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Concrete Shielding Activation for Proton Therapy Systems Using BDSIM and FISPACT-II

Proton therapy systems are used worldwide for patient treatment and fundamental research. The generation of secondary particles when the beam interacts with the beamline elements is a well-known issue. In particular, the energy degrader is the dominant source of secondary radiation. This poses new c...

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Autores principales: Ramoisiaux, Eliott, Gnacadja, Eustache, Hernalsteens, Cédric, Pauly, Nicolas, Stichelbaut, Frederic, Tesse, Robin, Vanwelde, Marion
Lenguaje:eng
Publicado: 2022
Materias:
Acceso en línea:https://dx.doi.org/10.18429/JACoW-IPAC2022-MOPOMS041
http://cds.cern.ch/record/2845732
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author Ramoisiaux, Eliott
Gnacadja, Eustache
Hernalsteens, Cédric
Pauly, Nicolas
Stichelbaut, Frederic
Tesse, Robin
Vanwelde, Marion
author_facet Ramoisiaux, Eliott
Gnacadja, Eustache
Hernalsteens, Cédric
Pauly, Nicolas
Stichelbaut, Frederic
Tesse, Robin
Vanwelde, Marion
author_sort Ramoisiaux, Eliott
collection CERN
description Proton therapy systems are used worldwide for patient treatment and fundamental research. The generation of secondary particles when the beam interacts with the beamline elements is a well-known issue. In particular, the energy degrader is the dominant source of secondary radiation. This poses new challenges for the concrete shielding of compact systems and beamline elements activation computation. We use a novel methodology to seamlessly simulate all the processes relevant to the activation evaluation. A realistic model of the system is developed using Beam Delivery Simulation (BDSIM), a Geant4-based particle tracking code that allows a single model to simulate primary and secondary particle tracking and all particle-matter interactions. The secondary particle fluxes extracted from the simulations are provided as input to FISPACT-II to compute the activation by solving the rate equations. This approach is applied to the Ion Beam Applications (IBA) Proteus®ONE (P1) system and the shielding of the proton therapy research centre of Charleroi, Belgium. Proton loss distributions are used to model the production of secondary neutrals inside the accelerator structure. Two models for the distribution of proton losses are compared for the computation of the clearance index at specific locations of the design. Results show that the variation in the accelerator loss models can be characterised as a systematic error.
id cern-2845732
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2022
record_format invenio
spelling cern-28457322023-01-11T21:31:14Zdoi:10.18429/JACoW-IPAC2022-MOPOMS041http://cds.cern.ch/record/2845732engRamoisiaux, EliottGnacadja, EustacheHernalsteens, CédricPauly, NicolasStichelbaut, FredericTesse, RobinVanwelde, MarionConcrete Shielding Activation for Proton Therapy Systems Using BDSIM and FISPACT-IIAccelerators and Storage RingsProton therapy systems are used worldwide for patient treatment and fundamental research. The generation of secondary particles when the beam interacts with the beamline elements is a well-known issue. In particular, the energy degrader is the dominant source of secondary radiation. This poses new challenges for the concrete shielding of compact systems and beamline elements activation computation. We use a novel methodology to seamlessly simulate all the processes relevant to the activation evaluation. A realistic model of the system is developed using Beam Delivery Simulation (BDSIM), a Geant4-based particle tracking code that allows a single model to simulate primary and secondary particle tracking and all particle-matter interactions. The secondary particle fluxes extracted from the simulations are provided as input to FISPACT-II to compute the activation by solving the rate equations. This approach is applied to the Ion Beam Applications (IBA) Proteus®ONE (P1) system and the shielding of the proton therapy research centre of Charleroi, Belgium. Proton loss distributions are used to model the production of secondary neutrals inside the accelerator structure. Two models for the distribution of proton losses are compared for the computation of the clearance index at specific locations of the design. Results show that the variation in the accelerator loss models can be characterised as a systematic error.oai:cds.cern.ch:28457322022
spellingShingle Accelerators and Storage Rings
Ramoisiaux, Eliott
Gnacadja, Eustache
Hernalsteens, Cédric
Pauly, Nicolas
Stichelbaut, Frederic
Tesse, Robin
Vanwelde, Marion
Concrete Shielding Activation for Proton Therapy Systems Using BDSIM and FISPACT-II
title Concrete Shielding Activation for Proton Therapy Systems Using BDSIM and FISPACT-II
title_full Concrete Shielding Activation for Proton Therapy Systems Using BDSIM and FISPACT-II
title_fullStr Concrete Shielding Activation for Proton Therapy Systems Using BDSIM and FISPACT-II
title_full_unstemmed Concrete Shielding Activation for Proton Therapy Systems Using BDSIM and FISPACT-II
title_short Concrete Shielding Activation for Proton Therapy Systems Using BDSIM and FISPACT-II
title_sort concrete shielding activation for proton therapy systems using bdsim and fispact-ii
topic Accelerators and Storage Rings
url https://dx.doi.org/10.18429/JACoW-IPAC2022-MOPOMS041
http://cds.cern.ch/record/2845732
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