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中国工程物理研究院 核物理与化学研究所,绵阳,621900
[ "通讯作者: 王立宗 E-mail:wanglz_caep@163.com" ]
纸质出版日期:2014-11-07
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王立宗, 朱学彬, 杨建伦, 等. 235U裂变碎片在PIN探测器中沉积能量的实验研究[J]. 核技术, 2014,37(11):110403
WANG Lizong, ZHU Xuebin, YANG Jianlun, et al. Experimental research of 235U fission fragment deposit energy in PIN detector[J]. Nuclear techniques, 2014, 37(11): 110403
王立宗, 朱学彬, 杨建伦, 等. 235U裂变碎片在PIN探测器中沉积能量的实验研究[J]. 核技术, 2014,37(11):110403 DOI: 10.11889/j.0253-3219.2014.hjs.37.110403.
WANG Lizong, ZHU Xuebin, YANG Jianlun, et al. Experimental research of 235U fission fragment deposit energy in PIN detector[J]. Nuclear techniques, 2014, 37(11): 110403 DOI: 10.11889/j.0253-3219.2014.hjs.37.110403.
利用中子与235U发生裂变反应的截面在裂变中子能区基本不变这一特点,可设计研制裂变靶室探测系统,该系统中子能量响应较平坦,在脉冲中子总数测量中有广阔的应用前景。利用K-400加速器稳态DT中子源,实验标定了235U裂变碎片在PIN探测器中的平均沉积能量,并与理论计算结果进行了比较。裂变靶室系统探测效率可通过数值计算准确给出,与平均沉积能量实验测量值相结合,可得到准确的中子灵敏度数据,进而获得裂变靶室探测系统中子能量响应曲线。
Background: Because 235U fission cross-section with neutrons remains almost constant in the fission neutron energy region
the neutron-induced fission fragments detection system with flat neutron energy response will be widely used in pulsed fission neutron yield measurement. Purpose: The neutron-induced fission target chamber detection system consisting of 235U target and PIN detector is designed and investigated experimentally. Methods: The fission fragment energy spectrum and average energy deposited in the PIN detector are calculated by Monte Carlo simulation coupling with TRIM2000. Average deposit energy of 235U fission fragment in PIN detector is measured by recording fragment energy spectrum at K-400 accelerator neutron source. Results: The experimental results are compared with theoretical calculation. The calculated average deposited energy is in fact over-estimated because of pulse height defect of fission fragments in PIN detector. With the calculated neutron detecting efficiency and the calibrated average effective deposited energy available
the neutron sensitivity can be determined
and neutron energy response curve of fission target chamber detection system can be obtained. Conclusion: The present results can furnish theoretical and experimental indication for design of fission target chamber detection system. Abstract
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