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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...

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Autores principales: Selvam, T. Palani, Mishra, Subhalaxmi, Vishwakarma, R.S.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2014
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
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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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