[1] Wan Y, Li J, Liu Y, et al. Overview of the present progress and activities on the CFETR [J]. Nucl. Fusion, 2017, 57: 102009.1-102009.17.
[2] Zhuang G, Li G, Li J, et al. Progress of the CFETR design [J]. Nucl. Fusion, 2019, 59: 112010.1 -112010.14.
[3] Wang X, Feng K, Chen Y, et al. Current design and R&D progress of CN HCCB TBS [J]. Nucl. Fusion, 2019, 59: 076019.1-076019.8.
[4] Forster R A, Godfrey T N K. MCNP - a general Monte-Carlo code for neutrons and photon transport [J]. Photonics and Statistical Physics, 1985, 240(10): 33-55.
[5] Qu S, Cao Q, Duan X, et al. Neutronics effects of homogeneous model on solid breeder blanket of CFETR [J]. Fusion Engineering and Design, 2020, 160: 111825.
[6] Lopez Al-dama D, Trkov A. FENDL-2.1: update of an evaluated nuclear data library for fusion applications [R]. Vienna: IAEA Report INDC (NDS)-467, 2004.
[7] Cao Qixiang, Zhao Fengchao, Zhao Zhou, et al. Neutronic calculation analysis for CN HCCB TBM-set [J]. Plasma Science and Technology, 2015, 17(7): 607 -611.
[8] Cao Qixiang. Neutronics analysis report for CN HCCB TBS [R]. ITER_D_N7T8EG, June, 2014.
[9] 巩保平,冯勇进,何开辉. 固态氚增殖包层中球床堆积性能研究 [J]. 核聚变与等离子体物理, 2018, 38(4): 420-427.
[10] 秦冬, 巨海涛, 强胜龙, 等. 双重非均匀性对燃耗计算影响的初步分析 [J]. 科技创新导报, 2015, (24): 247-249.
[11] 谢仲生. 核反应堆物理分析 [M]. 北京: 原子能出版社, 1985.
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