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Independent monitor unit verification for dynamic flattened beam plans on the Halcyon linac

Independent monitor unit verification (MUV) methods for the dynamic beam‐flattening (DBF) technique have not been established. The purpose of this study was to clarify whether MU values for the DBF technique can be calculated using in‐air and in‐water output ratios (S (c) and S (cp)). S (c) and S (c...

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Autores principales: Kubo, Kazuki, Tamura, Mikoto, Matsumoto, Kenji, Otsuka, Masakazu, Monzen, Hajime
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9859998/
https://www.ncbi.nlm.nih.gov/pubmed/36265085
http://dx.doi.org/10.1002/acm2.13807
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author Kubo, Kazuki
Tamura, Mikoto
Matsumoto, Kenji
Otsuka, Masakazu
Monzen, Hajime
author_facet Kubo, Kazuki
Tamura, Mikoto
Matsumoto, Kenji
Otsuka, Masakazu
Monzen, Hajime
author_sort Kubo, Kazuki
collection PubMed
description Independent monitor unit verification (MUV) methods for the dynamic beam‐flattening (DBF) technique have not been established. The purpose of this study was to clarify whether MU values for the DBF technique can be calculated using in‐air and in‐water output ratios (S (c) and S (cp)). S (c) and S (cp) were measured in the DBF mode, and the phantom scatter factor (S (p)) was calculated. The difference between calculated and planned MUs with square and rectangle fields and clinical plans for different treatment sites was also evaluated. S (c) values for the 4 × 4 to 24 × 24 cm(2) fields of the distal multi‐leaf collimator (MLC) layer at 2‐cm intervals were 0.887, 0.815, 0.715, 0.716, 0.611, 0.612, 0.511, 0.373, 0.374, 0.375, and 0.374, respectively. No collimator exchange effect was observed. S (c) also depends slightly on the field size of the distal MLC layer. If the distal‐MLC‐layered field size was less than 20% of the corresponding MLC sequence size in the proximal MLC layer, S (c) was affected by >1%, which was compensated using a correction factor (CF). S (p) increased as the field sizes of the MLC sequence and distal MLC leaves increased. MUs calculated using measured S (c), S (p), and CF for square and rectangle fields agreed with planned MUs within ±1.2%. A larger difference (−1.5%) between calculated and planned MUs was observed for clinical plans, whereas differences in MUs were within 2 MU for most fields (56 out of 64 fields). MU calculation for the DBF technique can be performed with S (c), S (p), and CF for independent MUV.
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spelling pubmed-98599982023-01-24 Independent monitor unit verification for dynamic flattened beam plans on the Halcyon linac Kubo, Kazuki Tamura, Mikoto Matsumoto, Kenji Otsuka, Masakazu Monzen, Hajime J Appl Clin Med Phys Radiation Oncology Physics Independent monitor unit verification (MUV) methods for the dynamic beam‐flattening (DBF) technique have not been established. The purpose of this study was to clarify whether MU values for the DBF technique can be calculated using in‐air and in‐water output ratios (S (c) and S (cp)). S (c) and S (cp) were measured in the DBF mode, and the phantom scatter factor (S (p)) was calculated. The difference between calculated and planned MUs with square and rectangle fields and clinical plans for different treatment sites was also evaluated. S (c) values for the 4 × 4 to 24 × 24 cm(2) fields of the distal multi‐leaf collimator (MLC) layer at 2‐cm intervals were 0.887, 0.815, 0.715, 0.716, 0.611, 0.612, 0.511, 0.373, 0.374, 0.375, and 0.374, respectively. No collimator exchange effect was observed. S (c) also depends slightly on the field size of the distal MLC layer. If the distal‐MLC‐layered field size was less than 20% of the corresponding MLC sequence size in the proximal MLC layer, S (c) was affected by >1%, which was compensated using a correction factor (CF). S (p) increased as the field sizes of the MLC sequence and distal MLC leaves increased. MUs calculated using measured S (c), S (p), and CF for square and rectangle fields agreed with planned MUs within ±1.2%. A larger difference (−1.5%) between calculated and planned MUs was observed for clinical plans, whereas differences in MUs were within 2 MU for most fields (56 out of 64 fields). MU calculation for the DBF technique can be performed with S (c), S (p), and CF for independent MUV. John Wiley and Sons Inc. 2022-10-20 /pmc/articles/PMC9859998/ /pubmed/36265085 http://dx.doi.org/10.1002/acm2.13807 Text en © 2022 The Authors. Journal of Applied Clinical Medical Physics published by Wiley Periodicals, LLC on behalf of The American Association of Physicists in Medicine. https://creativecommons.org/licenses/by/4.0/This is an open access article under the terms of the http://creativecommons.org/licenses/by/4.0/ (https://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
Kubo, Kazuki
Tamura, Mikoto
Matsumoto, Kenji
Otsuka, Masakazu
Monzen, Hajime
Independent monitor unit verification for dynamic flattened beam plans on the Halcyon linac
title Independent monitor unit verification for dynamic flattened beam plans on the Halcyon linac
title_full Independent monitor unit verification for dynamic flattened beam plans on the Halcyon linac
title_fullStr Independent monitor unit verification for dynamic flattened beam plans on the Halcyon linac
title_full_unstemmed Independent monitor unit verification for dynamic flattened beam plans on the Halcyon linac
title_short Independent monitor unit verification for dynamic flattened beam plans on the Halcyon linac
title_sort independent monitor unit verification for dynamic flattened beam plans on the halcyon linac
topic Radiation Oncology Physics
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9859998/
https://www.ncbi.nlm.nih.gov/pubmed/36265085
http://dx.doi.org/10.1002/acm2.13807
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