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Performance optimization of the Varian aS500 EPID system

Today, electronic portal imaging devices (EPIDs) are widely used as a replacement to portal films for patient position verification, but the image quality is not always optimal. The general aim of this study was to optimize the acquisition parameters of an amorphous silicon EPID commercially availab...

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Autores principales: Berger, Lucie, François, Pascal, Gaboriaud, Geneviève, Rosenwald, Jean‐Claude
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2006
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5722482/
https://www.ncbi.nlm.nih.gov/pubmed/16518322
http://dx.doi.org/10.1120/jacmp.v7i1.2158
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author Berger, Lucie
François, Pascal
Gaboriaud, Geneviève
Rosenwald, Jean‐Claude
author_facet Berger, Lucie
François, Pascal
Gaboriaud, Geneviève
Rosenwald, Jean‐Claude
author_sort Berger, Lucie
collection PubMed
description Today, electronic portal imaging devices (EPIDs) are widely used as a replacement to portal films for patient position verification, but the image quality is not always optimal. The general aim of this study was to optimize the acquisition parameters of an amorphous silicon EPID commercially available for clinical use in radiation therapy with the view to avoid saturation of the system. Special attention was paid to selection of the parameter corresponding to the number of rows acquired between accelerator pulses (NRP) for various beam energies and dose rates. The image acquisition system (IAS2) has been studied, and portal image acquisition was found to be strongly dependent on the accelerator pulse frequency. This frequency is set for each “energy — dose rate” combination of the linear accelerator. For all combinations, the image acquisition parameters were systematically changed to determine their influence on the performances of the Varian aS500 EPID system. New parameters such as the maximum number of rows (MNR) and the number of pulses per frame (NPF) were introduced to explain portal image acquisition theory. Theoretical and experimental values of MNR and NPF were compared, and they were in good agreement. Other results showed that NRP had a major influence on detector saturation and dose per image. A rule of thumb was established to determine the optimum NRP value to be used. This practical application was illustrated by a clinical example in which the saturation of the aSi EPID was avoided by NRP optimization. Moreover, an additional study showed that image quality was relatively insensitive to this parameter. PACS numbers: 87.53.Oq; 87.59.Jq
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spelling pubmed-57224822018-04-02 Performance optimization of the Varian aS500 EPID system Berger, Lucie François, Pascal Gaboriaud, Geneviève Rosenwald, Jean‐Claude J Appl Clin Med Phys Radiation Measurements Today, electronic portal imaging devices (EPIDs) are widely used as a replacement to portal films for patient position verification, but the image quality is not always optimal. The general aim of this study was to optimize the acquisition parameters of an amorphous silicon EPID commercially available for clinical use in radiation therapy with the view to avoid saturation of the system. Special attention was paid to selection of the parameter corresponding to the number of rows acquired between accelerator pulses (NRP) for various beam energies and dose rates. The image acquisition system (IAS2) has been studied, and portal image acquisition was found to be strongly dependent on the accelerator pulse frequency. This frequency is set for each “energy — dose rate” combination of the linear accelerator. For all combinations, the image acquisition parameters were systematically changed to determine their influence on the performances of the Varian aS500 EPID system. New parameters such as the maximum number of rows (MNR) and the number of pulses per frame (NPF) were introduced to explain portal image acquisition theory. Theoretical and experimental values of MNR and NPF were compared, and they were in good agreement. Other results showed that NRP had a major influence on detector saturation and dose per image. A rule of thumb was established to determine the optimum NRP value to be used. This practical application was illustrated by a clinical example in which the saturation of the aSi EPID was avoided by NRP optimization. Moreover, an additional study showed that image quality was relatively insensitive to this parameter. PACS numbers: 87.53.Oq; 87.59.Jq John Wiley and Sons Inc. 2006-02-21 /pmc/articles/PMC5722482/ /pubmed/16518322 http://dx.doi.org/10.1120/jacmp.v7i1.2158 Text en © 2006 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
Berger, Lucie
François, Pascal
Gaboriaud, Geneviève
Rosenwald, Jean‐Claude
Performance optimization of the Varian aS500 EPID system
title Performance optimization of the Varian aS500 EPID system
title_full Performance optimization of the Varian aS500 EPID system
title_fullStr Performance optimization of the Varian aS500 EPID system
title_full_unstemmed Performance optimization of the Varian aS500 EPID system
title_short Performance optimization of the Varian aS500 EPID system
title_sort performance optimization of the varian as500 epid system
topic Radiation Measurements
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5722482/
https://www.ncbi.nlm.nih.gov/pubmed/16518322
http://dx.doi.org/10.1120/jacmp.v7i1.2158
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