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张鑫, 陈志强, 刘丙岩, 韩瑞, 田国玉, 石福栋, 孙慧. 利用GEANT4研究轻带电粒子诱发反应出射中子双微分产额[J]. 原子核物理评论, 2020, 37(3): 617-620. DOI: 10.11804/NuclPhysRev.37.2019CNPC48
引用本文: 张鑫, 陈志强, 刘丙岩, 韩瑞, 田国玉, 石福栋, 孙慧. 利用GEANT4研究轻带电粒子诱发反应出射中子双微分产额[J]. 原子核物理评论, 2020, 37(3): 617-620. DOI: 10.11804/NuclPhysRev.37.2019CNPC48
Xin ZHANG, Zhiqiang CHEN, Bingyan LIU, Rui HAN, Guoyu TIAN, Fudong SHI, Hui SUN. Geant4 Simulations of Neutron Production Double Differential Yields in Light Charged Particle Induced Reaction[J]. Nuclear Physics Review, 2020, 37(3): 617-620. DOI: 10.11804/NuclPhysRev.37.2019CNPC48
Citation: Xin ZHANG, Zhiqiang CHEN, Bingyan LIU, Rui HAN, Guoyu TIAN, Fudong SHI, Hui SUN. Geant4 Simulations of Neutron Production Double Differential Yields in Light Charged Particle Induced Reaction[J]. Nuclear Physics Review, 2020, 37(3): 617-620. DOI: 10.11804/NuclPhysRev.37.2019CNPC48

利用GEANT4研究轻带电粒子诱发反应出射中子双微分产额

Geant4 Simulations of Neutron Production Double Differential Yields in Light Charged Particle Induced Reaction

  • 摘要: 轻带电粒子诱发反应产生次级中子的研究对于加速器屏蔽设计和优化具有重要意义。利用Geant4程序结合INCL、BIC、BERT物理模型分别计算了33 MeV的d核、65 MeV的3He核和4He核轰击厚的碳、铜和铅靶在0^\circ15^\circ45^\circ75^\circ135^\circ等方向出射中子的双微分产额,并与实验数据进行了比较。研究表明,对于33 MeV的d核诱发的核反应,INCL模型的计算结果基本上再现了碳靶和铜靶的实验数据,但高估了铅靶直接过程产生的中子。BIC模型和BERT模型的计算结果没有重现弹核削裂过程对应的宽峰。对于65 MeV的3He核诱发的核反应,三个模型的计算结果均未能重现前向角弹核削裂过程产生的中子,但在15^\circ45^\circ75^\circ135^\circ上三个模型的计算结果与实验数据符合较好。对于65 MeV的4He核诱发的核反应,INCL模型的计算结果与碳靶和铜靶的实验数据符合较好,但低估了铅靶的中子产额。BIC模型和BERT模型的计算结果低估了碳靶的实验数据,且在大角度上略微高估了铅靶的实验数据。

     

    Abstract: The study of secondary neutrons produced by light charged particles induced reaction is of great significance to the design and optimization of accelerator shielding. The neutron double differential yields from 33 MeV-d, 65 MeV-3He and 65 MeV-4He bombarding thick carbon, copper and lead targets in the directions of 0^\circ, 15^\circ, 45^\circ, 75^\circ, 135^\circ, are calculated by using Geant4 code with INCL, BIC and BERT physics models, and compared with the experimental data. The results show that, for the 33 MeV d-induced reaction, the results from the INCL model basically reproduced the experimental data of carbon and copper targets, but overestimated the neutron yields corresponding to the direct process in lead target. The results from the BIC model and Bert models failed to reproduce the broad peak due to the stripping of the projectiles. For the 65 MeV 3He-induced reaction, the results from the three models could not reproduce the neutrons in the stripping process in the forward angles. The calculated ones with these three models agreed well with the experimental results in other angles. For the 65 MeV 4He-induced reactions, the calculation results of the INCL model are in good agreement with the experimental ones for carbon and copper targets, but underestimated the neutrons for lead target. The calculation results of the BIC model and BERT model underestimated the experimental data for carbon target and slightly overestimated the experimental ones for lead target in large angles.

     

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