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Electron beam therapy at extended source‐to‐surface distance: a Monte Carlo investigation

Electron‐beam therapy is used to treat superficial tumors at a standard 100 cm source‐to‐surface distance (SSD). However, certain clinical situations require the use of an extended SSD. In the present study, Monte Carlo methods were used to investigate clinical electron beams, at standard and non‐st...

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Autores principales: O'Shea, Tuathan P., Foley, Mark J., Rajasekar, David, Downes, Patrick A., van der Putten, Wil, Moore, Margaret, Shearer, Andrew
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2008
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5722354/
https://www.ncbi.nlm.nih.gov/pubmed/19020487
http://dx.doi.org/10.1120/jacmp.v9i4.2811
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author O'Shea, Tuathan P.
Foley, Mark J.
Rajasekar, David
Downes, Patrick A.
van der Putten, Wil
Moore, Margaret
Shearer, Andrew
author_facet O'Shea, Tuathan P.
Foley, Mark J.
Rajasekar, David
Downes, Patrick A.
van der Putten, Wil
Moore, Margaret
Shearer, Andrew
author_sort O'Shea, Tuathan P.
collection PubMed
description Electron‐beam therapy is used to treat superficial tumors at a standard 100 cm source‐to‐surface distance (SSD). However, certain clinical situations require the use of an extended SSD. In the present study, Monte Carlo methods were used to investigate clinical electron beams, at standard and non‐standard SSDs, from a Siemens Oncor Avant Garde (Siemens Healthcare, Erlangen, Germany) linear accelerator (LINAC). The LINAC treatment head was modeled in BEAMnrc for electron fields 5 cm in diameter and [Formula: see text] , [Formula: see text] , and [Formula: see text]; for 6 MeV, 9 MeV, and 12 MeV; and for 100 cm, 110 cm, and 120 cm SSD. The DOSXYZnrc code was used to calculate extended SSD factors and dose contributions from various parts of the treatment head. The main effects of extended SSD on water phantom dose distributions were verified by Monte Carlo methods. Monte Carlo–calculated and measured extended SSD factors showed an average difference of [Formula: see text]. For the field 5 cm in diameter, the relative output at extended SSD declined more rapidly than it did for the larger fields. An investigation of output contributions showed this decline was mainly a result of a rapid loss of scatter dose reaching the [Formula: see text] point from the lower scrapers of the electron applicator. The field 5 cm in diameter showed a reduction in dose contributions; the larger fields generally showed an increased contribution from the scrapers with increase in SSD. Angular distributions of applicator‐scattered electrons have shown a large number of acute‐angle electron tracks contributing to the output for larger field sizes, explaining the shallow output reduction. PACS numbers: 87.53.Wz, 87.53.Vb, 87.53.Hv
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spelling pubmed-57223542018-04-02 Electron beam therapy at extended source‐to‐surface distance: a Monte Carlo investigation O'Shea, Tuathan P. Foley, Mark J. Rajasekar, David Downes, Patrick A. van der Putten, Wil Moore, Margaret Shearer, Andrew J Appl Clin Med Phys Radiation Oncology Physics Electron‐beam therapy is used to treat superficial tumors at a standard 100 cm source‐to‐surface distance (SSD). However, certain clinical situations require the use of an extended SSD. In the present study, Monte Carlo methods were used to investigate clinical electron beams, at standard and non‐standard SSDs, from a Siemens Oncor Avant Garde (Siemens Healthcare, Erlangen, Germany) linear accelerator (LINAC). The LINAC treatment head was modeled in BEAMnrc for electron fields 5 cm in diameter and [Formula: see text] , [Formula: see text] , and [Formula: see text]; for 6 MeV, 9 MeV, and 12 MeV; and for 100 cm, 110 cm, and 120 cm SSD. The DOSXYZnrc code was used to calculate extended SSD factors and dose contributions from various parts of the treatment head. The main effects of extended SSD on water phantom dose distributions were verified by Monte Carlo methods. Monte Carlo–calculated and measured extended SSD factors showed an average difference of [Formula: see text]. For the field 5 cm in diameter, the relative output at extended SSD declined more rapidly than it did for the larger fields. An investigation of output contributions showed this decline was mainly a result of a rapid loss of scatter dose reaching the [Formula: see text] point from the lower scrapers of the electron applicator. The field 5 cm in diameter showed a reduction in dose contributions; the larger fields generally showed an increased contribution from the scrapers with increase in SSD. Angular distributions of applicator‐scattered electrons have shown a large number of acute‐angle electron tracks contributing to the output for larger field sizes, explaining the shallow output reduction. PACS numbers: 87.53.Wz, 87.53.Vb, 87.53.Hv John Wiley and Sons Inc. 2008-10-24 /pmc/articles/PMC5722354/ /pubmed/19020487 http://dx.doi.org/10.1120/jacmp.v9i4.2811 Text en © 2008 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
O'Shea, Tuathan P.
Foley, Mark J.
Rajasekar, David
Downes, Patrick A.
van der Putten, Wil
Moore, Margaret
Shearer, Andrew
Electron beam therapy at extended source‐to‐surface distance: a Monte Carlo investigation
title Electron beam therapy at extended source‐to‐surface distance: a Monte Carlo investigation
title_full Electron beam therapy at extended source‐to‐surface distance: a Monte Carlo investigation
title_fullStr Electron beam therapy at extended source‐to‐surface distance: a Monte Carlo investigation
title_full_unstemmed Electron beam therapy at extended source‐to‐surface distance: a Monte Carlo investigation
title_short Electron beam therapy at extended source‐to‐surface distance: a Monte Carlo investigation
title_sort electron beam therapy at extended source‐to‐surface distance: a monte carlo investigation
topic Radiation Oncology Physics
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5722354/
https://www.ncbi.nlm.nih.gov/pubmed/19020487
http://dx.doi.org/10.1120/jacmp.v9i4.2811
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