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G4BogackiShampine23.hh
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//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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// G4BogackiShampine23
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//
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// Class description:
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//
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// Bogacki-Shampine - 4 - 3(2) non-FSAL implementation
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//
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// An implementation of the embedded RK method from the paper
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// [1] P. Bogacki and L. F. Shampine,
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// "A 3(2) pair of Runge - Kutta formulas"
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// Appl. Math. Lett., vol. 2, no. 4, pp. 321-325, Jan. 1989.
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//
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// This version does not utilise the FSAL property of the method,
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// which would allow the reuse of the last derivative in the next step.
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// (Alternative FSAL implementation created with revised interface)
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// Created: Somnath Banerjee, Google Summer of Code 2015, 20 May 2015
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// Supervision: John Apostolakis, CERN
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// --------------------------------------------------------------------
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#ifndef G4BOGACKI_SHAMPINE23_HH
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#define G4BOGACKI_SHAMPINE23_HH
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#include "
G4MagIntegratorStepper.hh
"
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#include "
G4FieldTrack.hh
"
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class
G4BogackiShampine23
:
public
G4MagIntegratorStepper
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{
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public
:
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G4BogackiShampine23
(
G4EquationOfMotion
* EqRhs,
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G4int
numberOfVariables = 6);
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virtual
void
Stepper
(
const
G4double
yInput[],
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const
G4double
dydx[],
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G4double
hstep,
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G4double
yOutput[],
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G4double
yError[])
override
;
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void
Stepper
(
const
G4double
yInput[],
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const
G4double
dydx[],
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G4double
hstep,
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G4double
yOutput[],
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G4double
yError[],
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G4double
dydxOutput[]);
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G4BogackiShampine23
(
const
G4BogackiShampine23
&) =
delete
;
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G4BogackiShampine23
&
operator =
(
const
G4BogackiShampine23
&) =
delete
;
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virtual
G4double
DistChord
()
const override
;
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virtual
G4int
IntegratorOrder
()
const override
{
return
3; }
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private
:
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void
makeStep
(
const
G4double
yInput[],
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const
G4double
dydx[],
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const
G4double
hstep,
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G4double
yOutput[],
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G4double
* dydxOutput =
nullptr
,
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G4double
* yError =
nullptr
)
const
;
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G4double
fyIn
[
G4FieldTrack::ncompSVEC
],
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fdydx
[
G4FieldTrack::ncompSVEC
],
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fyOut
[
G4FieldTrack::ncompSVEC
],
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fdydxOut
[
G4FieldTrack::ncompSVEC
];
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G4double
fhstep
= -1.0;
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};
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#endif
geant4
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geant4-10.6-release
source
geometry
magneticfield
include
G4BogackiShampine23.hh
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Jin Huang
. updated:
Wed Jun 29 2022 17:25:16
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