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作 者:冯天成[1,2] 贾明雁[2] 程建平[1] 冯元举[2]
机构地区:[1]清华大学工程物理系,北京100084 [2]西北核技术研究所,西安710024
出 处:《核电子学与探测技术》2010年第11期1434-1441,共8页Nuclear Electronics & Detection Technology
摘 要:通过理论推导和数值计算,对"多能峰模式"、"峰谷比模式"和"准直器模式"三种就地γ谱仪核素深度分布测量模式灵敏度进行研究。"多能峰模式"采用152Eu 244、1 408 keVγ射线,"峰谷比模式"采用137Cs 662 keVγ射线,"准直器模式"采用137Cs 662 keVγ射线和就地计数系统(ISOCS)30°、90°~180°准直器。研究表明,总体上灵敏度大小依次为"峰谷比模式"〉"多能峰模式"〉〉"准直器模式"。The main limitation of in-situ γ spectrometry lies in determining the depth-distribution of the artificial radionuclide in soil.So,many researchers have developed methods and models aimed at deducing the depth-distribution information from in-situ spectrum itself.Until now,there are three main methods studied and established,which includes "Multiple photopeak method","Peak-to-valley ratio method" and "Collimated or lead plate method".This paper presented the theoretical study on the method-sensitivity comparison.The experimental methods for Multiple photopeak,Peak-to-valley ratio and Collimated or lead plate are at the energy of 244 keV and 1 408 keV γ-rays of 152Eu,662 keV γ-ray of 137Cs,662 keV γ-ray of 137Cs,respectively,and the ISOCS was employed in Collimated or lead plate method.Results indicated that the sequence of method-sensitivity from the maximum to the minimum was as following: Peak-to-valley method,Multiple photopeak method,and Collimated or lead plate method,and the sensitivity of Collimated or lead plate method was far less than Multiple photopeak method.
关 键 词:就地Γ谱仪 多能峰模式 峰谷比模式 准直器模式 模式灵敏度
分 类 号:TL7[核科学技术—辐射防护及环境保护]
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