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Deriving detector‐specific correction factors for rectangular small fields using a scintillator detector

The goal of this study was to investigate small field output factors (OFs) for flattening filter‐free (FFF) beams on a dedicated stereotactic linear accelerator‐based system. From this data, the collimator exchange effect was quantified, and detector‐specific correction factors were generated. Outpu...

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Autores principales: Qin, Yujiao, Zhong, Hualiang, Wen, Ning, Snyder, Karen, Huang, Yimei, Chetty, Indrin J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5690516/
https://www.ncbi.nlm.nih.gov/pubmed/27929510
http://dx.doi.org/10.1120/jacmp.v17i6.6433
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author Qin, Yujiao
Zhong, Hualiang
Wen, Ning
Snyder, Karen
Huang, Yimei
Chetty, Indrin J.
author_facet Qin, Yujiao
Zhong, Hualiang
Wen, Ning
Snyder, Karen
Huang, Yimei
Chetty, Indrin J.
author_sort Qin, Yujiao
collection PubMed
description The goal of this study was to investigate small field output factors (OFs) for flattening filter‐free (FFF) beams on a dedicated stereotactic linear accelerator‐based system. From this data, the collimator exchange effect was quantified, and detector‐specific correction factors were generated. Output factors for 16 jaw‐collimated small fields (from 0.5 to 2 cm) were measured using five different detectors including an ion chamber (CC01), a stereotactic field diode (SFD), a diode detector (Edge), Gafchromic film (EBT3), and a plastic scintillator detector (PSD, W1). Chamber, diodes, and PSD measurements were performed in a Wellhofer water tank, while films were irradiated in solid water at 100 cm source‐to‐surface distance and 10 cm depth. The collimator exchange effect was quantified for rectangular fields. Monte Carlo (MC) simulations of the measured configurations were also performed using the EGSnrc/DOSXYZnrc code. Output factors measured by the PSD and verified against film and MC calculations were chosen as the benchmark measurements. Compared with plastic scintillator detector (PSD), the small volume ion chamber (CC01) underestimated output factors by an average of [Formula: see text] for [Formula: see text] square field). The stereotactic diode (SFD) overestimated output factors by [Formula: see text] for [Formula: see text] rectangular field). The other diode detector (Edge) also overestimated the OFs by an average of [Formula: see text] for [Formula: see text] square field). Gafchromic film (EBT3) measurements and MC calculations agreed with the scintillator detector measurements within [Formula: see text] and [Formula: see text] , respectively. Across all the X and Y jaw combinations, the average collimator exchange effect was computed: [Formula: see text] (CC01), [Formula: see text] (SFD), [Formula: see text] (Edge diode), [Formula: see text] (Monte Carlo), [Formula: see text] (film), and [Formula: see text] (PSD). Small field detectors should be used with caution with a clear understanding of their behaviors, especially for FFF beams and small, elongated fields. The scintillator detector exhibited good agreement against Gafchromic film measurements and MC simulations over the range of field sizes studied. The collimator exchange effect was found to be important at these small field sizes. Detector‐specific correction factors were computed using the scintillator measurements as the benchmark. PACS number(s): 87.56.Fc
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spelling pubmed-56905162018-04-02 Deriving detector‐specific correction factors for rectangular small fields using a scintillator detector Qin, Yujiao Zhong, Hualiang Wen, Ning Snyder, Karen Huang, Yimei Chetty, Indrin J. J Appl Clin Med Phys Radiation Measurements The goal of this study was to investigate small field output factors (OFs) for flattening filter‐free (FFF) beams on a dedicated stereotactic linear accelerator‐based system. From this data, the collimator exchange effect was quantified, and detector‐specific correction factors were generated. Output factors for 16 jaw‐collimated small fields (from 0.5 to 2 cm) were measured using five different detectors including an ion chamber (CC01), a stereotactic field diode (SFD), a diode detector (Edge), Gafchromic film (EBT3), and a plastic scintillator detector (PSD, W1). Chamber, diodes, and PSD measurements were performed in a Wellhofer water tank, while films were irradiated in solid water at 100 cm source‐to‐surface distance and 10 cm depth. The collimator exchange effect was quantified for rectangular fields. Monte Carlo (MC) simulations of the measured configurations were also performed using the EGSnrc/DOSXYZnrc code. Output factors measured by the PSD and verified against film and MC calculations were chosen as the benchmark measurements. Compared with plastic scintillator detector (PSD), the small volume ion chamber (CC01) underestimated output factors by an average of [Formula: see text] for [Formula: see text] square field). The stereotactic diode (SFD) overestimated output factors by [Formula: see text] for [Formula: see text] rectangular field). The other diode detector (Edge) also overestimated the OFs by an average of [Formula: see text] for [Formula: see text] square field). Gafchromic film (EBT3) measurements and MC calculations agreed with the scintillator detector measurements within [Formula: see text] and [Formula: see text] , respectively. Across all the X and Y jaw combinations, the average collimator exchange effect was computed: [Formula: see text] (CC01), [Formula: see text] (SFD), [Formula: see text] (Edge diode), [Formula: see text] (Monte Carlo), [Formula: see text] (film), and [Formula: see text] (PSD). Small field detectors should be used with caution with a clear understanding of their behaviors, especially for FFF beams and small, elongated fields. The scintillator detector exhibited good agreement against Gafchromic film measurements and MC simulations over the range of field sizes studied. The collimator exchange effect was found to be important at these small field sizes. Detector‐specific correction factors were computed using the scintillator measurements as the benchmark. PACS number(s): 87.56.Fc John Wiley and Sons Inc. 2016-11-08 /pmc/articles/PMC5690516/ /pubmed/27929510 http://dx.doi.org/10.1120/jacmp.v17i6.6433 Text en © 2016 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
Qin, Yujiao
Zhong, Hualiang
Wen, Ning
Snyder, Karen
Huang, Yimei
Chetty, Indrin J.
Deriving detector‐specific correction factors for rectangular small fields using a scintillator detector
title Deriving detector‐specific correction factors for rectangular small fields using a scintillator detector
title_full Deriving detector‐specific correction factors for rectangular small fields using a scintillator detector
title_fullStr Deriving detector‐specific correction factors for rectangular small fields using a scintillator detector
title_full_unstemmed Deriving detector‐specific correction factors for rectangular small fields using a scintillator detector
title_short Deriving detector‐specific correction factors for rectangular small fields using a scintillator detector
title_sort deriving detector‐specific correction factors for rectangular small fields using a scintillator detector
topic Radiation Measurements
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5690516/
https://www.ncbi.nlm.nih.gov/pubmed/27929510
http://dx.doi.org/10.1120/jacmp.v17i6.6433
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