Acta Physica Sinica, Volume. 69, Issue 11, 112801-1(2020)

Monte Carlo simulation technology based on characteristic γ-ray spectrum analysis

Li Deng1,2, Rui Li2、*, Xin Wang2, and Yuan-Guang Fu2
Author Affiliations
  • 1Institute of Applied Physics and Computational Mathematics (IAPCM), Beijing 100094, China
  • 2CAEP Software Centre for High Performance Numerical Simulation (CAEP-SCNS), Beijing 100088, China
  • show less
    Figures & Tables(8)
    The timing diagram of neutron induced inelastic γ and capture γ in C/O well-logging.
    Sketch of luggage model.
    Comparison of calculated result about energy spectra of secondary γ: (a) JMCT primary line γ; (b) JMCT Compton γ; (c) JMCT total γ; (d) MCNP total γ.
    Comparison of secondary γ-fluent tine spectrum between JMCT and MCNP.
    • Table 1. Energy of spectrum line from inelastic γ and capture γ about H, C, N, O, etc.

      View table
      View in Article

      Table 1. Energy of spectrum line from inelastic γ and capture γ about H, C, N, O, etc.

      元素反应类型特征γ 谱线能量/MeV
      H辐射俘获2.2233
      C非弹性散射4.433
      N辐射俘获非弹性散射1.8848, 5.2692, 5.5534, 6.3224, 7.2991, 10.8290, 2.3128, 4.4444, 5.1059, 7.0280
      O非弹性散射2.7419, 3.6841, 6.1310, 6.9170, 7.1190
      F非弹性散射0.1090, 0.1971, 1.2358, 1.3480, 1.3565
      P辐射俘获非弹性散射2.1542, 3.5228, 3.9003, 4.6713, 6.7853, 1.2661, 2.2334
      S辐射俘获0.8411, 2.3797, 2.9311, 3.2208, 4.4308, 4.8698, 5.4205,
      Cl辐射俘获0.5167, 0.7884, 1.1647, 1.9509, 1.9591, 2.8639, 5.7153, 6.1109, 6.6195, 7.4138
      As辐射俘获非弹性散射6.2941, 6.8094, 7.0192, 0.2646, 0.2795, 0.5725
      Al辐射俘获非弹性散射0.9840, 2.9598, 4.1329, 4.2522, 7.7239, 0.8438, 1.0144, 2.2118
      Fe辐射俘获非弹性散射0.3522, 1.7251, 5.9203, 6.0185, 7.6311, 7.6455, 8.8860, 9.2980, 0.8468, 1.2383, 1.4082, 1.8105, 2.1129, 2.5985
    • Table 2. Weight percentage of elements in some spirited detonators (TNT) and chemical weapons.

      View table
      View in Article

      Table 2. Weight percentage of elements in some spirited detonators (TNT) and chemical weapons.

      元素TNT沙林/GB神经性 毒气/VX 芥子气/HD孁烂性 毒气/L
      氢(H)2.27.19.75.01.0
      碳(C)37.034.349.430.211.4
      氮(N)18.55.2
      氧(O)42.322.912.0
      氟(F)13.6
      磷(P)22.111.6
      硫(S)12.020.1
      氯(Cl)44.751.3
      砷(As)36.1
    • Table 3. Comparison of calculated results about secondary γ between JMCT and MCNP.

      View table
      View in Article

      Table 3. Comparison of calculated results about secondary γ between JMCT and MCNP.

      程序原级线 光子 原级连续 光子 散射光子Jγ光子流 偏差/%
      注: 偏差 = [Jγ(JMCT) – Jγ(MCNP)]/ Jγ(MCNP).
      JMCT4.92519-704.34947-85.36014-70.4406
      MCNP5.38386-7标准解
    • Table 4. Count and percentage of prompt γ from H, C, N and O.

      View table
      View in Article

      Table 4. Count and percentage of prompt γ from H, C, N and O.

      元素计数份额比/%统计误差/%
      注: 偏差 = [Jγ(JMCT) – Jγ(MCNP)]/ Jγ(MCNP).
      H3.02643 × 10–1100.56
      C1.77077 × 10–7360.49
      N1.11146 × 10–7230.12
      O2.03254 × 10–7410.18
    Tools

    Get Citation

    Copy Citation Text

    Li Deng, Rui Li, Xin Wang, Yuan-Guang Fu. Monte Carlo simulation technology based on characteristic γ-ray spectrum analysis[J]. Acta Physica Sinica, 2020, 69(11): 112801-1

    Download Citation

    EndNote(RIS)BibTexPlain Text
    Save article for my favorites
    Paper Information

    Category: Research Articles

    Received: Feb. 24, 2020

    Accepted: --

    Published Online: Dec. 2, 2020

    The Author Email:

    DOI:10.7498/aps.69.20200279

    Topics