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Implementation and evaluation of an end‐to‐end IGRT test

The goal of this work was to develop and evaluate an end‐to‐end test for determining and verifying image‐guided radiation therapy setup accuracy relative to the radiation isocenter. This was done by placing a cube phantom with a central tungsten sphere directly on the treatment table and offset from...

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Detalles Bibliográficos
Autores principales: Kry, Stephen F., Jones, Jimmy, Childress, Nathan L.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2012
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5718216/
https://www.ncbi.nlm.nih.gov/pubmed/22955659
http://dx.doi.org/10.1120/jacmp.v13i5.3939
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author Kry, Stephen F.
Jones, Jimmy
Childress, Nathan L.
author_facet Kry, Stephen F.
Jones, Jimmy
Childress, Nathan L.
author_sort Kry, Stephen F.
collection PubMed
description The goal of this work was to develop and evaluate an end‐to‐end test for determining and verifying image‐guided radiation therapy setup accuracy relative to the radiation isocenter. This was done by placing a cube phantom with a central tungsten sphere directly on the treatment table and offset from isocenter either by 5.0 mm in the longitudinal, lateral, and vertical dimensions or by a random amount. A high‐resolution cone‐beam CT image was acquired and aligned with the tungsten sphere in the reference CT image. The table was shifted per this alignment, and megavoltage anterior–posterior and lateral images were acquired with the electronic portal imaging device. Agreement between the radiation isocenter (based on the MV field) and the center of the sphere (i.e., the alignment point based on kV imaging) was determined for each image via Winston‐Lutz analysis. This procedure was repeated 10 times to determine short‐term reproducibility, and then repeated daily for 51 days in a clinical setting. The short‐term reproducibility test yielded a mean 3D vector displacement of [Formula: see text] between the imaging‐based isocenter and the radiation isocenter, with a maximum displacement of 1.1 mm. The clinical reproducibility test yielded a mean displacement of [Formula: see text] with a maximum of 2.0 mm when the cube was offset by 5.0 mm, and a mean displacement of [Formula: see text] with a maximum of 1.8 mm when the cube was offset by a random amount. These differences were observed in all directions and were independent of the magnitude of the couch shift. This test was quick and easy to implement clinically and highlighted setup inaccuracies in an image‐guided radiation therapy environment. PACS numbers: 87.55.km; 87.55.Qr; 87.56.Fc
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spelling pubmed-57182162018-04-02 Implementation and evaluation of an end‐to‐end IGRT test Kry, Stephen F. Jones, Jimmy Childress, Nathan L. J Appl Clin Med Phys Radiation Oncology Physics The goal of this work was to develop and evaluate an end‐to‐end test for determining and verifying image‐guided radiation therapy setup accuracy relative to the radiation isocenter. This was done by placing a cube phantom with a central tungsten sphere directly on the treatment table and offset from isocenter either by 5.0 mm in the longitudinal, lateral, and vertical dimensions or by a random amount. A high‐resolution cone‐beam CT image was acquired and aligned with the tungsten sphere in the reference CT image. The table was shifted per this alignment, and megavoltage anterior–posterior and lateral images were acquired with the electronic portal imaging device. Agreement between the radiation isocenter (based on the MV field) and the center of the sphere (i.e., the alignment point based on kV imaging) was determined for each image via Winston‐Lutz analysis. This procedure was repeated 10 times to determine short‐term reproducibility, and then repeated daily for 51 days in a clinical setting. The short‐term reproducibility test yielded a mean 3D vector displacement of [Formula: see text] between the imaging‐based isocenter and the radiation isocenter, with a maximum displacement of 1.1 mm. The clinical reproducibility test yielded a mean displacement of [Formula: see text] with a maximum of 2.0 mm when the cube was offset by 5.0 mm, and a mean displacement of [Formula: see text] with a maximum of 1.8 mm when the cube was offset by a random amount. These differences were observed in all directions and were independent of the magnitude of the couch shift. This test was quick and easy to implement clinically and highlighted setup inaccuracies in an image‐guided radiation therapy environment. PACS numbers: 87.55.km; 87.55.Qr; 87.56.Fc John Wiley and Sons Inc. 2012-09-06 /pmc/articles/PMC5718216/ /pubmed/22955659 http://dx.doi.org/10.1120/jacmp.v13i5.3939 Text en © 2012 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
Kry, Stephen F.
Jones, Jimmy
Childress, Nathan L.
Implementation and evaluation of an end‐to‐end IGRT test
title Implementation and evaluation of an end‐to‐end IGRT test
title_full Implementation and evaluation of an end‐to‐end IGRT test
title_fullStr Implementation and evaluation of an end‐to‐end IGRT test
title_full_unstemmed Implementation and evaluation of an end‐to‐end IGRT test
title_short Implementation and evaluation of an end‐to‐end IGRT test
title_sort implementation and evaluation of an end‐to‐end igrt test
topic Radiation Oncology Physics
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5718216/
https://www.ncbi.nlm.nih.gov/pubmed/22955659
http://dx.doi.org/10.1120/jacmp.v13i5.3939
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