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Klein-Nishina electronic cross-section, Compton cross sections, and buildup factor of wax for radiation shielding and protection

机译:Klein-Nishina电子横截面,康普顿横截面,以及用于辐射屏蔽和保护的蜡的积累系数

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Klein-Nishina scattering cross-sections, Compton scattering, mass attenuation and energy transfer cross-sections, linear attenuation coefficient and buildup factor of 99.99% pure paraffin wax (Carbon = 85.14%, Hydrogen = 14.86%). are calculated using 0.662, 0.835, 1.17 and 1.33 MeV gamma-rays. The mentioned gamma-rays were obtained from Cs-137, Mn-54 and Co-60 radioisotopes. Gamma rays obtained from these radioisotopes were passed through circular shaped wax slices and allowed to fall on a NaI detector. The thickness of wax slices were 0.33-2.9 cm with 6 cm diameter. Lead collimator of 1 cm diameter hole in the middle was used to obtain a collimated beam for narrow beam geometry. Broad beam geometry was used by removing the collimator to investigate buildup factor. Results show that Klein-Nishina electronic cross-section, Compton mass attenuation coefficient and Compton energy transfer coefficient all decrease with increasing photon energy. Linear attenuation coefficients mu = 0.0532 cm(-1) for 1.17 MeV beam and mu = 0.0419 cm(-1) for 1.33 MeV gamma-rays were obtained for wax. Variations in buildup factors are observed with increasing thickness of wax for 1.17 and 1.33 MeV beams.
机译:Klein-Nishina散射横截面,Compton散射,质量衰减和能量转移横截面,线性衰减系数和累积系数99.99%纯石蜡(碳= 85.14%,氢= 14.86%)。使用0.662,0.835,1.17和1.33 MeV伽马射线计算。所提述的γ射线是从CS-137,MN-54和CO-60放射性同位素获得的。从这些放射性同位素获得的γ射线通过圆形蜡切片,并使其落在Nai检测器上。蜡切片的厚度为0.33-2.9cm,直径为6厘米。中间中1cm直径孔的铅准直器用于获得用于窄梁几何的准直梁。通过去除准直器来调查积累因子来使用宽梁几何形状。结果表明,Klein-Nishina电子横截面,Compton质量衰减系数和康普顿能量传递系数随着光子能量的增加而降低。为1.17meV梁的线性衰减系数mu = 0.0532cm(-1),获得1.33mevγ射线的mu = 0.0419cm(-1)。随着蜡的厚度增加1.17和1.33MeV梁的厚度,观察到积聚因子的变化。

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