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Calibration of 4π NaI(Tl) detectors with coincidence summing correction using new numerical procedure and ANGLE4 software

机译:使用新的数值程序和ANGLE4软件通过重合和校正校正4πNaI(Tl)检测器

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摘要

The 4π NaI(Tl) γ-ray detectors are consisted of the well cavity with cylindrical cross section, and the enclosing geometry of measurements with large detection angle. This leads to exceptionally high efficiency level and a significant coincidence summing effect, much more than a single cylindrical or coaxial detector especially in very low activity measurements. In the present work, the detection effective solid angle in addition to both full-energy peak and total efficiencies of well-type detectors, were mainly calculated by the new numerical simulation method (NSM) and ANGLE4 software. To obtain the coincidence summing correction factors through the previously mentioned methods, the simulation of the coincident emission of photons was modeled mathematically, based on the analytical equations and complex integrations over the radioactive volumetric sources including the self-attenuation factor. The measured full-energy peak efficiencies and correction factors were done by using 152Eu, where an exact adjustment is required for the detector efficiency curve, because neglecting the coincidence summing effect can make the results inconsistent with the whole. These phenomena, in general due to the efficiency calibration process and the coincidence summing corrections, appear jointly. The full-energy peak and the total efficiencies from the two methods typically agree with discrepancy 10%. The discrepancy between the simulation, ANGLE4 and measured full-energy peak after corrections for the coincidence summing effect was on the average, while not exceeding 14%. Therefore, this technique can be easily applied in establishing the efficiency calibration curves of well-type detectors.
机译:4πNaI(Tl)γ射线探测器由具有圆柱形横截面的井腔和具有大探测角的封闭测量几何组成。这导致异常高的效率水平和显着的重合求和效果,比单个圆柱形或同轴检测器要高得多,尤其是在非常低的活动性测量中。在目前的工作中,主要通过新的数值模拟方法(NSM)和ANGLE4软件来计算除阱型探测器的全能峰值和总效率以外的探测有效立体角。为了通过前述方法获得同时求和的校正因子,基于解析方程和包括自衰减因子在内的放射性体积源的复杂积分,对光子同时发射的模拟进行数学建模。使用 152 Eu完成了测得的全能峰值效率和校正因子,其中需要对检测器效率曲线进行精确调整,因为忽略重合和效应可能会使结果与整体不一致。通常,由于效率校准过程和同时求和校正,这些现象共同出现。两种方法的全能量峰值和总效率通常相差10%。校正巧合和效应后,模拟,ANGLE4与测得的全能峰之间的差异为平均水平,但不超过14%。因此,该技术可以容易地应用于建立井型检测器的效率校准曲线。

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