蒙特卡罗法模拟P型同轴高纯锗探测器结构对探测效率影响

Simulation of Structural Effects on Detection Efficiency in P-Type Coaxial High-Purity Germanium Detectors Using the Monte Carlo Method

  • 摘要: 为确定高纯锗探测器的全能峰效率(FEPE),进行放射性核素定量分析,本研究针对实际测量的高纯锗晶体尺寸构建探测器MC模型;通过实验和模拟结合的方法优化MC模型死层厚度,使得模拟与实际探测效率的平均相对偏差为1.74%;模拟分析高纯锗晶体结构和铜电极棒尺寸变化对全能峰效率(FEPE)的影响。结果表明,低能伽玛射线对晶体顶端结构变化较为敏感,晶体顶部圆角化边缘对59.5 keV射线效率影响相对偏差最大为19.21%;底部保护环的存在对高能射线探测效率的影响随入射能量和源距增加而变大,而对低能射线的影响可以忽略不计;由于铜电极棒对射线造成阻挡,其直径的变化导致高能射线探测效率最高下降1.78%。本研究结果可为优化探测器结构设计和提升FEPE校准精度提供参考依据。

     

    Abstract: Determining the full-energy peak efficiency (FEPE) of a high-purity germanium (HPGe) detector through experimental methods or Monte Carlo (MC) simulations is crucial for accurate radionuclide quantification. This study presents a meticulously constructed MC model tailored to the actual dimensions of the measured HPGe crystal. Optimization of the dead layer thickness within the model was achieved through an integrated approach of experimental validation and simulation efforts, yielding a minimal average relative deviation of 1.74% between simulated and actual detection efficiencies. Subsequent simulations were conducted to assess the impact of structural modifications in the HPGe crystal and variations in the diameter of copper electrode rods on FEPE. The findings indicate that low-energy gamma rays exhibit increased sensitivity to modifications at the crystal’s top, with the rounded edges displaying a substantial relative deviation in detection efficiency of up to 19.21% at 59.5 keV. Additionally, the presence of a protective ring at the crystal’s base significantly enhances the detection efficiency for high-energy rays as incident energy and source distance increase, while its impact on low-energy rays remains minimal. Changes in the diameter of the copper electrode rods, which act as ray-blocking devices, were found to decrease the detection efficiency of high-energy rays by as much as 1.78%. These insights are pivotal for refining detector design and advancing the calibration precision of FEPE in scientific applications.

     

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