Estimation of surface doses in the presence of an air gap under a bolus for a 6 MV clinical photon beam - a phantom study.

IF 1.5 4区 环境科学与生态学 Q3 BIOLOGY
Radiation and Environmental Biophysics Pub Date : 2025-03-01 Epub Date: 2025-01-28 DOI:10.1007/s00411-025-01106-6
Dilson Lobo, Challapalli Srinivas, Sourjya Banerjee, M S Athiyamaan, K Johan Sunny, Abhishek Krishna
{"title":"Estimation of surface doses in the presence of an air gap under a bolus for a 6 MV clinical photon beam - a phantom study.","authors":"Dilson Lobo, Challapalli Srinivas, Sourjya Banerjee, M S Athiyamaan, K Johan Sunny, Abhishek Krishna","doi":"10.1007/s00411-025-01106-6","DOIUrl":null,"url":null,"abstract":"<p><p>Goal of the present study was to develop and build a phantom that replicates the air gaps under a gel bolus and to estimate the surface dose (D<sub>surf</sub>) under normal incidence with a 6 MV photon beam. For this, an acrylic phantom with 10 plates, each including five open slots (one in the centre and four off axis) with a size of 2 cm × 2 cm at depths of 0.54 cm, 0.72 cm, 0.90 cm, 1.26 cm, and 1.62 cm from the phantom's surface was used. Computed tomography image sets were obtained without and with a gel bolus (thickness: 2 mm, 4 mm, and 6 mm) placed on top of the phantom. Dose calculations were performed with the XiO treatment planning system (TPS) for a 6 MV photon beam at normal incidence and a field size of 15 cm × 15 cm that covered all the slots. A virtual bolus in TPS was employed in CT picture sets that did not include a bolus. Six points of interest at a depth of 1 mm from the surface contour of each slot were used to determine the mean surface dose (D<sub>surf</sub>) estimated by the TPS with and without the presence of a bolus. It turned out that, as the depth of the air gap (between skin surface and bolus surface) increased from 0.54 cm to 1.62 cm, there was a 25.2% increase in D<sub>surf</sub> without bolus, followed by an increase of 7.6%, 6.4%, and 7.7% for a virtual bolus with 2 mm, 4 mm, and 6 mm thickness, while corresponding increases were 14.8%, 14.3%, and 8.3% for an actual bolus, respectively. However, as the thickness of the air gap increased, D<sub>surf</sub> under the bolus decreased (from - 17.5% to -18.8%, and from - 10.4% to -16.9%, for a virtual and a physical bolus, respectively). It is concluded that, to ensure a homogeneous D<sub>surf</sub> across the treatment area, extra attention should be given while utilizing a bolus in clinical radiation applications, to avoid any air gaps under the bolus.</p>","PeriodicalId":21002,"journal":{"name":"Radiation and Environmental Biophysics","volume":" ","pages":"77-83"},"PeriodicalIF":1.5000,"publicationDate":"2025-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11971206/pdf/","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Radiation and Environmental Biophysics","FirstCategoryId":"93","ListUrlMain":"https://doi.org/10.1007/s00411-025-01106-6","RegionNum":4,"RegionCategory":"环境科学与生态学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2025/1/28 0:00:00","PubModel":"Epub","JCR":"Q3","JCRName":"BIOLOGY","Score":null,"Total":0}
引用次数: 0

