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18兆电子伏、28兆电子伏和38兆电子伏电子束在厚靶中产生的轫致辐射和二次电子吸收剂量的角分布。

Angular distributions of absorbed dose of Bremsstrahlung and secondary electrons induced by 18-, 28- and 38-MeV electron beams in thick targets.

作者信息

Takada Masashi, Kosako Kazuaki, Oishi Koji, Nakamura Takashi, Sato Kouichi, Kamiyama Takashi, Kiyanagi Yoshiaki

机构信息

National Institute of Radiological Sciences, Chiba 263-8555, Japan.

出版信息

Radiat Prot Dosimetry. 2013 Mar;153(3):369-83. doi: 10.1093/rpd/ncs114. Epub 2012 Jul 3.

Abstract

Angular distributions of absorbed dose of Bremsstrahlung photons and secondary electrons at a wide range of emission angles from 0 to 135°, were experimentally obtained using an ion chamber with a 0.6 cm(3) air volume covered with or without a build-up cap. The Bremsstrahlung photons and electrons were produced by 18-, 28- and 38-MeV electron beams bombarding tungsten, copper, aluminium and carbon targets. The absorbed doses were also calculated from simulated photon and electron energy spectra by multiplying simulated response functions of the ion chambers, simulated with the MCNPX code. Calculated-to-experimental (C/E) dose ratios obtained are from 0.70 to 1.57 for high-Z targets of W and Cu, from 15 to 135° and the C/E range from 0.6 to 1.4 at 0°; however, the values of C/E for low-Z targets of Al and C are from 0.5 to 1.8 from 0 to 135°. Angular distributions at the forward angles decrease with increasing angles; on the other hand, the angular distributions at the backward angles depend on the target species. The dependences of absorbed doses on electron energy and target thickness were compared between the measured and simulated results. The attenuation profiles of absorbed doses of Bremsstrahlung beams at 0, 30 and 135° were also measured.

摘要

使用一个空气体积为0.6立方厘米、带有或不带有累积帽的电离室,通过实验获得了在0至135°的宽发射角范围内轫致辐射光子和二次电子的吸收剂量角分布。轫致辐射光子和电子由18兆电子伏、28兆电子伏和38兆电子伏的电子束轰击钨、铜、铝和碳靶产生。吸收剂量也通过将用MCNPX代码模拟的电离室响应函数与模拟的光子和电子能谱相乘来计算。对于钨和铜等高Z靶,在15至135°时计算得到的与实验(C/E)剂量比为0.70至1.57,在0°时C/E范围为0.6至1.4;然而,对于铝和碳等低Z靶,在0至135°时C/E值为0.5至1.8。前向角的角分布随角度增加而减小;另一方面,后向角的角分布取决于靶物质种类。比较了测量结果和模拟结果中吸收剂量对电子能量和靶厚度的依赖性。还测量了在0°、30°和135°时轫致辐射束吸收剂量的衰减曲线。

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