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DISCRIMINATION METHOD FOR GAMMA RAY DOSES IN NEUTRON FIELDS USING AN IONIZATION CHAMBER WITH ATTENUATION FILTERS

机译:带有衰减滤波器的电离室对中子场伽玛射线剂量的判别方法

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Neutron fields produced by an accelerator-driven neutron source are generally mixed radiation fields that consist of fast neutrons and gamma rays. To estimate the biological effects of fast neutrons precisely, the gamma ray dose contamination must be evaluated in neutron fields. In this work, we developed a discrimination technique for absorbed doses (Co-60 gamma-ray equivalent) of fast neutrons and gamma rays using an ionization chamber. The filter thickness dependences of the absorbed doses of fast neutrons and gamma rays are different for a given filter material. Thus, the absorbed doses of each type of radiation were distinguished by fitting the dose attenuation curve, which was measured with an ionization chamber and attenuation filters, with a two-component exponential function. The absorbed dose of fast neutrons and gamma rays with no attenuation filter was evaluated from the y-intercept of the fitting function. This technique was demonstrated in two neutron fields produced by 4 MeV proton and deuteron bombardment of a Be-9 target. The thicknesses of the polyethylene attenuation filters were 0-350 mm. The dose attenuation coefficients of fast neutrons obtained by the two-component exponential fitting function for the Be-9(p,n)(9) and Be-9(d,n) reactions showed differences of 1.5 and 1.7%, respectively, from the reference measurements using a CR-39 plastic nuclear track detector. The absorbed dose contributions of gamma rays in neutrons fields of the Be-9(p,n)B-9 and Be-9(d,n) reactions were evaluated as 30.2 +/- 3.24% and 20.4 +/- 5.16%, respectively, without polyethylene filters.
机译:由加速器驱动的中子源产生的中子场通常是由快速中子和伽马射线组成的混合辐射场。为了精确估计快速中子的生物效应,必须在中子场中评估伽马射线剂量污染。在这项工作中,我们使用电离室为快速中子和伽马射线的吸收剂量(Co-60伽马射线当量)开发了一种判别技术。对于给定的过滤材料,快速中子和伽马射线吸收剂量对过滤器厚度的依赖性是不同的。因此,通过拟合剂量衰减曲线来区分每种类型的辐射的吸收剂量,该剂量衰减曲线是用电离室和衰减滤光片测量的,具有两组分指数函数。从拟合函数的y截距评估没有衰减滤波器的快中子和伽马射线的吸收剂量。这项技术在由4 MeV质子和氘核轰击Be-9靶所产生的两个中子场中得到证明。聚乙烯衰减滤波器的厚度为0-350mm。通过对Be-9(p,n)(9)和Be-9(d,n)反应的双组分指数拟合函数获得的快中子的剂量衰减系数与图9的差异分别为1.5和1.7%。使用CR-39塑料核径迹探测器进行参考测量。在Be-9(p,n)B-9和Be-9(d,n)反应的中子场中伽马射线的吸收剂量贡献评估为30.2 +/- 3.24%和20.4 +/- 5.16%,分别没有聚乙烯过滤器。

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