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Optimization of the photoneutron target geometry for e-accelerator based BNCT

BACKGROUND AND AIM: Today, electron accelerators are taken into consideration as photoneutron sources. Therefore, for maximum production of epithermal neutron flux, designing a photoneutron target is of significant importance. In this paper, the effect of thickness and geometric shape of a photoneut...

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Autores principales: Chegeni, Nahid, Pur, Saleh Boveiry, Razmjoo, Sasan, Hoseini, Seydeh Khadijed
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Electronic physician 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5557140/
https://www.ncbi.nlm.nih.gov/pubmed/28848635
http://dx.doi.org/10.19082/4590
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author Chegeni, Nahid
Pur, Saleh Boveiry
Razmjoo, Sasan
Hoseini, Seydeh Khadijed
author_facet Chegeni, Nahid
Pur, Saleh Boveiry
Razmjoo, Sasan
Hoseini, Seydeh Khadijed
author_sort Chegeni, Nahid
collection PubMed
description BACKGROUND AND AIM: Today, electron accelerators are taken into consideration as photoneutron sources. Therefore, for maximum production of epithermal neutron flux, designing a photoneutron target is of significant importance. In this paper, the effect of thickness and geometric shape of a photoneutron target on neutron output were investigated. METHODS: In this study, a pencil photon source with 13, 15, 18, 20 and 25 MeV energies and a diameter of 2 mm was investigated using Monte Carlo simulation method using MCNP code. To optimize the design of the photoneutron target, the tungsten target with various geometries and thicknesses was investigated. RESULTS: The maximum neutron flux produced for all target geometries and thicknesses occurred at neutron energy peak of around 0.46 MeV. As the thickness increased to 2 cm, neutron flux increased and then a decreasing trend was observed. For various geometrical shapes, the determining factor in photoneutron output was the effective target thickness in the photon interaction path that increased by the increase in the area of interaction. Another factor was the angle of the photon’s incidence with the target surface that resulted in a significant decrease in photoneutron output in cone-shaped targets CONCLUSION: Three factors including the total neutron flux, neutrons energy spectrum, and convergence of neutrons plays an important role in the selection of geometry and shape of the target that should be investigated considering beam shaping assembly (BSA) shape.
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spelling pubmed-55571402017-08-28 Optimization of the photoneutron target geometry for e-accelerator based BNCT Chegeni, Nahid Pur, Saleh Boveiry Razmjoo, Sasan Hoseini, Seydeh Khadijed Electron Physician Original Article BACKGROUND AND AIM: Today, electron accelerators are taken into consideration as photoneutron sources. Therefore, for maximum production of epithermal neutron flux, designing a photoneutron target is of significant importance. In this paper, the effect of thickness and geometric shape of a photoneutron target on neutron output were investigated. METHODS: In this study, a pencil photon source with 13, 15, 18, 20 and 25 MeV energies and a diameter of 2 mm was investigated using Monte Carlo simulation method using MCNP code. To optimize the design of the photoneutron target, the tungsten target with various geometries and thicknesses was investigated. RESULTS: The maximum neutron flux produced for all target geometries and thicknesses occurred at neutron energy peak of around 0.46 MeV. As the thickness increased to 2 cm, neutron flux increased and then a decreasing trend was observed. For various geometrical shapes, the determining factor in photoneutron output was the effective target thickness in the photon interaction path that increased by the increase in the area of interaction. Another factor was the angle of the photon’s incidence with the target surface that resulted in a significant decrease in photoneutron output in cone-shaped targets CONCLUSION: Three factors including the total neutron flux, neutrons energy spectrum, and convergence of neutrons plays an important role in the selection of geometry and shape of the target that should be investigated considering beam shaping assembly (BSA) shape. Electronic physician 2017-06-25 /pmc/articles/PMC5557140/ /pubmed/28848635 http://dx.doi.org/10.19082/4590 Text en © 2017 The Authors This is an open access article under the terms of the Creative Commons Attribution-NonCommercial-NoDerivs License (http://creativecommons.org/licenses/by-nc-nd/3.0/) , which permits use and distribution in any medium, provided the original work is properly cited, the use is non-commercial and no modifications or adaptations are made.
spellingShingle Original Article
Chegeni, Nahid
Pur, Saleh Boveiry
Razmjoo, Sasan
Hoseini, Seydeh Khadijed
Optimization of the photoneutron target geometry for e-accelerator based BNCT
title Optimization of the photoneutron target geometry for e-accelerator based BNCT
title_full Optimization of the photoneutron target geometry for e-accelerator based BNCT
title_fullStr Optimization of the photoneutron target geometry for e-accelerator based BNCT
title_full_unstemmed Optimization of the photoneutron target geometry for e-accelerator based BNCT
title_short Optimization of the photoneutron target geometry for e-accelerator based BNCT
title_sort optimization of the photoneutron target geometry for e-accelerator based bnct
topic Original Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5557140/
https://www.ncbi.nlm.nih.gov/pubmed/28848635
http://dx.doi.org/10.19082/4590
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