1. New short-lived isotope 223Np and the absence of the Z = 92 subshell closure near N = 126
- Author
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H.B. Yang, J. Jiang, Z. H. Li, Miao Liu, Cenxi Yuan, X. Wang, Zhi Liu, Yu-Tong Wang, K.L. Wang, Feng-Shou Zhang, C. J. Lin, Jing Li, Luodan Yu, J. G. Wang, Guang-Cheng Xiao, Zibao Gan, H. Lu, Xiaojuan Zhou, M. D. Sun, X.Y. Liu, N. R. Ma, W.Q. Zhang, Chong Qi, Li-Jie Sun, Bing Ding, Tao Huang, Wei Zuo, Lin Ma, Zhoubin Zhang, and H. S. Xu
- Subjects
Physics ,Nuclear and High Energy Physics ,Spectrometer ,Isotope ,010308 nuclear & particles physics ,Nuclear structure ,Pulse processing ,01 natural sciences ,lcsh:QC1-999 ,Recoil separator ,0103 physical sciences ,Nuclear fusion ,Decay chain ,Atomic physics ,010306 general physics ,Ground state ,lcsh:Physics - Abstract
The N = 130 short-lived isotope 223 Np was produced as evaporation residue (ER) in the fusion reaction 40 Ar + 187 Re at the gas-filled recoil separator Spectrometer for Heavy Atom and Nuclear Structure (SHANS). It was identified through temporal and spatial correlations with α decays of 215 Ac and/or 211 Fr, the third and fourth members of the α -decay chain starting from 223 Np. The pileup signals of ER( 223 Np)– α ( 223 Np)– α ( 219 Pa) were resolved by using the digital pulse processing technique. An α decay with half-life of T 1 / 2 = 2.15 ( 52 100 ) μs and energy of E α = 9477 ( 44 ) keV was attributed to 223 Np. Spin and parity of 9 / 2 − were tentatively proposed for the ground state of 223 Np by combining the reduced α -decay width and large-scale shell-model calculations. This assignment together with the proton separation energy disprove the existence of a Z = 92 subshell closure.
- Published
- 2017
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