首页|BNCT治疗束γ能谱仪的校准方法研究

BNCT治疗束γ能谱仪的校准方法研究

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受硼中子俘获疗法(BNCT)治疗束的特点所限,源项γ射线能谱的测量难度较大,国际上开展的相关工作很少,且未对其谱仪进行校准。为得到准确的源项γ能谱,本文主要开展了适用于BNCT治疗束7能谱仪的校准方法研究。谱仪由高纯锗(HPGe)探测器及屏蔽系统组成,因为屏蔽效果很好,无法通过实验方法校准整个谱仪系统的γ响应。由于其主要影响因素是HPGe探测器的死层分布,谱仪可通过下述方法进行校准:对裸探测器进行校准,获取探测器的准确模型;利用精细测量及材料分析得到屏蔽体的精确模型,建立谱仪的计算模型;通过MCNP计算获得谱仪的响应函数。由此将结果溯源至相应的国家或国防标准,确保谱仪关键参数的准确可靠,为后续解谱工作奠定基础。
Study on Calibration Method of γ Spectrometer for BNCT Treatment
Limited by the characteristics of the boron neutron capture therapy(BNCT)treatment beam,it is difficult to measure the γ ray energy spectrum of the source term.There are few relevant work has been carried out.Up to now,only the γ energy spec-trometer directly measured the source term γ rays,but the spectrometer was not been calibrated and unfold.In order to obtain an accurate γ energy spectrum of the source term,it is necessary to calibrate the γ energy spectrometer and establish the reliable response function of the system.This paper briefly introduces the γ energy spectrometer designed for BNCT treatment beam,and mainly introduces the calibration method suit-able for this spectrometer.The spectrometer consists of a high purity germanium(HPGe)detector and a shield system.Since the entire spectrometer is designed for high intensity neutron/γ mixed fields,the shield effect of the spectrometer is so effective,and it is impossible to calibrate the γ response of the entire spectrometer system through experimental methods.By analyzing the spectrometer system,the dead layer distribu-tion of the HPGe detector is the main influence factor,and other structures can be accurately obtained through X-ray radiography and geometric measurements.There-fore,the calibration method of the spectrometer is as follows:obtain an accurate model of the HPGe detector by X-ray radiography and calibration;use precision measure-ments,fine geometric measurement and material analysis to obtain an accurate model of the shield,and establish a calculation model of the spectrometer;acquire the response function of the spectrometer system through Monte Carlo N particle transport code(MCNP)calculation,and the energy spans from 0.1 MeV to 11 MeV with an energy interval of 10 keV.Among them,the HPGe detector dead layer distribution can be confirmed using the following steps.The efficiency of the HPGe detector was calibrated utilizing standard γ sources and high-energy γ reference radiation fields.The dead layer distribution of the HPGe detector was adjusted using MCNP to ensure agreement between calculated and measured efficiencies,thereby determining the geometric distri-bution of the dead layer.Therefore,using a combination of Monte Carlo simulation and experimental methods,the results can be traced to the corresponding national or nation-al defense standards,ensuring the accuracy and reliability of the key parameters of the spectrometer,and laying the foundation for subsequent spectrum unfold work.

γ energy spectrometerresponse functionHPGe detectorMCNP

张书峰、石斌、肖鸿飞、陈军、刘蕴韬、张庆贤、宋明哲

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中国原子能科学研究院,北京 102413

成都理工大学,四川成都 610059

γ能谱仪 响应函数 HPGe探测器 MCNP

2024

原子能科学技术
中国原子能科学研究院

原子能科学技术

CSTPCD北大核心
影响因子:0.372
ISSN:1000-6931
年,卷(期):2024.58(4)
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