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[直线加速器机房迷路中铅屏蔽散射X射线的空气比释动能传输因子]

[Air kerma transmission factors of Scattered X-rays in the maze of a Linac room for lead shield].

作者信息

Kato Hideki

机构信息

S. S. Techno-engineering Corporation.

出版信息

Nihon Hoshasen Gijutsu Gakkai Zasshi. 2005 Jan 20;61(1):96-103. doi: 10.6009/jjrt.kj00003326619.

Abstract

Spectra of scattered X-rays in the maze of a Linac (X-ray energies of 4, 6, and 10 MV) room were estimated by means of the Monte Carlo simulation, and air kerma transmission factors of the X-rays scattered through a lead shield were evaluated based on those spectra. Spectra of scattered X-rays showed a maximum in the energy area below 200 keV. The higher the accelerated electron energy, also, the smaller the scattering angle that tended to spread to the higher energy area of the distribution of spectra. The air kerma transmission factor of 120 degrees scattered X-rays of 4 MV X-rays obtained in this study was larger than the transmission factors of 124 degrees scattered photons of (60)Co gamma rays through a lead shield given in ICRP. The air kerma transmission factors of 120 degrees scattered X-rays of 6 MV X-rays were smaller than the transmission factors of 90 degrees scattered photons of (60)Co gamma rays. The air kerma transmission factors of 120 degrees scattered X-rays of 10 MV X-rays was slightly larger than transmission factors of 90 degrees scattered photons of (60)Co gamma rays. Therefore, in the case of a 4 MV X-ray Linac room, the calculation method given in the "Manual of Practical Shield Calculation of Radiation Facilities (2000)" causes underestimation of leakage doses.

摘要

通过蒙特卡罗模拟估算了直线加速器(X射线能量为4、6和10兆电子伏特)机房迷宫中散射X射线的能谱,并基于这些能谱评估了穿过铅屏蔽散射的X射线的空气比释动能传输因子。散射X射线能谱在200千电子伏特以下的能量区域出现最大值。此外,加速电子能量越高,散射角越小,散射角倾向于扩展到能谱分布的更高能量区域。本研究中获得的4兆电子伏特X射线120度散射X射线的空气比释动能传输因子大于国际辐射防护委员会(ICRP)给出的(60)钴γ射线124度散射光子穿过铅屏蔽的传输因子。6兆电子伏特X射线120度散射X射线的空气比释动能传输因子小于(60)钴γ射线90度散射光子的传输因子。10兆电子伏特X射线120度散射X射线的空气比释动能传输因子略大于(60)钴γ射线90度散射光子的传输因子。因此,在4兆电子伏特X射线直线加速器机房的情况下,《辐射设施实用屏蔽计算手册(2000)》中给出的计算方法会导致对泄漏剂量的低估。

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