1 Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai 201800, China; 2 CAS Innovative Academy in TMSR Energy System, Chinese Academy of Sciences, Shanghai 201800, China; 3 University of Chinese Academy of Sciences, Beijing 100049, China; 4 Key Laboratory of Nuclear Data, China Institute of Atomic Energy, Beijing 102413, China; 5 Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China; 6 China Spallation Neutron Source, Dongguan 523803, China; 7 Shanghai Advanced Research Institute, Chinese Academy of Sciences, Shanghai 201210, China
Abstract The neutron capture cross section of 232Th was measured at the neutron time-of-flight facility Back-n of China Spallation Neutron Source (CSNS) for the first time. The measurement was performed with 4 hydrogen-free deuterated benzene C6D6 liquid scintillation detectors, in the ES#2 experiment station on the beam line, at a distance of about 76 m from the neutron-production assembly. The total energy detection principle in combination with the pulse height weighting technique (PHWT) was applied to analyze the measured data. Results of the 232Th (n,γ) reaction cross section in the unresolved resonance region from 4 keV to 100 keV were obtained, which shows a good agreement with the existing experimental data from EXFOR, as well as with the evaluated data from the ENDF/B-VIII.0 and CENDL-3.1. In addition, the excitation function of 232Th (n,γ)233Th reaction in the unresolved resonance region was theoretically calculated by using the code TALYS-1.95. By fitting the experimental cross section and theoretical data, the average parameters in the unresolved resonance region were extracted. The datasets are openly available at http://dx.doi.org/10.11922/sciencedb.j00113.00015.
Fund: Project supported by the Chinese TMSR Strategic Pioneer Science and Technology Project (Grant No. XDA02010000) and the National Natural Science Foundation of China (Grant No. 11790321).
Corresponding Authors:
Xiaohe Wang, Jingen Chen, Xiangzhou Cai
E-mail: wangxiaohe@sinap.ac.cn;chenjingen@sinap.ac.cn;caixiangzhou@sinap.ac.cn
Cite this article:
Bing Jiang(姜炳), Jianlong Han(韩建龙), Jie Ren(任杰), Wei Jiang(蒋伟), Xiaohe Wang(王小鹤), Zian Guo(郭子安), Jianglin Zhang(张江林), Jifeng Hu(胡继峰), Jingen Chen(陈金根), Xiangzhou Cai(蔡翔舟), Hongwei Wang(王宏伟), Longxiang Liu(刘龙祥), Xinxiang Li(李鑫祥), Xinrong Hu(胡新荣), and Yue Zhang(张岳) Measurement of 232Th (n,γ) cross section at the CSNS Back-n facility in the unresolved resonance region from 4 keV to 100 keV 2022 Chin. Phys. B 31 060101
[1] Cai X Z, Dai Z M and Xu H J 2016 Physics 45 578 (in Chinese) [2] Jiang M H, Xu H J and Dai Z M 2012 Bull. Chin. Acad. Sci. 27 366 (in Chinese) [3] Bowman C D, Arthur E D, Lisowski P W, et al. 1992 Nucl. Instr. Meth. A320 336 [4] Hu J F, Wang X H, Wu J H, Cai X Z, Han J L and Chen J G 2018 At. Energy Sci. Technol. 52 1206 (in Chinese) [5] Aerts G, Abbondanno U, Álvarez P H, et al. 2006 Phys. Rev. C73 054610 [6] Gunsing F, Berthoumieux E, Aerts G, et al. 2012 Phys. Rev. C85 064601 [7] Lobo G, Corvi F, Schillebeeckx P, Janeva N, Brusegan A and Mutti P 2002 J. Nucl. Sci. Technol. 39 429 [8] Borella A, Volev K, Brusegan A, Schillebeeckx P, Corvi F, Koyumdjieva N, Janeva N and Lukyanov A A 2006 Nucl. Sci. Eng. 152 1 [9] Tang J Y, Jing H T, Xia H H, Tang H Q, Zhang C, Zhou Z Y, Ruan X C, Zhang Q W and Yang Z 2013 At. Energy Sci. Technol. 