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1.中国原子能科学研究院 核数据重点实验室 北京 102413
2.中国科学院高能物理研究所 北京 100049
3.东莞中子科学中心 东莞 523803
[ "栾广源, 男, 1990年出生, 2017年于中国原子能科学研究院获硕士学位, 粒子物理与原子核物理专业, 从事中子探测器及其应用研究", "LUAN Guangyuan, male, born in 1990, graduated from China Institute of Atomic Energy with a master's degree in 2017, major in particle physics and nuclear physics, engaged in neutron detectors and applications" ]
鲍杰, E-mail:baojie@ciae.ac.cn BAO Jie, E-mail:baojie@ciae.ac.cn
收稿日期:2017-02-07,
修回日期:2017-03-19,
纸质出版日期:2017-11-10
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栾广源, 王琦, 鲍杰, 等. 用于CSNS反角白光中子能谱及注量率测量的快裂变室[J]. 核技术, 2017,40(11):110501
Guangyuan LUAN, Qi WANG, Jie BAO, et al. Physical design of fast fission chamber for neutron spectrum and flux measurement at the CSNS backstreaming white neutron source[J]. Nuclear techniques, 2017, 40(11): 110501
栾广源, 王琦, 鲍杰, 等. 用于CSNS反角白光中子能谱及注量率测量的快裂变室[J]. 核技术, 2017,40(11):110501 DOI: 10.11889/j.0253-3219.2017.hjs.40.110501.
Guangyuan LUAN, Qi WANG, Jie BAO, et al. Physical design of fast fission chamber for neutron spectrum and flux measurement at the CSNS backstreaming white neutron source[J]. Nuclear techniques, 2017, 40(11): 110501 DOI: 10.11889/j.0253-3219.2017.hjs.40.110501.
即将建成的中国散裂中子源(China Spallation Neutron Source,CSNS)反角白光中子束线可为核数据测量提供高注量率的脉冲白光中子束流,填补我国核数据测量用白光中子源的空白,提高我国核数据测量水平,满足核能、核技术及基础核物理研究对核数据的需求。该束线建成后,其中子能谱及注量率的精确测量将是开展其它物理实验的基础,快裂变电离室因其独特优点被选为中子能谱和注量率测量探测器。通过实验研究了快裂变电离室的粒子分辨性能、时间分辨性能;确定阴、阳极的合理间距为10 mm,据此测得电离室的时间分辨约15 ns;利用
235
U样品量计算的探测效率与利用伴随粒子法给出的探测效率在不确定度范围内符合,因此可以标定快裂变室的探测效率。通过这些工作,完成了满足反角白光中子束能谱及注量率测量需求的快裂变室的物理设计。
Background
2
The backstreaming white neutron source (Back-n) of China spallation neutron source (CSNS) will provide pulsed white neutron beam with a high fluence rate for nuclear data measurement. The accurate measurement of the neutron spectrum and fluence rate after the Back-n's completion will be the basis of the following physical experiments.
Purpose
2
This study aims to design a fast fission chamber for the CSNS Back-n flux measuring and monitoring system.
Methods
2
The detector performance including time resolution
particle distinction and detection efficiency was studied by experiments. Based on the study
the parameters of the fission chamber were determined
and its detection efficiency calculated by the
235
U sample quantity was compared with that measured by concomitant particle method.
Results
2
Considering the particle distinction
the distance between the anode and the target of the fission chamber was determined as 10 mm
the time resolution of the fission chamber was measured to be about 15 ns. The deviation of calculated detection efficiency from the measurement was in the range of 5%.
Conclusion
2
According to the detection efficiency and the demand of the neutron flux monitoring
the quantity of the uranium for the fast fission chamber can be determined. With appropriate parameters
the fast fission chamber can be used in CSNS Back-n flux measuring and monitoring.
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王 琦 , 鲍 杰 , 侯 龙 , . 裂变室在散裂中子源反角方向束流监视系统中的应用研究 . 核技术 , 2015 . 38 ( 10 ): 100403 DOI: 10.11889/j.0253-3219.2015.hjs.38.100403 http://doi.org/10.11889/j.0253-3219.2015.hjs.38.100403 http://www.j.sinap.ac.cn/hejishu/CN/abstract/abstract482.shtml .
Qi WANG , Jie BAO , Long HOU , . Study of fission ionization chamber in CSNS flux monitor system . Nuclear Techniques , 2015 . 38 ( 10 ): 100403 DOI: 10.11889/j.0253-3219.2015.hjs.38.100403 http://doi.org/10.11889/j.0253-3219.2015.hjs.38.100403 http://www.j.sinap.ac.cn/hejishu/CN/abstract/abstract482.shtml .
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