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Volume 36 Issue 2
Jul.  2019
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SUN Shiqi, HU Liyuan, HOU Yingwei, LIU Huilan, SONG Yushou. Simulation of Uranium Mass Measurement Based on Active Neutron Multiplicity[J]. Nuclear Physics Review, 2019, 36(2): 266-271. doi: 10.11804/NuclPhysRev.36.02.266
Citation: SUN Shiqi, HU Liyuan, HOU Yingwei, LIU Huilan, SONG Yushou. Simulation of Uranium Mass Measurement Based on Active Neutron Multiplicity[J]. Nuclear Physics Review, 2019, 36(2): 266-271. doi: 10.11804/NuclPhysRev.36.02.266

Simulation of Uranium Mass Measurement Based on Active Neutron Multiplicity

doi: 10.11804/NuclPhysRev.36.02.266
Funds:  Special Fund for Basic Scientific Research Business Fees of Central Universities (HEUCFP201851)
  • Received Date: 2018-09-12
  • Rev Recd Date: 2019-03-06
  • Publish Date: 2019-06-20
  • Neutron multiplicity technique is commonly used to measure and verify nuclear materials, especially for objects with heavy shields. Plutonium material has high spontaneous fission rate and passive measurement is available. Currently, there are many different measurement devices. However, uranium material measurement can only be performed by active method due to its low spontaneous fission rate. The existing active well type coincidence counter (AWCC) is capable of performing active neutron multiplicity measurement of uranium. But the detection efficiency is low and there are lots of accidental coincidence counts caused by the Am-Li neutron source. In order to improve the efficiency and the accuracy it is necessary to carry out comprehensive investigation on active neutron multiplicity measurement method. A neutron multiplicity measurement system was modeled based on Geant4 referring to the AWCC structure. The effects of different gate width and delay time on the measurement deviation were studied. The optimal gate width of the counter is 44 μs and the range of the gate width is suitable for about 1.5 times of the counter die-away time; after the delay time is greater than 3 times the counter die-away time, the relative deviation is significantly reduced. The influence of 235U enrichment on the result was also discussed. This work provides a reference for the design of the active neutron multiplicity counter.
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    [2] WANG Xiaozhong, JIA Xiangjun. Atomic Energy Science and Technology, 1998, 32(3):256. (in Chinese) (王效忠, 贾向军. 原子能科学技术, 1998, 32(3):256.)
    [3] ZHAO Deshan, CHEN Qi, CHEN Xianglin. Nuclear Electronics and Detection Technology, 2004, 24(6):726. (in Chinese) (赵德山, 陈琦, 陈想林. 核电子学与探测技术, 2004, 24(6):726.)
    [4] SPRINKLE J. Passive Nondestructive Assay of Nuclear Materials, NUREG/CR-5550, United States Nuclear Regulatory Commission, 1991:435.
    [5] KRICK M S, MENLOVE H O. High-level neutron coincidence counter (HLNCC):Users' Manual[R]. Los Alamos Scientific Lab, 1979.
    [6] ENSSLIN N, HARKER W C, KRICK M S, et al. Los Alamos Report LA-13422-M, 1998.
    [7] PEERANI P, FERRER M M. Nucl Instr and Meth A, 2008, 589(2):304.
    [8] GÖTTSCHE M, KIRCHNER G. Nucl Instr and Meth A, 2015, 798:99.
    [9] GODDARD B, CROFT S, LOUSTEAU A, et al. Nucl Instr and Meth A, 2016, 830:256.
    [10] CHEN Ligao, LIU Xiaobo, GONG Jian, et al. Journal of Tsinghua University:Science and Technology, 2015, 54(2):159. (in Chinese) (陈利高, 刘晓波, 龚建, 等. 清华大学学报:自然科学版, 2015, 54(2):159.)
    [11] LI Sufen, ZHANG Quanhu, DI Yuming, et al. Computer Simulation of Active Neutron Multiplicity Measurement[C]//The 16th National Conference on Nuclear Electronics and Nuclear Detection Technology, Mianyang, 2012. (in Chinese) (黎素芬, 张全虎, 弟宇鸣, 等. 有源中子多重性测量计算机模拟研究[C]//第十六届全国核电子学与核探测技术学术年会, 绵阳, 2012.)
    [12] ZHU Jianyu, XU Xuefeng, JIANG Yimin, et al. Nuclear Physics Review, 2015, 32(3):323. (in Chinese) (朱剑钰, 徐雪峰, 蒋翊民, 等. 原子核物理评论, 2015, 32(3):323.)
    [13] ENSSLIN N, KRICK M S, LANGNER D G, et al. Active Neutron Multiplicity Counting of Bulk Uranium[R]. Los Alamos National Lab, NM (United States), 1991.
    [14] KRICK M S, ENSSLIN N, CEO R N, et al. Analysis of Active Neutron Multiplicity Data for Y-12 Skull Oxide Samples[R]. Los Alamos National Lab, 1996.
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Simulation of Uranium Mass Measurement Based on Active Neutron Multiplicity

doi: 10.11804/NuclPhysRev.36.02.266
Funds:  Special Fund for Basic Scientific Research Business Fees of Central Universities (HEUCFP201851)

Abstract: Neutron multiplicity technique is commonly used to measure and verify nuclear materials, especially for objects with heavy shields. Plutonium material has high spontaneous fission rate and passive measurement is available. Currently, there are many different measurement devices. However, uranium material measurement can only be performed by active method due to its low spontaneous fission rate. The existing active well type coincidence counter (AWCC) is capable of performing active neutron multiplicity measurement of uranium. But the detection efficiency is low and there are lots of accidental coincidence counts caused by the Am-Li neutron source. In order to improve the efficiency and the accuracy it is necessary to carry out comprehensive investigation on active neutron multiplicity measurement method. A neutron multiplicity measurement system was modeled based on Geant4 referring to the AWCC structure. The effects of different gate width and delay time on the measurement deviation were studied. The optimal gate width of the counter is 44 μs and the range of the gate width is suitable for about 1.5 times of the counter die-away time; after the delay time is greater than 3 times the counter die-away time, the relative deviation is significantly reduced. The influence of 235U enrichment on the result was also discussed. This work provides a reference for the design of the active neutron multiplicity counter.

SUN Shiqi, HU Liyuan, HOU Yingwei, LIU Huilan, SONG Yushou. Simulation of Uranium Mass Measurement Based on Active Neutron Multiplicity[J]. Nuclear Physics Review, 2019, 36(2): 266-271. doi: 10.11804/NuclPhysRev.36.02.266
Citation: SUN Shiqi, HU Liyuan, HOU Yingwei, LIU Huilan, SONG Yushou. Simulation of Uranium Mass Measurement Based on Active Neutron Multiplicity[J]. Nuclear Physics Review, 2019, 36(2): 266-271. doi: 10.11804/NuclPhysRev.36.02.266
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