用放射性致色膜周期性测量固定龙门系统中的被动质子束宽度

T. Shimozato, K. Yasui, Hireto Kinou, Fumiaki Komatsu
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引用次数: 0

摘要

背景与目的:双散射法和点扫描法等辐照方法已被应用于质子束治疗装置中。在散射方法中,使用脊状滤波器或距离调制轮来产生展开的布拉格峰,但由于入射光束的位置偏差,布拉格峰在患者位置的分布可能会发生变化。因此,即使在散射方法中,对光束入射位置的评估也是非常重要的。为了研究质子束在进入RMW前的宽度和分布,在输送管的出口和剖面监测探测器的入口安装了一个放射性变色膜。方法:采用薄膜法测量输送管出口和监测探测器入口的光束分布。光束宽度是根据分布得到的剖面的最大一半处的全宽度来测量的。每月进行一次测量,持续10个月。结果:输送管出口水平方向输出宽度为1.82 ~ 2.30 mm,垂直方向输出宽度为4.25 ~ 5.33 mm。从监测探测器入口输出水平方向宽度为2.16 ~ 2.67 mm,垂直方向宽度为4.06 ~ 5.31 mm的光束。监测探测器入口10个月最大宽度波动为水平方向0.55 mm,垂直方向1.26 mm。结论:质子束的分布是在散射器散射前得到的,然后我们提出了一种每月定期测量和监测质子束分布变化的方法。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Periodic Measurements of Passive Proton Beam Width Using Radiochromic Film in Fixed Gantry System
Background and Aim: Irradiation methods such as double scattering method and spot scanning method have been used in proton beam treatment devices. In the scattering method, a ridge filter or a range modulation wheel is used to create a spread-out Bragg peak, but the distribution at the patient position may change due to positional deviation of the incident beam. Therefore, assessment of the incident position of the beam is very important even in the scattering method. To investigate the width and distribution of the proton beam before entering the RMW, a radiochromic film was installed at the outlet of the transport pipe and the entrance of the profile-monitoring detector. Methods: In this study, the distributions of the beam at the exit of the transport pipe and the entrance of the monitor detector were measured using films. The beam width was measured from the full width at half maximum of the profile obtained from the distribution. Measurements were conducted every month for 10 months. Results: Beams of widths ranging from 1.82 to 2.30 mm in the horizontal direction and 4.25 to 5.33 mm in the vertical direction were outputted from the exit of the transport pipe. Beams of widths ranging from 2.16 to 2.67 mm in the horizontal direction and 4.06 to 5.31 mm in the vertical direction were outputted from the entrance of the monitor detector. The maximum width fluctuation for 10 months was 0.55 mm in the horizontal direction and 1.26 mm in the vertical direction at the entrance of the monitor detector. Conclusions: The distribution was obtained before the proton beam was scattered by the scatterer, and then we propose a method to periodically measure and monitor the changes in the beam distributions every month.
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