| 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: G4EqMagElectricField.cc,v 1.14 2008/04/24 12:33:35 tnikitin Exp $
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| 28 | // GEANT4 tag $Name: geant4-09-02-cand-01 $
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| 29 | //
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| 30 | //
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| 31 | // This is the standard right-hand side for equation of motion.
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| 32 | //
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| 33 | // The only case another is required is when using a moving reference
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| 34 | // frame ... or extending the class to include additional Forces,
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| 35 | // eg an electric field
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| 36 | //
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| 37 | // 10.11.98 V.Grichine
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| 38 | //
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| 39 | // -------------------------------------------------------------------
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| 40 |
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| 41 | #include "G4EqMagElectricField.hh"
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| 42 | #include "globals.hh"
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| 43 |
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| 44 | void
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| 45 | G4EqMagElectricField::SetChargeMomentumMass(G4double particleCharge, // e+ units
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| 46 | G4double,
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| 47 | G4double particleMass)
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| 48 | {
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| 49 | fElectroMagCof = eplus*particleCharge*c_light ;
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| 50 | fMassCof = particleMass*particleMass ;
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| 51 | }
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| 52 |
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| 53 |
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| 54 |
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| 55 | void
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| 56 | G4EqMagElectricField::EvaluateRhsGivenB(const G4double y[],
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| 57 | const G4double Field[],
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| 58 | G4double dydx[] ) const
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| 59 | {
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| 60 |
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| 61 | // Components of y:
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| 62 | // 0-2 dr/ds,
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| 63 | // 3-5 dp/ds - momentum derivatives
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| 64 |
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| 65 | G4double pSquared = y[3]*y[3] + y[4]*y[4] + y[5]*y[5] ;
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| 66 |
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| 67 | G4double Energy = std::sqrt( pSquared + fMassCof );
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| 68 | G4double cof2 = Energy/c_light ;
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| 69 |
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| 70 | G4double pModuleInverse = 1.0/std::sqrt(pSquared) ;
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| 71 |
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| 72 | // G4double inverse_velocity = Energy * c_light * pModuleInverse;
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| 73 | G4double inverse_velocity = Energy * pModuleInverse / c_light;
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| 74 |
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| 75 | G4double cof1 = fElectroMagCof*pModuleInverse ;
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| 76 |
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| 77 | // G4double vDotE = y[3]*Field[3] + y[4]*Field[4] + y[5]*Field[5] ;
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| 78 |
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| 79 |
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| 80 | dydx[0] = y[3]*pModuleInverse ;
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| 81 | dydx[1] = y[4]*pModuleInverse ;
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| 82 | dydx[2] = y[5]*pModuleInverse ;
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| 83 |
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| 84 | dydx[3] = cof1*(cof2*Field[3] + (y[4]*Field[2] - y[5]*Field[1])) ;
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| 85 |
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| 86 | dydx[4] = cof1*(cof2*Field[4] + (y[5]*Field[0] - y[3]*Field[2])) ;
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| 87 |
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| 88 | dydx[5] = cof1*(cof2*Field[5] + (y[3]*Field[1] - y[4]*Field[0])) ;
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| 89 |
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| 90 | dydx[6] = 0.;//not used
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| 91 |
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| 92 | // Lab Time of flight
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| 93 | dydx[7] = inverse_velocity;
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| 94 | return ;
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| 95 | }
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