NUCLEAR TECHNIQUES, Volume. 48, Issue 5, 050401(2025)

Passive fast neutron multiplicity counting system based on liquid scintillation detectors

Yuezhuang LIU1, Shaodong ZHANG1,3, Yuanjiang YOU1, Xurun LIN1, Zhibo ZHOU2, Duohong LI2, Xingyu ZHOU1, Mengyuan LI1, Baoliang JIN1, Meng LI1, Lin MA1, Qi ZHANG1, Da LI2, Zhaohui WU2, and Xiaodong ZHANG4、*
Author Affiliations
  • 1School of Nuclear Science and Engineering, North China Electric Power University, Beijing 102206, China
  • 2State Nuclear Security Technology Center, Beijing 102401, China
  • 3China Nuclear Power Technology Research Institute Co., Ltd., Shenzhen 518031, China
  • 4Shenzhen Key Laboratory of Nuclear and Radiation Safety, Institute for Advanced Study in Nuclear Energy & Safety, College of Physics and Optoelectronic Engineering, Shenzhen University, Shenzhen 518060, China
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    Figures & Tables(16)
    Photographs of the FNMC system and its readout electronics
    Photograph of the self-developed 32-channel high-voltage power supply
    Screen-shot of the self-developed 32-channel high-voltage power supply control software
    Screen-shots of the user-friendly graphical interface of the FNMC system
    Neutron-gamma discrimination spectra of detector No.0 in the FNMC system
    Fitting results of the FNMC device using the Doubles parameter method
    Measurement results of the FNMC system with the fast neutron multiplicity analytical method (a) The estimated spontaneous fission rate, (b) The relative differences of the estimated spontaneous fission rate
    Photographs of different test scenarios(a) Layout of the test scenarios, (b) Source, (c) Source+ lead, (d) Source+ polyethylene
    Neutron multiplicity counting rates under different radiation backgrounds (color online) (a) Count rates of background, (b) Count rates of the test samples
    Measurement results of the spontaneous fission rate of a 252Cf neutron source using the fast neutron multiplicity analytical method under different radiation backgrounds (a) Estimated spontaneous fission rate, (b) Relative differences of the estimated spontaneous fission rate
    • Table 1. The spontaneous fission rate for the 252Cf neutron sources

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      Table 1. The spontaneous fission rate for the 252Cf neutron sources

      样品编号

      Sample number

      自发裂变率

      Spontaneous fission rate / fissionss-1

      1#732.77
      2#1 484.60
      3#2 185.32
      4#3 669.92
      5#4 402.68
      6#28 593.69
    • Table 2. Measured Doubles rate of 252Cf neutron sources with known spontaneous fission rate

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      Table 2. Measured Doubles rate of 252Cf neutron sources with known spontaneous fission rate

      样品编号

      Sample number

      Doubles计数率

      Doubles rate / s-1

      1#1.80±0.03
      2#3.53±0.04
      3#5.19±0.06
      4#8.70±0.09
      6#65.77±1.04
    • Table 3. The neutron multiplicity count rate of 252Cf neutron source measured by the FNMC device

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      Table 3. The neutron multiplicity count rate of 252Cf neutron source measured by the FNMC device

      样品编号

      Sample number / #

      总中子计数率

      Singles rate / s-1

      双重中子符合计数率

      Doubles rate / s-1

      三重中子符合计数率

      Triples rate / s-1

      160.90±0.151.80±0.030.03±0.003
      2123.24±0.263.53±0.040.05±0.005
      3179.36±0.355.19±0.060.07±0.007
      4299.44±0.538.70±0.090.14±0.01
      5355.13±0.6410.09±0.110.15±0.01
      62 278.36±6.1265.77±1.041.03±0.13
    • Table 4. Spontaneous fission rate of 252Cf neutron sources measured by the FNMC system with the fast neutron multiplicity analytical method

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      Table 4. Spontaneous fission rate of 252Cf neutron sources measured by the FNMC system with the fast neutron multiplicity analytical method

      样品编号

      Sample number / #

      自发裂变率

      Spontaneous fission rate / fissions∙s-1

      评估的自发裂变率

      Estimated spontaneous fission rate / fissions∙s-1

      相对偏差

      Relative difference / %

      1732.77759.45±10.913.64±1.49
      21 484.601 487.28±18.310.18±1.23
      32 185.322 184.62±23.92-0.03±1.09
      43 669.923 662.43±38.01-0.20±1.04
      54 402.684 247.42±45.29-3.53±1.03
      628 593.6927 696.99±437.98-3.14±1.53
    • Table 5. The neutron multiplicity count rate for different test scenarios

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      Table 5. The neutron multiplicity count rate for different test scenarios

      测试场景

      Test scenario

      本底计数率

      Count rate of background / s-1

      待测样品计数率

      Count rate of the test samples / s-1

      总中子计数率

      Singles rate / s-1

      双重中子计数率

      Doubles rate / s-1

      三重中子计数率

      Triples rate / s-1

      总中子计数率

      Singles rate / s-1

      双重中子计数率

      Doubles rate / s-1

      三重中子计数率

      Triples rate / s-1

      自然本底

      Natural background

      0.51±0.020.001±0.000 80.00±0.00122.49±0.273.43±0.040.07±0.01

      干扰源+聚乙烯

      Source+polyethylene

      47.27±0.290.16±0.020.00±0.00169.72±0.393.62±0.060.06±0.01

      干扰源+铅

      Source+lead

      73.97±0.280.20±0.010.00±0.00196.80±0.373.75±0.050.06±0.01
      干扰源 Source111.42±0.460.33±0.030.00±0.00233.53±0.473.87±0.060.05±0.01
    • Table 6. Spontaneous fission rate of 252Cf neutron sources measured for different test scenarios

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      Table 6. Spontaneous fission rate of 252Cf neutron sources measured for different test scenarios

      测试场景

      Test scenario

      评估的自发裂变率

      Estimated spontaneous fission rate / fissions∙s-1

      相对偏差

      Relative difference / %

      自然本底

      Natural background

      1 445.32±18.93-2.65±1.28

      干扰源+聚乙烯

      Source+polyethylene

      1 457.38±25.07-1.83±1.69

      干扰源+铅

      Source+lead

      1 496.13±22.170.78±1.49
      干扰源 Source1 488.49±27.740.26±1.87
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    Yuezhuang LIU, Shaodong ZHANG, Yuanjiang YOU, Xurun LIN, Zhibo ZHOU, Duohong LI, Xingyu ZHOU, Mengyuan LI, Baoliang JIN, Meng LI, Lin MA, Qi ZHANG, Da LI, Zhaohui WU, Xiaodong ZHANG. Passive fast neutron multiplicity counting system based on liquid scintillation detectors[J]. NUCLEAR TECHNIQUES, 2025, 48(5): 050401

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    Paper Information

    Category: NUCLEAR ELECTRONICS AND INSTRUMENTATION

    Received: Sep. 14, 2024

    Accepted: --

    Published Online: Jun. 26, 2025

    The Author Email: Xiaodong ZHANG (张小东)

    DOI:10.11889/j.0253-3219.2025.hjs.48.240364

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