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首页> 外文期刊>Applied radiation and isotopes: including data, instrumentation and methods for use in agriculture, industry and medicine >Experimental response function of a 3 in x 3 in NaI(Tl) detector by inverse matrix method and effective atomic number of composite materials by gamma backscattering technique
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Experimental response function of a 3 in x 3 in NaI(Tl) detector by inverse matrix method and effective atomic number of composite materials by gamma backscattering technique

机译:逆矩阵法在NaI(Tl)探测器中3 in x 3的实验响应函数和伽马反向散射技术对复合材料的有效原子序数

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Response function of a widely used 3 in x 3 in NaI(Tl) detector is constructed to correct the observed pulse height distribution. A 10 x 10 inverse matrix is constructed using 7 mono-energetic gamma sources (Co-57, Hg-203, Ba-133, Na-22, Cs-137, Mn-54 and Zn-65) which are evenly spaced in energy scale to unscramble the observed pulse height distribution. Bin widths (E)(1/2) of 0.01 (MeV)(1/2) are used to construct the matrix. Backscattered photons for an angle of 110 degrees are obtained from a well-collimated 0.2146 GBq (5.8 mCi) Cs-137 gamma source for carbon, aluminium, iron, copper, granite and Portland cement. For each observed spectrum, single scattered spectrum is constructed analytically using detector parameters like FWHM, photo-peak efficiency and peak counts. Response corrected multiple scattered photons are extracted from the observed pulse height distribution by dividing the spectrum into a 10 x 1 matrix. Saturation thicknesses of carbon, aluminium, iron, copper, granite and Portland cement are found out. Variation of multiple scattered photons as a function of target thickness are simulated using MCNP code. A relationship between experimental and simulated saturation thicknesses of carbon, aluminium, iron and copper is obtained as a function of atomic number. Using this relation, effective atomic numbers of granite and Portland cement are obtained from interpolation method. Effective atomic numbers of granite and Portland cement are also obtained by theoretical equation using their elemental composition and comparing with the experimental and simulated results. (C) 2016 Elsevier Ltd. All rights reserved.
机译:构建NaI(Tl)检测器中广泛使用的3 in x 3的响应函数,以校正观察到的脉冲高度分布。使用7个能量均匀分布的7个单能伽马源(Co-57,Hg-203,Ba-133,Na-22,Cs-137,Mn-54和Zn-65)构建10 x 10逆矩阵缩放以解扰观察到的脉冲高度分布。 0.01(MeV)(1/2)的面元宽度(E)(1/2)用于构建矩阵。从高度准直的0.2146 GBq(5.8 mCi)Cs-137γ源获得了110度角的反向散射光子,用于碳,铝,铁,铜,花岗岩和硅酸盐水泥。对于每个观察到的光谱,使用诸如FWHM,光峰效率和峰值计数之类的检测器参数来解析地构建单个散射光谱。通过将光谱分成10 x 1矩阵,从观察到的脉冲高度分布中提取经过响应校正的多个散射光子。发现了碳,铝,铁,铜,花岗岩和波特兰水泥的饱和厚度。使用MCNP代码模拟了多个散射光子随目标厚度的变化。获得了碳,铝,铁和铜的实验饱和厚度与模拟饱和厚度之间的关系,该关系是原子序数的函数。利用这种关系,可以通过插值法获得花岗岩和硅酸盐水泥的有效原子序数。花岗岩和硅酸盐水泥的有效原子序数也可以通过理论方程,利用其元素组成并与实验和模拟结果进行比较来获得。 (C)2016 Elsevier Ltd.保留所有权利。

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