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Neutron source strength measurements for Varian, Siemens, Elekta, and General Electric linear accelerators

The shielding calculations for high energy ([Formula: see text]) linear accelerators must include the photoneutron production within the head of the accelerator. Procedures have been described to calculate the treatment room door shielding based on the neutron source strength (Q value) for a specifi...

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Autores principales: Followill, David S., Stovall, Marilyn S., Kry, Stephen F., Ibbott, Geoffrey S.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2003
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5724447/
https://www.ncbi.nlm.nih.gov/pubmed/12841788
http://dx.doi.org/10.1120/jacmp.v4i3.2514
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author Followill, David S.
Stovall, Marilyn S.
Kry, Stephen F.
Ibbott, Geoffrey S.
author_facet Followill, David S.
Stovall, Marilyn S.
Kry, Stephen F.
Ibbott, Geoffrey S.
author_sort Followill, David S.
collection PubMed
description The shielding calculations for high energy ([Formula: see text]) linear accelerators must include the photoneutron production within the head of the accelerator. Procedures have been described to calculate the treatment room door shielding based on the neutron source strength (Q value) for a specific accelerator and energy combination. Unfortunately, there is currently little data in the literature stating the neutron source strengths for the most widely used linear accelerators. In this study, the neutron fluence for 36 linear accelerators, including models from Varian, Siemens, Elekta/Philips, and General Electric, was measured using gold‐foil activation. Several of the models and energy combinations had multiple measurements. The neutron fluence measured in the patient plane was independent of the surface area of the room, suggesting that neutron fluence is more dependent on the direct neutron fluence from the head of the accelerator than from room scatter. Neutron source strength, Q, was determined from the measured neutron fluences. As expected, Q increased with increasing photon energy. The Q values ranged from 0.02 for a 10 MV beam to [Formula: see text] neutrons per photon Gy for a 25 MV beam. The most comprehensive set of neutron source strength values, Q, for the current accelerators in clinical use are presented for use in calculating room shielding. PACS number(s): 87.53.–j, 87.52.–g
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spelling pubmed-57244472018-04-02 Neutron source strength measurements for Varian, Siemens, Elekta, and General Electric linear accelerators Followill, David S. Stovall, Marilyn S. Kry, Stephen F. Ibbott, Geoffrey S. J Appl Clin Med Phys Radiation Oncology Physics The shielding calculations for high energy ([Formula: see text]) linear accelerators must include the photoneutron production within the head of the accelerator. Procedures have been described to calculate the treatment room door shielding based on the neutron source strength (Q value) for a specific accelerator and energy combination. Unfortunately, there is currently little data in the literature stating the neutron source strengths for the most widely used linear accelerators. In this study, the neutron fluence for 36 linear accelerators, including models from Varian, Siemens, Elekta/Philips, and General Electric, was measured using gold‐foil activation. Several of the models and energy combinations had multiple measurements. The neutron fluence measured in the patient plane was independent of the surface area of the room, suggesting that neutron fluence is more dependent on the direct neutron fluence from the head of the accelerator than from room scatter. Neutron source strength, Q, was determined from the measured neutron fluences. As expected, Q increased with increasing photon energy. The Q values ranged from 0.02 for a 10 MV beam to [Formula: see text] neutrons per photon Gy for a 25 MV beam. The most comprehensive set of neutron source strength values, Q, for the current accelerators in clinical use are presented for use in calculating room shielding. PACS number(s): 87.53.–j, 87.52.–g John Wiley and Sons Inc. 2003-06-01 /pmc/articles/PMC5724447/ /pubmed/12841788 http://dx.doi.org/10.1120/jacmp.v4i3.2514 Text en © 2003 The Authors. This is an open access article under the terms of the Creative Commons Attribution (http://creativecommons.org/licenses/by/3.0/) License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited.
spellingShingle Radiation Oncology Physics
Followill, David S.
Stovall, Marilyn S.
Kry, Stephen F.
Ibbott, Geoffrey S.
Neutron source strength measurements for Varian, Siemens, Elekta, and General Electric linear accelerators
title Neutron source strength measurements for Varian, Siemens, Elekta, and General Electric linear accelerators
title_full Neutron source strength measurements for Varian, Siemens, Elekta, and General Electric linear accelerators
title_fullStr Neutron source strength measurements for Varian, Siemens, Elekta, and General Electric linear accelerators
title_full_unstemmed Neutron source strength measurements for Varian, Siemens, Elekta, and General Electric linear accelerators
title_short Neutron source strength measurements for Varian, Siemens, Elekta, and General Electric linear accelerators
title_sort neutron source strength measurements for varian, siemens, elekta, and general electric linear accelerators
topic Radiation Oncology Physics
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5724447/
https://www.ncbi.nlm.nih.gov/pubmed/12841788
http://dx.doi.org/10.1120/jacmp.v4i3.2514
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