Abstract

Goal of the present study was to develop and build a phantom that replicates the air gaps under a gel bolus and to estimate the surface dose (Dsurf) under normal incidence with a 6 MV photon beam. For this, an acrylic phantom with 10 plates, each including five open slots (one in the centre and four off axis) with a size of 2 cm × 2 cm at depths of 0.54 cm, 0.72 cm, 0.90 cm, 1.26 cm, and 1.62 cm from the phantom's surface was used. Computed tomography image sets were obtained without and with a gel bolus (thickness: 2 mm, 4 mm, and 6 mm) placed on top of the phantom. Dose calculations were performed with the XiO treatment planning system (TPS) for a 6 MV photon beam at normal incidence and a field size of 15 cm × 15 cm that covered all the slots. A virtual bolus in TPS was employed in CT picture sets that did not include a bolus. Six points of interest at a depth of 1 mm from the surface contour of each slot were used to determine the mean surface dose (Dsurf) estimated by the TPS with and without the presence of a bolus. It turned out that, as the depth of the air gap (between skin surface and bolus surface) increased from 0.54 cm to 1.62 cm, there was a 25.2% increase in Dsurf without bolus, followed by an increase of 7.6%, 6.4%, and 7.7% for a virtual bolus with 2 mm, 4 mm, and 6 mm thickness, while corresponding increases were 14.8%, 14.3%, and 8.3% for an actual bolus, respectively. However, as the thickness of the air gap increased, Dsurf under the bolus decreased (from - 17.5% to -18.8%, and from - 10.4% to -16.9%, for a virtual and a physical bolus, respectively). It is concluded that, to ensure a homogeneous Dsurf across the treatment area, extra attention should be given while utilizing a bolus in clinical radiation applications, to avoid any air gaps under the bolus.

估计6毫伏临床光子束中存在气隙时的表面剂量-一项幻象研究。
本研究的目的是开发和建立一个模拟凝胶丸下气隙的模体,并估计正常入射下6 MV光子束的表面剂量(Dsurf)。为此,使用了一个有10个板的丙烯酸体,每个板包括5个开槽(一个在中心,四个离轴),尺寸为2厘米× 2厘米,深度分别为0.54厘米、0.72厘米、0.90厘米、1.26厘米和1.62厘米,距离体表面。将凝胶丸(厚度分别为2mm、4mm和6mm)放置在幻膜顶部,在没有凝胶丸的情况下获得计算机断层扫描图像集。使用XiO治疗计划系统(TPS)计算正常入射的6 MV光子束和覆盖所有狭缝的15 cm × 15 cm场的剂量。在不包括丸的CT图像集中采用TPS中的虚拟丸。在距离每个狭缝表面轮廓1mm深度处的六个兴趣点被用来确定有和没有丸存在的TPS估计的平均表面剂量(Dsurf)。结果表明,当皮肤表面与丸表面之间的气隙深度从0.54 cm增加到1.62 cm时,无丸的Dsurf增加了25.2%,其次是厚度为2mm、4mm和6mm的虚拟丸,分别增加了7.6%、6.4%和7.7%,而实际丸的相应增加分别为14.8%、14.3%和8.3%。然而,随着气隙厚度的增加,弹下的Dsurf减小(虚拟弹和物理弹分别从- 17.5%减小到-18.8%,从- 10.4%减小到-16.9%)。结论是,为了确保整个治疗区域的均匀辐射,在临床放射应用中使用丸剂时应特别注意,以避免丸剂下的任何气隙。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
CiteScore
4.00
自引率
5.90%
发文量
53
审稿时长
>36 weeks
期刊介绍: This journal is devoted to fundamental and applied issues in radiation research and biophysics. The topics may include: Biophysics of ionizing radiation: radiation physics and chemistry, radiation dosimetry, radiobiology, radioecology, biophysical foundations of medical applications of radiation, and radiation protection. Biological effects of radiation: experimental or theoretical work on molecular or cellular effects; relevance of biological effects for risk assessment; biological effects of medical applications of radiation; relevance of radiation for biosphere and in space; modelling of ecosystems; modelling of transport processes of substances in biotic systems. Risk assessment: epidemiological studies of cancer and non-cancer effects; quantification of risk including exposures to radiation and confounding factors Contributions to these topics may include theoretical-mathematical and experimental material, as well as description of new techniques relevant for the study of these issues. They can range from complex radiobiological phenomena to issues in health physics and environmental protection.
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信