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400~1500 MeV质子轰击铅靶和钨靶的出射中子能谱的FLUKA和Geant4模拟研究

宋林 陈志强 韩瑞 孙琪 田国玉 任培培

宋林, 陈志强, 韩瑞, 孙琪, 田国玉, 任培培. 400~1500 MeV质子轰击铅靶和钨靶的出射中子能谱的FLUKA和Geant4模拟研究[J]. 原子核物理评论, 2018, 35(1): 100-104. doi: 10.11804/NuclPhysRev.35.01.100
引用本文: 宋林, 陈志强, 韩瑞, 孙琪, 田国玉, 任培培. 400~1500 MeV质子轰击铅靶和钨靶的出射中子能谱的FLUKA和Geant4模拟研究[J]. 原子核物理评论, 2018, 35(1): 100-104. doi: 10.11804/NuclPhysRev.35.01.100
SONG Lin, CHEN Zhiqiang, HAN Rui, SUN Qi, TIAN Guoyu, REN Peipei. FLUKA and Geant4 Simulation of Spallation Neutrons from Lead and Tungsten Targets Bombarded with 400~1500 MeV Protons[J]. Nuclear Physics Review, 2018, 35(1): 100-104. doi: 10.11804/NuclPhysRev.35.01.100
Citation: SONG Lin, CHEN Zhiqiang, HAN Rui, SUN Qi, TIAN Guoyu, REN Peipei. FLUKA and Geant4 Simulation of Spallation Neutrons from Lead and Tungsten Targets Bombarded with 400~1500 MeV Protons[J]. Nuclear Physics Review, 2018, 35(1): 100-104. doi: 10.11804/NuclPhysRev.35.01.100

400~1500 MeV质子轰击铅靶和钨靶的出射中子能谱的FLUKA和Geant4模拟研究

doi: 10.11804/NuclPhysRev.35.01.100
基金项目: 国家自然科学基金资助项目(914263011,11605257);中国科学院战略性先导科技专项资助项目(XDA030300200)
详细信息
    作者简介:

    宋林(1991-),男,辽宁大连人,硕士研究生,从事中子学模拟研究;E-mail:songlin@impcas.ac.cn

    通讯作者: 陈志强,E-mail:zqchen@impcas.ac.cn。
  • 中图分类号: O571.55

FLUKA and Geant4 Simulation of Spallation Neutrons from Lead and Tungsten Targets Bombarded with 400~1500 MeV Protons

Funds: National Natural Science Foundation China(914263011, 11605257); Strategic Priority Research Program of Chinese Academy of Sciences(XDA030300200)
  • 摘要: 在ADS散裂靶系统的优化设计中,蒙特卡罗方法结合可靠的散裂反应理论模型进行中子学计算具有重要的作用。本工作利用Geant4程序中的INCLXX模型、BIC模型以及BERT模型和FLUKA程序分别模拟了597 MeV和1 500 MeV质子轰击薄铅靶不同出射角度的中子双微分截面,500,1 500 MeV质子轰击厚铅靶不同出射角度的中子双微分产额,以及400,600,800,1 000和1 200 MeV质子轰击厚钨靶在反角方向(175 °)的中子双微分产额,并与实验数据进行比较。研究表明,对于薄铅靶,Geant4程序的INCLXX模型和FLUKA程序模拟结果与实验符合得更好。能量在10~40 MeV范围内,BIC模型模拟结果明显高于实验数据,而BERT模型模拟结果略微低于实验数据。对于厚铅靶,在40 MeV左右所有的模拟结果都低于实验数据。对于厚钨靶,Geant4程序的BIC模型和FLUKA程序与实验数据符合得较好,INCLXX模型在能量高于60 MeV时模拟结果低于实验数据,BERT模型与实验数据差异较大。总体来看,Geant4程序的INCLXX模型和FLUKA程序进行ADS散裂靶相关的中子学的计算是合理和可靠的。