47 1089 (in Chinese) [10] Tang J Y, An Q, Bai J B, et al. 2021 Nucl. Sci. Tech. 32 1 [11] Wei J, Chen H S, Chen Y W, et al. 2009 Nucl. Instr. Meth. A600 10 [12] Chen H S and Wang X L 2016 Nat. Mater.15 689 [13] Koning A J and Rochman D 2012 Nucl. Data Sheets113 2841 [14] Zhang L Y, Jing H T, Tang J Y, Li Q, Ruan X C, Ren J, Ning C J, Yu Y J, Tan Z X, Wang P C, He Y C and Wang X Q 2018 Appl. Radiat. Isot. 132 212 [15] Jiang B, Han J L, Jiang W, Hu J F, Wang X H, Chen J G and Cai X Z 2021 Nucl. Instr. Meth. A1013 165677 [16] Jing H T, Tang J Y, Tang H Q, Xia H H, Liang T J, Zhou Z Y, Zhong Q P and Ruan X C 2010 Nucl. Instr. Meth. A621 91 [17] Macklin R L and Gibbons J H 1967 Phys. Rev.159 1007 [18] Abbondanno U, Aerts G, Alvarez H, et al. 2004 Nucl. Instr. Meth. A521 454 [19] Borella A, Aerts G, Gunsing F, Moxon M, Schillebeeckx P and Wynants R 2007 Nucl. Instr. Meth. A577 626 [20] Ren J, Ruan X C, Bao J, et al. 2019 Radiat. Detec. Technol. Meth.3 1 [21] Antcheva I, Ballintijn M, Bellenot B, et al. 2009 Comput. Phys. Commun180 2499 [22] Ren J, Ruan X C, Jiang W, et al. 2021 Chin. Phys. C (Accepted) [23] Li X X, Liu L X, Jiang W, et al. 2020 Nucl. Tech. 43 86 (in Chinese) [24] Hu X R, Fan G T, Jiang W, et al. 2021 Nucl. Sci. Tech. 32 1 [25] Ren J, Ruan X C, Jiang W, et al.2021 Nucl. Instr. Meth. A 985 164703 [26] Agostinelli S, Allison J, Amako K, et al. 2003 Nucl. Instr. Meth. A506 250 [27] Massimi C, Domingo-Pardo C, Vannini G, et al. 2010 Phys. Rev. C81 044616 [28] Lederer C, Massimi C, Berthoumieux E, et al. 2014 Phys. Rev. C89 025810 [29] Mastromarco M, Manna A, Aberle O, et al. 2019 Eur. Phys. J. A55 1 [30] Tain J L, Gunsing F, Aniel-Cano D, et al. 2002 J. Nucl. Sci. Technol. 39 689 [31] Macklin R L, Halperin J and Winters R R 1979 Nucl. Instr. Meth.164 213 [32] Chen Y H, Luan G Y, Bao J, et al. 2019 Eur. Phys. J. A55 1 [33] Li Q, Luan G, Bao J, et al. 2019 Nucl. Instr. Meth. A946 162497 [34] Li X X, Liu L X, Jiang W, et al. 2021 Phys. Rev. C104 054302 [35] Larson N M and Volev K N 2002 PHYSOR 2002, October 7-10, 2002, Seoul, Korea [36] Larson N M 2000 Technical Report, ORNL/TM-9179 R5, Oak Ridge National Laboratory, Oak Ridge, TN, USA [37] Brown D A, Chadwick M B and Capote R 2018 Nucl. Data Sheets148 1 [38] Ge Z G, Zhao Z X, Xia H H, Zhuang Y X, Liu T J, Zhang J S and Wu H C 2011 J. Korean Phys. Soc59 1052 [39] Soukhovitskii E S, Capote R, Quesada J M and Chiba S 2005 Phys. Rev. C72 024604 [40] Rowlands J 2006 Ann. Nucl. Energy33 1157
[1]
New experimental measurement of natSe(n, γ) cross section between 1 eV to 1 keV at the CSNS Back-n facility Xin-Rong Hu(胡新荣), Long-Xiang Liu(刘龙祥), Wei Jiang(蒋伟), Jie Ren(任杰), Gong-Tao Fan(范功涛), Hong-Wei Wang(王宏伟), Xi-Guang Cao(曹喜光), Long-Long Song(宋龙龙), Ying-Du Liu(刘应都), Yue Zhang(张岳), Xin-Xiang Li(李鑫祥), Zi-Rui Hao(郝子锐), Pan Kuang(匡攀), Xiao-He Wang(王小鹤), Ji-Feng Hu(胡继峰), Bing Jiang(姜炳), De-Xin Wang(王德鑫), Suyalatu Zhang(张苏雅拉吐), Zhen-Dong An(安振东), Yu-Ting Wang(王玉廷), Chun-Wang Ma(马春旺), Jian-Jun He(何建军), Jun Su(苏俊), Li-Yong Zhang(张立勇), Yu-Xuan Yang(杨宇萱), Sheng Jin(金晟), and Kai-Jie Chen(陈开杰). Chin. Phys. B, 2022, 31(8): 080101.
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