Methods of formation and control of radiation fields of M-30 microtron

IF 0.7 Q3 PHYSICS, MULTIDISCIPLINARY
M. Romanyuk, J. J. Gaynish, O. M. Turhovsky, M. V. Goshovsky, G. F. Pitchenko, I. Megela, O. Parlag, V. Maslyuk
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引用次数: 1

Abstract

articles on the formation of radiation (cid:28)elds and discusses their characteristics for nuclear physics installati-ons. It includes application of various methods of measuring the currents of charged particles, methods of detecting radiation (cid:28)elds using various recording media and changing the spatial distribution using (cid:29)attening (cid:28)lters. Attention is also paid to an alternative low-cost registration method using commercial window glass. For the (cid:16)Mikrotron M-30(cid:17) accelerator, parameters of the radiation (cid:28)elds were investigated on a metrological bench oriented along the electron beam at distances of 0(cid:21)400 cm from the M-30 beam output node. Dosimetric characteristics were determined using ionization chambers of the ROBOTRON dosimeter and a Faraday cylinder designed for diagnostics of electron beams with energies up to 30 MeV. In this work, to control the spatial uniformity of the radiation (cid:28)eld, we used a registration method based on glass plates; the degree of uniformity of the radiation (cid:28)eld was determined by a change in their optical characteristics, namely, the degree of darkening. For correctness of the obtained distributions, the radiation dose was limited to the region of linearity of glass darkening from the absorbed dose. The use of a radiation shaper ensured irradiation of samples with radiation of a uniform (cid:28)eld in the irradiation plane of 30%, which satis(cid:28)es the conditions of radiation tests for most objects. Analytical dependencies of the radiation dose on the distance to the output node M-30 were obtained using a Faraday cylinder. The combination of these dose dependencies of glass darkening, the spatial homogeneity of the (cid:28)elds, along with the dose dependence on the distance to the source node, made it possible to develop protocols for dosimetric tracking of the irradiation process for materials and devices for various purposes.
M-30微管辐射场的形成与控制方法
文章介绍了核物理装置辐射场的形成,并讨论了其特点。它包括测量带电粒子电流的各种方法的应用,使用各种记录介质检测辐射(cid:28)电场的方法,以及使用(cid:29)衰减(cid:28)字母改变空间分布的方法。还注意到使用商用玻璃窗的另一种低成本注册方法。对于(cid:16) microtron M-30(cid:17)加速器,在距离M-30束流输出节点0(cid:21)400 cm处沿电子束定向的测量台上,研究了辐射(cid:28)场的参数。使用ROBOTRON剂量计的电离室和用于诊断能量高达30 MeV的电子束的法拉第圆柱体来确定剂量学特性。在这项工作中,为了控制辐射(cid:28)场的空间均匀性,我们使用了基于玻璃板的配准方法;辐射场的均匀度(cid:28)由其光学特性的变化决定,即变暗程度。为了得到的分布的正确性,辐射剂量被限制在玻璃从吸收剂量变暗的线性区域内。使用辐射整形器,保证了样品在30%的辐照面辐照强度为均匀场(cid:28),满足大多数物体的辐射试验条件(cid:28)。利用法拉第柱体获得了辐射剂量与输出节点M-30距离的解析依赖关系。结合玻璃变暗的剂量依赖性、(cid:28)场的空间均匀性以及与源节点距离的剂量依赖性,可以制定用于各种用途的材料和设备辐照过程的剂量学跟踪方案。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Journal of Physical Studies
Journal of Physical Studies PHYSICS, MULTIDISCIPLINARY-
CiteScore
1.00
自引率
20.00%
发文量
19
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