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A Geant4/Garfield++ and Geant4/Degrad Interface for the Simulation of Gaseous Detectors

For several years, attempts have been made to interface Geant4 and other software packages with the aim of simulating the complete response of a gaseous particle detector. The present paper illustrates different possibilities to interface Geant4 with two such packages, Garfield++ and Degrad. The bas...

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Autores principales: Pfeiffer, Dorothea, De Keukeleere, Lennert, Azevedo, Carlos, Belloni, Francesca, Biagi, Stephen, Grichine, Vladimir, Hayen, Leendert, Hanu, Andrei R., Hřivnáčová, Ivana, Ivanchenko, Vladimir, Krylov, Vladyslav, Schindler, Heinrich, Veenhof, Rob
Lenguaje:eng
Publicado: 2018
Materias:
Acceso en línea:http://cds.cern.ch/record/2628557
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author Pfeiffer, Dorothea
De Keukeleere, Lennert
Azevedo, Carlos
Belloni, Francesca
Biagi, Stephen
Grichine, Vladimir
Hayen, Leendert
Hanu, Andrei R.
Hřivnáčová, Ivana
Ivanchenko, Vladimir
Krylov, Vladyslav
Schindler, Heinrich
Veenhof, Rob
author_facet Pfeiffer, Dorothea
De Keukeleere, Lennert
Azevedo, Carlos
Belloni, Francesca
Biagi, Stephen
Grichine, Vladimir
Hayen, Leendert
Hanu, Andrei R.
Hřivnáčová, Ivana
Ivanchenko, Vladimir
Krylov, Vladyslav
Schindler, Heinrich
Veenhof, Rob
author_sort Pfeiffer, Dorothea
collection CERN
description For several years, attempts have been made to interface Geant4 and other software packages with the aim of simulating the complete response of a gaseous particle detector. The present paper illustrates different possibilities to interface Geant4 with two such packages, Garfield++ and Degrad. The basic idea is to use the Geant4 physics parameterization feature and to implement a Garfield++ or Degrad based detector simulation as an external model. With the Geant4/Degrad interface, detailed simulations of the X-ray interaction in gaseous detectors, including shell absorption by photoelectric effect, subsequent Auger shake-off, and fluorescence emission, become possible. The Geant4/Garfield++ interface can be used for photons and charged particles of all kinetic energies. Depending on the particular physics case, either the Geant4 PAI model, the Heed PAI model or both Geant4 and Heed are responsible for primary ionization and the production of the conduction electrons. For the case in which the Geant4 PAI model is used in conjunction with the Heed PAI model, a more detailed analysis is performed. Parameters, such as the lower production cut of the PAI model and the lowest electron energy limit of the physics list have to be set correctly. The paper demonstrates how to determine these parameters with the help of the W value and Fano factor of the gas mixture. The simulation results of this Geant4/Heed PAI model interface are then verified against the results obtained with the standalone software packages.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2018
record_format invenio
spelling cern-26285572019-11-04T14:58:55Zhttp://cds.cern.ch/record/2628557engPfeiffer, DorotheaDe Keukeleere, LennertAzevedo, CarlosBelloni, FrancescaBiagi, StephenGrichine, VladimirHayen, LeendertHanu, Andrei R.Hřivnáčová, IvanaIvanchenko, VladimirKrylov, VladyslavSchindler, HeinrichVeenhof, RobA Geant4/Garfield++ and Geant4/Degrad Interface for the Simulation of Gaseous Detectorsphysics.comp-phOther Fields of Physicsphysics.ins-detDetectors and Experimental TechniquesFor several years, attempts have been made to interface Geant4 and other software packages with the aim of simulating the complete response of a gaseous particle detector. The present paper illustrates different possibilities to interface Geant4 with two such packages, Garfield++ and Degrad. The basic idea is to use the Geant4 physics parameterization feature and to implement a Garfield++ or Degrad based detector simulation as an external model. With the Geant4/Degrad interface, detailed simulations of the X-ray interaction in gaseous detectors, including shell absorption by photoelectric effect, subsequent Auger shake-off, and fluorescence emission, become possible. The Geant4/Garfield++ interface can be used for photons and charged particles of all kinetic energies. Depending on the particular physics case, either the Geant4 PAI model, the Heed PAI model or both Geant4 and Heed are responsible for primary ionization and the production of the conduction electrons. For the case in which the Geant4 PAI model is used in conjunction with the Heed PAI model, a more detailed analysis is performed. Parameters, such as the lower production cut of the PAI model and the lowest electron energy limit of the physics list have to be set correctly. The paper demonstrates how to determine these parameters with the help of the W value and Fano factor of the gas mixture. The simulation results of this Geant4/Heed PAI model interface are then verified against the results obtained with the standalone software packages.arXiv:1806.05880oai:cds.cern.ch:26285572018
spellingShingle physics.comp-ph
Other Fields of Physics
physics.ins-det
Detectors and Experimental Techniques
Pfeiffer, Dorothea
De Keukeleere, Lennert
Azevedo, Carlos
Belloni, Francesca
Biagi, Stephen
Grichine, Vladimir
Hayen, Leendert
Hanu, Andrei R.
Hřivnáčová, Ivana
Ivanchenko, Vladimir
Krylov, Vladyslav
Schindler, Heinrich
Veenhof, Rob
A Geant4/Garfield++ and Geant4/Degrad Interface for the Simulation of Gaseous Detectors
title A Geant4/Garfield++ and Geant4/Degrad Interface for the Simulation of Gaseous Detectors
title_full A Geant4/Garfield++ and Geant4/Degrad Interface for the Simulation of Gaseous Detectors
title_fullStr A Geant4/Garfield++ and Geant4/Degrad Interface for the Simulation of Gaseous Detectors
title_full_unstemmed A Geant4/Garfield++ and Geant4/Degrad Interface for the Simulation of Gaseous Detectors
title_short A Geant4/Garfield++ and Geant4/Degrad Interface for the Simulation of Gaseous Detectors
title_sort geant4/garfield++ and geant4/degrad interface for the simulation of gaseous detectors
topic physics.comp-ph
Other Fields of Physics
physics.ins-det
Detectors and Experimental Techniques
url http://cds.cern.ch/record/2628557
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