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Measurements of neutron energy spectra of 9Be(d,n)10B reaction with a thick beryllium target Supported by the National Natural Science Foundation of China (11875155, 11705071, 12075105), the NSFC-Nuclear Technology Innovation Joint Fund (U1867213), the NSAF (U1830102), the Fundamental Research Funds for the Central Universities of China (lzujbky-2020-kb09) and the Project of National Defense Science and Technology Industry for Nuclear Power Technology Innovation Center (HDLCXZX-2019-HD-33)
Chinese Physics C ( IF 3.6 ) Pub Date : 2021-01-27 , DOI: 10.1088/1674-1137/abce13
Shuang-Jiao Zhang 1 , Zhi-Jie Hu 1 , Zhi-Ming Hu 1 , Chao Han 1 , Xiao-Hou Bai 1 , Chang-Qi Liu 1 , Chang Huang 1 , Qin Xie 1 , Dong-Ying Huo 1 , Kang Wu 1 , Yang-Bo Nie 2 , Yan-Yan Ding 2 , Kai Zhang 2 , Yu Zhang 1, 3 , Zhi-Yong Deng 4 , Rui Guo 4 , Zheng Wei 1, 3 , Ze-En Yao 1, 3
Affiliation  

Novel measurements of the neutron energy spectra of the 9Be(d,n)10B reaction with a thick beryllium target are performed using a fast neutron time-of-flight (TOF) spectrometer for the neutron emission angles $\theta=0^\circ$ and $45^\circ$, and the incident deuteron energies are 250 and 300 keV, respectively. The neutron contributions from the 9Be(d,n)10B reaction are distributed relatively independently for the ground state and the first, second, and third excited states of 10B. The branching ratios of the 9Be(d,n)10B reaction for the different excited states of 10B are obtained for the neutron emission angles $\theta=0^\circ$ and $45^\circ$, and the incident deuteron energies are 250 and 300 keV, respectively. The branching ratio of the 9Be(d,n)10B reaction for the third excited state decreases with increase in the incident deuteron energy, and the branching ratios for the ground state and the second excited state increase with increase in the neutron emission angle.



中文翻译:

9Be(d,n)10B 与厚铍靶反应的中子能谱测量 国家自然科学基金 (11875155, 11705071, 12075105), NSFC-核技术创新联合基金 (U1867213), NSAF (U1830102)、中央高校基本科研业务费专项资金(lzujbky-2020-kb09)和国防科技产业核电技术创新中心项目(HDLCXZX-2019-HD-33)

9 Be( d , n ) 10 B 反应与厚铍靶的中子能谱的新测量是使用快中子飞行时间 (TOF) 光谱仪测量中子发射角$\theta=0^\circ$$45^\circ$, 和入射氘核能量分别为 250 和 300 keV。9 Be( d , n ) 10 B 反应的中子贡献相对独立地分布在10 B 的基态和第一、第二和第三激发态。9 Be( d , n )的支化率对于中子发射角和,得到10 B不同激发态的 10 B 反应,入射氘核能量分别为 250 和 300 keV。9 Be( d , n ) 10 B反应对第三激发态的分支比随着入射氘核能量的增加而减小,基态和第二激发态的分支比随着中子发射角的增加而增加.$\theta=0^\circ$$45^\circ$

更新日期:2021-01-27
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