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Spectroscopy of A=9 hyperlithium with the (e,e′K+) reaction

T. Gogami1,2, C. Chen3, D. Kawama2, P. Achenbach4, A. Ahmidouch5, I. Albayrak3, D. Androic6, A. Asaturyan7, R. Asaturyan7,* et al. (HKS (JLab E05-115) Collaboration)

R. Asaturyan7,*, O. Ates3, P. Baturin8, R. Badui8, W. Boeglin8, J. Bono8, E. Brash9, P. Carter9, A. Chiba2, E. Christy3, S. Danagoulian5, R. De Leo10, D. Doi2, M. Elaasar11, R. Ent12, Y. Fujii2, M. Fujita2, M. Furic6, M. Gabrielyan8, L. Gan13, F. Garibaldi14, D. Gaskell12, A. Gasparian5, Y. Han3, O. Hashimoto2,*, T. Horn12, B. Hu15, Ed. V. Hungerford16, M. Jones12, H. Kanda2, M. Kaneta2, S. Kato17, M. Kawai2, H. Khanal8, M. Kohl3, A. Liyanage3, W. Luo15, K. Maeda2, A. Margaryan7, P. Markowitz8, T. Maruta2, A. Matsumura2, V. Maxwell8, D. Meekins12, A. Mkrtchyan7, H. Mkrtchyan7, S. Nagao2, S. N. Nakamura2, A. Narayan18, C. Neville8, G. Niculescu19, M. I. Niculescu19, A. Nunez8, Nuruzzaman18, Y. Okayasu2, T. Petkovic6, J. Pochodzalla4, X. Qiu15, J. Reinhold8, V. M. Rodriguez20, C. Samanta21, B. Sawatzky12, T. Seva6, A. Shichijo2, V. Tadevosyan7, L. Tang3,12, N. Taniya2, K. Tsukada2, M. Veilleux9, W. Vulcan12, F. R. Wesselmann22, S. A. Wood12, T. Yamamoto2, L. Ya3, Z. Ye3, K. Yokota2, L. Yuan3, S. Zhamkochyan7, and L. Zhu3 (HKS (JLab E05-115) Collaboration)

  • 1Graduate School of Science, Kyoto University, Kyoto, Kyoto 606-8502, Japan
  • 2Graduate School of Science, Tohoku University, Sendai, Miyagi 980-8578, Japan
  • 3Department of Physics, Hampton University, Hampton, Virginia 23668, USA
  • 4Institute for Nuclear Physics, Johannes Gutenberg-University, D-55099 Mainz, Germany
  • 5Department of Physics, North Carolina A&T State University, Greensboro, North Carolina 27411, USA
  • 6Department of Physics, University of Zagreb, HR-10000 Zagreb, Croatia and Department of Applied Physics, University of Zagreb, HR-10000 Zagreb, Croatia
  • 7A. I. Alikhanyan National Science Laboratory, Yerevan 0036, Armenia
  • 8Department of Physics, Florida International University, Miami, Florida 27411, USA
  • 9Department of Physics, Computer Science and Engineering, Christopher Newport University, Newport News, Virginia 23606, USA
  • 10Istituto Nazionale di Fisica Nucleare, Sezione di Bari, University of Bari, I-70126 Bari, Italy
  • 11Department of Physics, Southern University at New Orleans, New Orleans, Louisiana 70126, USA
  • 12Thomas Jefferson National Accelerator Facility (JLab), Newport News, Virginia 23606, USA
  • 13Department of Physics, University of North Carolina at Wilmington, Wilmington, North Carolina 28403, USA
  • 14INFN, Sezione Sanità, Istituto Superiore di Sanità, 00161 Rome, Italy
  • 15Nuclear Physics Institute, Lanzhou University, Gansu 730000, China
  • 16Department of Physics, University of Houston, Houston, Texas 77204, USA
  • 17Department of Physics, Yamagata University, Yamagata, 990-8560, Japan
  • 18Mississippi State University, Mississippi State, Mississippi 39762, USA
  • 19Department of Physics and Astronomy, James Madison University, Harrisonburg, Virginia 22807, USA
  • 20División de Ciencias y Tecnología, Universidad Ana G. Méndez, Recinto de Cupey, San Juan 00926, Puerto Rico
  • 21Department of Physics and Astronomy, Virginia Military Institute, Lexington, Virginia 24450, USA
  • 22Department of Physics, Xavier University of Louisiana, New Orleans, Louisiana 70125, USA

  • *Deceased.

Phys. Rev. C 103, L041301 – Published 5 April, 2021

DOI: https://doi.org/10.1103/PhysRevC.103.L041301

Abstract

Missing mass spectroscopy with the (e,e′K+) reaction was performed at Jefferson Laboratory's Hall C for the neutron-rich Λ hypernucleus LiΛ9. The ground-state (g.s.) energy was obtained to be BΛg.s.=8.84±0.17stat.±0.15sys.MeV by using shell-model calculations of a cross-section ratio and an energy separation of the spin doublet states (3/21+ and 5/21+). In addition, peaks that are considered to be states of [Li8(3+)⊗sΛ=3/22+,1/2+] and [Li8(1+)⊗sΛ=5/22+,7/2+] were observed at EΛ(no.2)=1.74±0.27stat.±0.11sys. and EΛ(no.3)=3.30±0.24stat.±0.11sys.MeV, respectively. The EΛ(no.3) is larger than shell-model predictions by a few hundred keV, and the difference would indicate that a He5+t structure is more developed for the 3+ state than those for the 2+ and 1+ states in a core nucleus Li8 as a cluster model calculation suggests.

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