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Monte Carlo calculation of beam quality correction for solid‐state detectors and phantom scatter correction at (137)Cs energy
Beam quality correction [Formula: see text] , which reflects the absorbed energy dependence of the detector, is calculated for solid‐state detector materials diamond, LiF, [Formula: see text] , and [Formula: see text] for the [Formula: see text] RTR brachytherapy source using the Monte Carlo‐based E...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
John Wiley and Sons Inc.
2014
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5711252/ https://www.ncbi.nlm.nih.gov/pubmed/24423840 http://dx.doi.org/10.1120/jacmp.v15i1.4445 |
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author | Selvam, T. Palani Mishra, Subhalaxmi Vishwakarma, R.S. |
author_facet | Selvam, T. Palani Mishra, Subhalaxmi Vishwakarma, R.S. |
author_sort | Selvam, T. Palani |
collection | PubMed |
description | Beam quality correction [Formula: see text] , which reflects the absorbed energy dependence of the detector, is calculated for solid‐state detector materials diamond, LiF, [Formula: see text] , and [Formula: see text] for the [Formula: see text] RTR brachytherapy source using the Monte Carlo‐based EGSnrc code system. The study also includes calculation of detector‐specific phantom scatter corrections [Formula: see text] for solid phantoms such as PMMA, polystyrene, RW1, solid water, virtual water, and plastic water. Above corrections are calculated as a function of distance r along the transverse axis of the source. [Formula: see text] is about unity for the [Formula: see text] detector. LiF detector shows a gradual decrease in [Formula: see text] with r (decrease is about 2% over the distance range of 1‐15 cm). Diamond detector shows a gradual increase in [Formula: see text] with r (about 3% larger than unity at 15 cm). In the case of [Formula: see text] detector, [Formula: see text] decreases with r steeply (about 14% over the distance range of 1‐15 cm). The study shows that some solid‐state detectors demonstrate distance‐dependent [Formula: see text] values, but the degree of deviation from unity depends on the type of solid phantom and the detector. PACS number: 87.10.Rt, 87.53.Bn, 87.53.Jw, 87.56.Bg |
format | Online Article Text |
id | pubmed-5711252 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2014 |
publisher | John Wiley and Sons Inc. |
record_format | MEDLINE/PubMed |
spelling | pubmed-57112522018-04-02 Monte Carlo calculation of beam quality correction for solid‐state detectors and phantom scatter correction at (137)Cs energy Selvam, T. Palani Mishra, Subhalaxmi Vishwakarma, R.S. J Appl Clin Med Phys Radiation Measurements Beam quality correction [Formula: see text] , which reflects the absorbed energy dependence of the detector, is calculated for solid‐state detector materials diamond, LiF, [Formula: see text] , and [Formula: see text] for the [Formula: see text] RTR brachytherapy source using the Monte Carlo‐based EGSnrc code system. The study also includes calculation of detector‐specific phantom scatter corrections [Formula: see text] for solid phantoms such as PMMA, polystyrene, RW1, solid water, virtual water, and plastic water. Above corrections are calculated as a function of distance r along the transverse axis of the source. [Formula: see text] is about unity for the [Formula: see text] detector. LiF detector shows a gradual decrease in [Formula: see text] with r (decrease is about 2% over the distance range of 1‐15 cm). Diamond detector shows a gradual increase in [Formula: see text] with r (about 3% larger than unity at 15 cm). In the case of [Formula: see text] detector, [Formula: see text] decreases with r steeply (about 14% over the distance range of 1‐15 cm). The study shows that some solid‐state detectors demonstrate distance‐dependent [Formula: see text] values, but the degree of deviation from unity depends on the type of solid phantom and the detector. PACS number: 87.10.Rt, 87.53.Bn, 87.53.Jw, 87.56.Bg John Wiley and Sons Inc. 2014-01-06 /pmc/articles/PMC5711252/ /pubmed/24423840 http://dx.doi.org/10.1120/jacmp.v15i1.4445 Text en © 2014 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 Measurements Selvam, T. Palani Mishra, Subhalaxmi Vishwakarma, R.S. Monte Carlo calculation of beam quality correction for solid‐state detectors and phantom scatter correction at (137)Cs energy |
title | Monte Carlo calculation of beam quality correction for solid‐state detectors and phantom scatter correction at (137)Cs energy |
title_full | Monte Carlo calculation of beam quality correction for solid‐state detectors and phantom scatter correction at (137)Cs energy |
title_fullStr | Monte Carlo calculation of beam quality correction for solid‐state detectors and phantom scatter correction at (137)Cs energy |
title_full_unstemmed | Monte Carlo calculation of beam quality correction for solid‐state detectors and phantom scatter correction at (137)Cs energy |
title_short | Monte Carlo calculation of beam quality correction for solid‐state detectors and phantom scatter correction at (137)Cs energy |
title_sort | monte carlo calculation of beam quality correction for solid‐state detectors and phantom scatter correction at (137)cs energy |
topic | Radiation Measurements |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5711252/ https://www.ncbi.nlm.nih.gov/pubmed/24423840 http://dx.doi.org/10.1120/jacmp.v15i1.4445 |
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