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Observation of He6+t cluster states in Li9

W. H. Ma (马维虎)1,2, D. Patel1,3, Y. Y. Yang (杨彦云)1, J. S. Wang (王建松)4,1,*, Y. Kanada-En'yo5, R. F. Chen (陈若富)1, J. Lubian6, Y. L. Ye (叶沿林)7, Z. H. Yang (杨再宏)7 et al.

Z. Z. Ren (任中洲)8, S. Mukherjee9, J. B. Ma (马军兵)1, S. L. Jin (金仕纶)1, P. Ma (马朋)1, J. X. Li (李加兴)10, Y. S. Song (宋玉收)11, Q. Hu (胡强)1, Z. Bai (白真)1, M. R. Huang (黄美容)12, X. Q. Liu (刘星泉)1, Y. J. Zhou (周远杰)1,13, J. Chen (陈杰)1,13, Z. H. Gao (高志浩)1, F. F. Duan (段芳芳)1,14, S. Y. Jin (金树亚)1, S. W. Xu (许世伟)1, G. M. Yu (余功明)1, G. Z. Shi (石国柱)1, Q. Wang (王琦)1, T. F. Wang (王涛峰)15, X. Y. Ju (巨欣跃)16, Z. G. Hu (胡正国)1, Y. H. Zhang (张玉虎)1, X. H. Zhou (周小红)1, H. S. Xu (徐瑚珊)1, G. Q. Xiao (肖国青)1, and W. L. Zhan (詹文龙)1

  • 1Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Science, Lanzhou 730000, People's Reublic of China
  • 2Key Laboratory of Nuclear Physics and Ion-beam Application, Institute of Modern Physics, Fudan University, Shanghai 200433, People's Republic of China
  • 3Department of Physics, Sardar Vallabhbhai National Institute of Technology, Surat 395007, India
  • 4School of Science, Huzhou University, Huzhou 313000, People's Republic of China
  • 5Department of Physics, Kyoto University, Kyoto 606-8502, Japan
  • 6Instituto de Fısica, Universidade Federal Fluminense, Avenida Litoranea s/n, Gragoatá, Niteroi, Rio de Janeiro 24210-340, Brazil
  • 7State Key Laboratory of Nuclear Physics and Technology, School of Physics, Peking University, Beijing 100871, People's Reublic of China
  • 8School of Physics Science and Engineering, Tongji University, Shanghai 200092, People's Reublic of China
  • 9Physics Department, Faculty of Science, M.S. University of Baroda, Vadodara 390002, India
  • 10Southwest University, Chongqing 400044, People's Reublic of China
  • 11Fundamental Science on Nuclear Safety and Simulation Technology Laboratory, Harbin Engineering University, Harbin 150001, China
  • 12College of Physics and Electronics information, Inner Mongolia University for Nationalities, Tongliao 028000, China
  • 13University of Chinese Academy of Science, Beijing 100049, People's Reublic of China
  • 14School of Nuclear Science and Technology, Lanzhou University, Lanzhou 730000, China
  • 15BeiHang University, Beijing 100083, People's Reublic of China
  • 16University of Science and Technology of China, Hefei 230026, People's Reublic of China

  • *wjs@zjhu.edu.cn

Phys. Rev. C 103, L061302 – Published 28 June, 2021

DOI: https://doi.org/10.1103/PhysRevC.103.L061302

Abstract

Two resonant states above the He6+t threshold in Li9 have been observed using a Li9 beam bombarding a Pb208 target at the incident energy of 32.7 MeV/nucleon. An angular correlation analysis and the continuum discretized coupled channels (CDCC) method have been applied to identify the spin-parities of observed resonant states. The obtained results from the present methods of calculations indicate the first resonant state at 9.8 MeV with a spin-parity of 3/2−. The second resonant state at 12.8 MeV with limited statistics might suggest the spin-parity of 7/2−, which needs to be further investigated. The monopole matrix element of the 3/2− state is extracted as 8.1(8) fm2 with a multipole decomposition analysis based on a distorted wave Born approximation (DWBA) calculation. These results give the first experimental evidence supporting the theoretical prediction of the generator coordinate method (GCM) and disclose the feature of clustering structure involving two neutron-rich clusters in the neutron-rich nucleus Li9.

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