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Determination of saturation depth in aluminium and lead for 662 keV gamma rays

机译:662 keV伽马射线的铝和铅饱和深度的测定

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摘要

Compton scattering process is a powerful tool for determining electron distribution in an atom, non-destructive testing of a sample and reactor shielding. There is a significant radiation dose arising from the gamma rays backscattered from the surface of the shielding material. Present experiment is performed to study the contribution of multiply scattered photons as a function of thickness of the scatterer in the backscattering geometry. For this purpose a 137{sup left}Cs radioactive source of strength 110 mCi is used to obtain 662 keV gamma rays. The incident gamma rays irradiates the samples of aluminium and lead of different thicknesses in the backscattered geometry. The backscattered photons are detected by a Na1 (T1) scintillation detector of dimensions 51 mm diameter and 51 mm thickness at a scattering angle of 120°. To extract the contribution of the multiply scattered photons from the measured spectrum, a singly scattered photon spectrum is reconstructed analytically. Saturation depth is determined from experimental data and it comes out to be 90 mm and 9 mm for aluminium and lead respectively.
机译:康普顿散射过程是确定原子中电子分布,样品的无损检测和反应堆屏蔽的有力工具。从屏蔽材料的表面反向散射的伽马射线会产生大量的辐射剂量。进行本实验是为了研究在后向散射几何结构中多重散射光子对散射体厚度的影响。为此目的,使用强度为110 mCi的137 Cs放射源获得662 keV的伽马射线。入射的伽马射线以反向散射的几何形状辐照铝和不同厚度的铅样品。反向散射光子由直径为51毫米,厚度为51毫米的Na1(T1)闪烁探测器以120°的散射角进行探测。为了从测得的光谱中提取多重散射光子的贡献,可以解析地重建单个散射光子光谱。根据实验数据确定饱和深度,铝和铅的饱和深度分别为90 mm和9 mm。

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