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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Veröffentlicht in: | Journal of physics. Conference series 2023-01, Vol.2420 (1), p.12064 |
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creator | Ramoisiaux, E Hernalsteens, C Tesse, R Gnacadja, E Pauly, N Vanwelde, M Stichelbaut, F |
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. |
doi_str_mv | 10.1088/1742-6596/2420/1/012064 |
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®
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.</description><identifier>ISSN: 1742-6588</identifier><identifier>EISSN: 1742-6596</identifier><identifier>DOI: 10.1088/1742-6596/2420/1/012064</identifier><language>eng</language><publisher>Bristol: IOP Publishing</publisher><subject>Computation ; Ion beams ; Particle tracking ; Physics ; Protons ; Radiation shielding ; Radiation therapy ; Research facilities ; Simulation ; Systematic errors ; Therapy</subject><ispartof>Journal of physics. Conference series, 2023-01, Vol.2420 (1), p.12064</ispartof><rights>Published under licence by IOP Publishing Ltd</rights><rights>Published under licence by IOP Publishing Ltd. This work is published under http://creativecommons.org/licenses/by/3.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c2744-7ab15bb9fc8dc2a8c54022831692eec05ca7eb8e0b6e11adea85e19745e73dac3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.1088/1742-6596/2420/1/012064/pdf$$EPDF$$P50$$Giop$$Hfree_for_read</linktopdf><link.rule.ids>314,776,780,27903,27904,38847,38869,53819,53846</link.rule.ids></links><search><creatorcontrib>Ramoisiaux, E</creatorcontrib><creatorcontrib>Hernalsteens, C</creatorcontrib><creatorcontrib>Tesse, R</creatorcontrib><creatorcontrib>Gnacadja, E</creatorcontrib><creatorcontrib>Pauly, N</creatorcontrib><creatorcontrib>Vanwelde, M</creatorcontrib><creatorcontrib>Stichelbaut, F</creatorcontrib><title>Concrete shielding activation for proton therapy systems using BDSIM and FISPACT-II</title><title>Journal of physics. Conference series</title><addtitle>J. Phys.: Conf. Ser</addtitle><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.</description><subject>Computation</subject><subject>Ion beams</subject><subject>Particle tracking</subject><subject>Physics</subject><subject>Protons</subject><subject>Radiation shielding</subject><subject>Radiation therapy</subject><subject>Research facilities</subject><subject>Simulation</subject><subject>Systematic errors</subject><subject>Therapy</subject><issn>1742-6588</issn><issn>1742-6596</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><sourceid>O3W</sourceid><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNqFkNFLwzAQxoMoOKd_gwXfhNokTZP0cVanlYmDzueQplfXsbU16YT997ZUFEHwXu7gvu-744fQJcE3BEsZEMGoz6OYB5RRHJAAE4o5O0KT783x9yzlKTpzboNx2JeYoCxpamOhA8-tK9gWVf3madNVH7qrmtorG-u1tun6sVuD1e3BcwfXwc55ezdob--y9NnTdeHN02w5S1Z-mp6jk1JvHVx89Sl6nd-vkkd_8fKQJrOFb6hgzBc6J1Gex6WRhaFamohhSmVIeEwBDI6MFpBLwDkHQnQBWkZAYsEiEGGhTThFV2Nu_-H7HlynNs3e1v1JRQUXjEec414lRpWxjXMWStXaaqftQRGsBoJqYKMGTmogqIgaCfbOcHRWTfsT_b_r-g_X0zLJfgtVW5ThJ7ENf7k</recordid><startdate>20230101</startdate><enddate>20230101</enddate><creator>Ramoisiaux, E</creator><creator>Hernalsteens, C</creator><creator>Tesse, R</creator><creator>Gnacadja, E</creator><creator>Pauly, N</creator><creator>Vanwelde, M</creator><creator>Stichelbaut, F</creator><general>IOP Publishing</general><scope>O3W</scope><scope>TSCCA</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>H8D</scope><scope>HCIFZ</scope><scope>L7M</scope><scope>P5Z</scope><scope>P62</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope></search><sort><creationdate>20230101</creationdate><title>Concrete shielding activation for proton therapy systems using BDSIM and FISPACT-II</title><author>Ramoisiaux, E ; Hernalsteens, C ; Tesse, R ; Gnacadja, E ; Pauly, N ; Vanwelde, M ; Stichelbaut, F</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c2744-7ab15bb9fc8dc2a8c54022831692eec05ca7eb8e0b6e11adea85e19745e73dac3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Computation</topic><topic>Ion beams</topic><topic>Particle tracking</topic><topic>Physics</topic><topic>Protons</topic><topic>Radiation shielding</topic><topic>Radiation therapy</topic><topic>Research facilities</topic><topic>Simulation</topic><topic>Systematic errors</topic><topic>Therapy</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ramoisiaux, E</creatorcontrib><creatorcontrib>Hernalsteens, C</creatorcontrib><creatorcontrib>Tesse, R</creatorcontrib><creatorcontrib>Gnacadja, E</creatorcontrib><creatorcontrib>Pauly, N</creatorcontrib><creatorcontrib>Vanwelde, M</creatorcontrib><creatorcontrib>Stichelbaut, F</creatorcontrib><collection>IOP Publishing Free Content</collection><collection>IOPscience (Open Access)</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>Aerospace Database</collection><collection>SciTech Premium Collection</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Advanced Technologies & Aerospace Database</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><jtitle>Journal of physics. Conference series</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ramoisiaux, E</au><au>Hernalsteens, C</au><au>Tesse, R</au><au>Gnacadja, E</au><au>Pauly, N</au><au>Vanwelde, M</au><au>Stichelbaut, F</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Concrete shielding activation for proton therapy systems using BDSIM and FISPACT-II</atitle><jtitle>Journal of physics. Conference series</jtitle><addtitle>J. Phys.: Conf. Ser</addtitle><date>2023-01-01</date><risdate>2023</risdate><volume>2420</volume><issue>1</issue><spage>12064</spage><pages>12064-</pages><issn>1742-6588</issn><eissn>1742-6596</eissn><abstract>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.</abstract><cop>Bristol</cop><pub>IOP Publishing</pub><doi>10.1088/1742-6596/2420/1/012064</doi><tpages>6</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Computation Ion beams Particle tracking Physics Protons Radiation shielding Radiation therapy Research facilities Simulation Systematic errors Therapy |
title | Concrete shielding activation for proton therapy systems using BDSIM and FISPACT-II |
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