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Transit and non‐transit 3D EPID dosimetry versus detector arrays for patient specific QA
PURPOSE: Despite their availability and simplicity of use, Electronic Portal Imaging Devices (EPIDs) have not yet replaced detector arrays for patient specific QA in 3D. The purpose of this study is to perform a large scale dosimetric evaluation of transit and non‐transit EPID dosimetry against abso...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
John Wiley and Sons Inc.
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6560233/ https://www.ncbi.nlm.nih.gov/pubmed/31083776 http://dx.doi.org/10.1002/acm2.12610 |
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author | Olaciregui‐Ruiz, Igor Vivas‐Maiques, Begoña Kaas, Jochem Perik, Thijs Wittkamper, Frits Mijnheer, Ben Mans, Anton |
author_facet | Olaciregui‐Ruiz, Igor Vivas‐Maiques, Begoña Kaas, Jochem Perik, Thijs Wittkamper, Frits Mijnheer, Ben Mans, Anton |
author_sort | Olaciregui‐Ruiz, Igor |
collection | PubMed |
description | PURPOSE: Despite their availability and simplicity of use, Electronic Portal Imaging Devices (EPIDs) have not yet replaced detector arrays for patient specific QA in 3D. The purpose of this study is to perform a large scale dosimetric evaluation of transit and non‐transit EPID dosimetry against absolute dose measurements in 3D. METHODS: After evaluating basic dosimetric characteristics of the EPID and two detector arrays (Octavius 1500 and Octavius 1000(SRS)), 3D dose distributions for 68 VMAT arcs, and 10 IMRT plans were reconstructed within the same phantom geometry using transit EPID dosimetry, non‐transit EPID dosimetry, and the Octavius 4D system. The reconstructed 3D dose distributions were directly compared by γ‐analysis (2L2 = 2% local/2 mm and 3G2 = 3% global/2 mm, 50% isodose) and by the percentage difference in median dose to the high dose volume (%∆HDV(D) (50)). RESULTS: Regarding dose rate dependency, dose linearity, and field size dependence, the agreement between EPID dosimetry and the two detector arrays was found to be within 1.0%. In the 2L2 γ‐comparison with Octavius 4D dose distributions, the average γ‐pass rate value was 92.2 ± 5.2%(1SD) and 94.1 ± 4.3%(1SD) for transit and non‐transit EPID dosimetry, respectively. 3G2 γ‐pass rate values were higher than 95% in 150/156 cases. %∆HDV(D) (50) values were within 2% in 134/156 cases and within 3% in 155/156 cases. With regard to the clinical classification of alerts, 97.5% of the treatments were equally classified by EPID dosimetry and Octavius 4D. CONCLUSION: Transit and non‐transit EPID dosimetry are equivalent in dosimetric terms to conventional detector arrays for patient specific QA. Non‐transit 3D EPID dosimetry can be readily used for pre‐treatment patient specific QA of IMRT and VMAT, eliminating the need of phantom positioning. |
format | Online Article Text |
id | pubmed-6560233 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | John Wiley and Sons Inc. |
record_format | MEDLINE/PubMed |
spelling | pubmed-65602332019-06-17 Transit and non‐transit 3D EPID dosimetry versus detector arrays for patient specific QA Olaciregui‐Ruiz, Igor Vivas‐Maiques, Begoña Kaas, Jochem Perik, Thijs Wittkamper, Frits Mijnheer, Ben Mans, Anton J Appl Clin Med Phys Radiation Oncology Physics PURPOSE: Despite their availability and simplicity of use, Electronic Portal Imaging Devices (EPIDs) have not yet replaced detector arrays for patient specific QA in 3D. The purpose of this study is to perform a large scale dosimetric evaluation of transit and non‐transit EPID dosimetry against absolute dose measurements in 3D. METHODS: After evaluating basic dosimetric characteristics of the EPID and two detector arrays (Octavius 1500 and Octavius 1000(SRS)), 3D dose distributions for 68 VMAT arcs, and 10 IMRT plans were reconstructed within the same phantom geometry using transit EPID dosimetry, non‐transit EPID dosimetry, and the Octavius 4D system. The reconstructed 3D dose distributions were directly compared by γ‐analysis (2L2 = 2% local/2 mm and 3G2 = 3% global/2 mm, 50% isodose) and by the percentage difference in median dose to the high dose volume (%∆HDV(D) (50)). RESULTS: Regarding dose rate dependency, dose linearity, and field size dependence, the agreement between EPID dosimetry and the two detector arrays was found to be within 1.0%. In the 2L2 γ‐comparison with Octavius 4D dose distributions, the average γ‐pass rate value was 92.2 ± 5.2%(1SD) and 94.1 ± 4.3%(1SD) for transit and non‐transit EPID dosimetry, respectively. 3G2 γ‐pass rate values were higher than 95% in 150/156 cases. %∆HDV(D) (50) values were within 2% in 134/156 cases and within 3% in 155/156 cases. With regard to the clinical classification of alerts, 97.5% of the treatments were equally classified by EPID dosimetry and Octavius 4D. CONCLUSION: Transit and non‐transit EPID dosimetry are equivalent in dosimetric terms to conventional detector arrays for patient specific QA. Non‐transit 3D EPID dosimetry can be readily used for pre‐treatment patient specific QA of IMRT and VMAT, eliminating the need of phantom positioning. John Wiley and Sons Inc. 2019-05-13 /pmc/articles/PMC6560233/ /pubmed/31083776 http://dx.doi.org/10.1002/acm2.12610 Text en © 2019 The Authors. Journal of Applied Clinical Medical Physics published by Wiley Periodicals, Inc. on behalf of American Association of Physicists in Medicine This is an open access article under the terms of the http://creativecommons.org/licenses/by/4.0/ License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited. |
spellingShingle | Radiation Oncology Physics Olaciregui‐Ruiz, Igor Vivas‐Maiques, Begoña Kaas, Jochem Perik, Thijs Wittkamper, Frits Mijnheer, Ben Mans, Anton Transit and non‐transit 3D EPID dosimetry versus detector arrays for patient specific QA |
title | Transit and non‐transit 3D EPID dosimetry versus detector arrays for patient specific QA
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title_full | Transit and non‐transit 3D EPID dosimetry versus detector arrays for patient specific QA
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title_fullStr | Transit and non‐transit 3D EPID dosimetry versus detector arrays for patient specific QA
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title_full_unstemmed | Transit and non‐transit 3D EPID dosimetry versus detector arrays for patient specific QA
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title_short | Transit and non‐transit 3D EPID dosimetry versus detector arrays for patient specific QA
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title_sort | transit and non‐transit 3d epid dosimetry versus detector arrays for patient specific qa |
topic | Radiation Oncology Physics |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6560233/ https://www.ncbi.nlm.nih.gov/pubmed/31083776 http://dx.doi.org/10.1002/acm2.12610 |
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