    The reliable Monte Carlo simulation codes coupled with nuclear reaction models play an important role in the neutronic calculation for the design and optimization of the ADS spallation target. In this work, the double differential cross sections at different angles produced from a thin lead target bombarded with 597 and 1 500 MeV protons, the neutron energy spectra at different angles produced from a thick lead target bombarded with 500 and 1 500 MeV protons, and the neutron energy spectra in the backward direction(175°) produced from a thick tungsten target bombarded with 400, 600, 800, 1 000 and 1 200 MeV protons are calculated with the Geant4 code coupled INCLXX, BIC and BERT models and the FLUKA code. The calculations are compared with the available experimental data. The results show that, for the thin lead target, the calculations with the Geant4 coupled INCLXX model and FLUKA code well reproduce the experimental results. In a energy range from 10 to 40 MeV, BIC model obviously overestimates the experimental results, and BERT model slightly underestimates the experimental results. For the thick lead target, all of the calculations underestimate the experimental results around 40MeV. For the thick tungsten target, the Geant4 coupled BIC model and FLUKA code well reproduce the experimental results. INCLXX model underestimates the experimental results above 60 MeV. BERT model bad reproduces the experimental results. Overall, the neutronic calculations with the Geant4 code coupled INCLXX model and FLUKA code for the ADS spallation target is reasonable and reliable.
  • [1] WANG Junsheng, ZHANG Ying, ZHANG Lixing, et al. Chinese Journal of Computational Physics, 2003, 20(5):408. (in Chinese) (万俊生, 张颖, 张利兴. 计算物理, 2003, 20(5):408.)
    [2] SATO T, NⅡTA K, MATSUDA N, et al. J Nucl Sci Technol, 2013, 50(9):913.
    [3] MCKINNEY G W. Physics and Algorithm Enhancements for a Validated MNCP/X Monte Carlo Simulation Tool, Phase VⅡ[C]. DNDO/NSF ARI Grantees Conference, Leesburg, Virginia, United States, 2012:1.
    [4] Geant4 Collaboration. Geant4 User's Guide for Application Developers, December, 2011.
    [5] BATTISTONI G, BOEHLEN T, CERUTTI F, et al. Ann Nucl Energy, 2015, 82:10.
    [6] ZHANG Suyalatu, LUO Fei, CHEN Zhiqiang, et al. Nuclear Physics Review, 2016, 33(3):370. (in Chinese) (张苏雅拉吐, 罗飞, 陈志强, 等. 原子核物理评论, 2016, 33(3):370.)
    [7] FAN Sheng, YU Hongwei, SHEN Qingbiao, et al. Nuclear Physics Review, 2002, 19(4):390. (in Chinese) (樊胜, 于洪伟, 申庆彪, 等. 原子核物理评论, 2002, 19(4):390.)
    [8] NIKHIL VITTAL SHETTY, Study of Particle Transport in a High Power Spallation Target for an Accelerator-Driven Transmutation System[O]. India:Aachen University, 2013:51.
    [9] YIN Chenyan, LI Zhiyuan,ZHOU Chao, et al. Journal of Unicersity of South China:Science and Technology, 2010, 24(2):1. (in Chinese) (尹陈艳, 李志远, 周超, 等. 南华大学学报:自然科学版, 2010, 24(2):1.)
    [10] LEE S C, BUNGAU C, CYWINSKI R, et al. Geant4 Simulations of Proton-Induced Spallation for Applications in ADSR Systems[C]. Proceedings of IPAC2016, Busan, Korea, 2016:1943.
    [11] HEILBRONN L, NAKAMURA T, IWATA, et al. Overview of Secondary Neutron Production Relevant to Shielding in Space, 2005, 116(1-4):140.
    [12] AMIAN W B, BYRD R C, CLARKET D A, et al. Nuclear Science and Engineering, 1993, 115(1):1.
    [13] TSTSUSHI NALAMOTO, KENJI ISHIBASHI, NARUHIRO MATSUFUHI, et al. Journal of Nuclear Science and Techology, 1995, 32(9):827.
    [14] KENJI ISHIBASHI, HIROSHI TAKADA, TATSUSHI NAKAMOTO, et al. Journal of Nuclear Science and Techology, 1997, 34(6):529.
    [15] MEIGO S, TAKADA H, CHIBA S, et al. Nucl Instr Meth A, 1999, 432:521.
    [16] TANG Jingyu, JING Hantao, XIA Haihong, et al. Atomic Energy Science and Technology, 2013, 47(7):1089. (in Chinese) (唐靖宇, 敬罕涛, 夏海鸿, 等. 原子能科学技术, 2013, 47(7):1089.)
    [17] BELYKOV-BODIN V I, KATINOV Y V, NOZDTACHEV V N, et al. Nucl Instr Meth A, 2008, 596:434.
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出版历程
  • 收稿日期:  2017-10-11
  • 修回日期:  2017-12-11
  • 刊出日期:  2018-03-20

400~1500 MeV质子轰击铅靶和钨靶的出射中子能谱的FLUKA和Geant4模拟研究

doi: 10.11804/NuclPhysRev.35.01.100
    基金项目:  国家自然科学基金资助项目(914263011,11605257);中国科学院战略性先导科技专项资助项目(XDA030300200)
    作者简介:

    宋林(1991-),男,辽宁大连人,硕士研究生,从事中子学模拟研究;E-mail:songlin@impcas.ac.cn

    通讯作者: 陈志强,E-mail:zqchen@impcas.ac.cn。
  • 中图分类号: O571.55

摘要: 在ADS散裂靶系统的优化设计中,蒙特卡罗方法结合可靠的散裂反应理论模型进行中子学计算具有重要的作用。本工作利用Geant4程序中的INCLXX模型、BIC模型以及BERT模型和FLUKA程序分别模拟了597 MeV和1 500 MeV质子轰击薄铅靶不同出射角度的中子双微分截面,500,1 500 MeV质子轰击厚铅靶不同出射角度的中子双微分产额,以及400,600,800,1 000和1 200 MeV质子轰击厚钨靶在反角方向(175 °)的中子双微分产额,并与实验数据进行比较。研究表明,对于薄铅靶,Geant4程序的INCLXX模型和FLUKA程序模拟结果与实验符合得更好。能量在10~40 MeV范围内,BIC模型模拟结果明显高于实验数据,而BERT模型模拟结果略微低于实验数据。对于厚铅靶,在40 MeV左右所有的模拟结果都低于实验数据。对于厚钨靶,Geant4程序的BIC模型和FLUKA程序与实验数据符合得较好,INCLXX模型在能量高于60 MeV时模拟结果低于实验数据,BERT模型与实验数据差异较大。总体来看,Geant4程序的INCLXX模型和FLUKA程序进行ADS散裂靶相关的中子学的计算是合理和可靠的。


The reliable Monte Carlo simulation codes coupled with nuclear reaction models play an important role in the neutronic calculation for the design and optimization of the ADS spallation target. In this work, the double differential cross sections at different angles produced from a thin lead target bombarded with 597 and 1 500 MeV protons, the neutron energy spectra at different angles produced from a thick lead target bombarded with 500 and 1 500 MeV protons, and the neutron energy spectra in the backward direction(175°) produced from a thick tungsten target bombarded with 400, 600, 800, 1 000 and 1 200 MeV protons are calculated with the Geant4 code coupled INCLXX, BIC and BERT models and the FLUKA code. The calculations are compared with the available experimental data. The results show that, for the thin lead target, the calculations with the Geant4 coupled INCLXX model and FLUKA code well reproduce the experimental results. In a energy range from 10 to 40 MeV, BIC model obviously overestimates the experimental results, and BERT model slightly underestimates the experimental results. For the thick lead target, all of the calculations underestimate the experimental results around 40MeV. For the thick tungsten target, the Geant4 coupled BIC model and FLUKA code well reproduce the experimental results. INCLXX model underestimates the experimental results above 60 MeV. BERT model bad reproduces the experimental results. Overall, the neutronic calculations with the Geant4 code coupled INCLXX model and FLUKA code for the ADS spallation target is reasonable and reliable.

English Abstract

宋林, 陈志强, 韩瑞, 孙琪, 田国玉, 任培培. 400~1500 MeV质子轰击铅靶和钨靶的出射中子能谱的FLUKA和Geant4模拟研究[J]. 原子核物理评论, 2018, 35(1): 100-104. doi: 10.11804/NuclPhysRev.35.01.100
引用本文: 宋林, 陈志强, 韩瑞, 孙琪, 田国玉, 任培培. 400~1500 MeV质子轰击铅靶和钨靶的出射中子能谱的FLUKA和Geant4模拟研究[J]. 原子核物理评论, 2018, 35(1): 100-104. doi: 10.11804/NuclPhysRev.35.01.100
SONG Lin, CHEN Zhiqiang, HAN Rui, SUN Qi, TIAN Guoyu, REN Peipei. FLUKA and Geant4 Simulation of Spallation Neutrons from Lead and Tungsten Targets Bombarded with 400~1500 MeV Protons[J]. Nuclear Physics Review, 2018, 35(1): 100-104. doi: 10.11804/NuclPhysRev.35.01.100
Citation: SONG Lin, CHEN Zhiqiang, HAN Rui, SUN Qi, TIAN Guoyu, REN Peipei. FLUKA and Geant4 Simulation of Spallation Neutrons from Lead and Tungsten Targets Bombarded with 400~1500 MeV Protons[J]. Nuclear Physics Review, 2018, 35(1): 100-104. doi: 10.11804/NuclPhysRev.35.01.100
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