::sin(theta/2)
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| 149 | // d theta hc
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| 150 |
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| 151 | // d sigma k0 1 - y
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| 152 | // --------- = r0^2 * pi * F^2(x, Z) * ( 1 + y^2), x = ---- std::sqrt ( ------- ), y = std::cos(theta)
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| 153 | // d y hc 2
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| 154 |
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| 155 | // Z
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| 156 | // F(x, Z) ~ --------
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| 157 | // a + bx
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| 158 | //
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| 159 | // The time to exit from the outer loop grows as ~ k0
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| 160 | // On pcgeant2 the time is ~ 1 s for k0 ~ 1 MeV on the oxygen element. A 100 GeV
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| 161 | // event will take ~ 10 hours.
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| 162 | //
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| 163 | // On the avarage the inner loop does 1.5 iterations before exiting
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| 164 |
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| 165 | const G4double xFactor = (incomingPhotonEnergy*cm)/(h_Planck*c_light);
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| 166 | const G4VEMDataSet * formFactorData = GetScatterFunctionData();
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| 167 |
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| 168 | G4double cosTheta;
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| 169 | G4double fCosTheta;
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| 170 | G4double x;
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| 171 | G4double fValue;
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| 172 |
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| 173 | do
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| 174 | {
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| 175 | do
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| 176 | {
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| 177 | cosTheta = 2.*G4UniformRand()-1.;
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| 178 | fCosTheta = (1.+cosTheta*cosTheta)/2.;
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| 179 | }
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| 180 | while (fCosTheta < G4UniformRand());
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| 181 |
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| 182 | x = xFactor*std::sqrt((1.-cosTheta)/2.);
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| 183 |
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| 184 | if (x > 1.e+005)
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| 185 | fValue = formFactorData->FindValue(x, zAtom-1);
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| 186 | else
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| 187 | fValue = formFactorData->FindValue(0., zAtom-1);
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| 188 |
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| 189 | fValue/=zAtom;
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| 190 | fValue*=fValue;
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| 191 | }
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| 192 | while(fValue < G4UniformRand());
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| 193 |
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| 194 | return cosTheta;
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| 195 | }
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| 196 |
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| 197 |
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| 198 |
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| 199 | G4double G4LowEnergyPolarizedRayleigh::GeneratePhi(G4double cosTheta) const
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| 200 | {
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| 201 | // d sigma
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| 202 | // --------- = alpha * ( 1 - sin^2 (theta) * cos^2 (phi) )
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| 203 | // d phi
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| 204 |
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| 205 | // On the average the loop takes no more than 2 iterations before exiting
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| 206 |
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| 207 | G4double phi;
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| 208 | G4double cosPhi;
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| 209 | G4double phiProbability;
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| 210 | G4double sin2Theta;
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| 211 |
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| 212 | sin2Theta=1.-cosTheta*cosTheta;
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| 213 |
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| 214 | do
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| 215 | {
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| 216 | phi = twopi * G4UniformRand();
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| 217 | cosPhi = std::cos(phi);
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| 218 | phiProbability= 1. - sin2Theta*cosPhi*cosPhi;
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| 219 | }
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| 220 | while (phiProbability < G4UniformRand());
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| 221 |
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| 222 | return phi;
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| 223 | }
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| 224 |
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| 225 |
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| 226 |
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| 227 |
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| 228 |
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| 229 | G4double G4LowEnergyPolarizedRayleigh::GeneratePolarizationAngle(void) const
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| 230 | {
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| 231 | // Rayleigh polarization is always on the x' direction
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| 232 |
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| 233 | return 0;
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| 234 | }
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