{ "id": "1504.07735", "version": "v1", "published": "2015-04-29T06:41:48.000Z", "updated": "2015-04-29T06:41:48.000Z", "title": "Resonant states of neutron-rich $Λ$ hypernucleus $^7_Λ$He", "authors": [ "E. Hiyama", "M. Isaka", "M. Kamimura", "T. Myo", "T. Motoba" ], "comment": "6 pages, 4 figures,published in Physical Review C", "categories": [ "nucl-th" ], "abstract": "The structure of neutron-rich $\\Lambda$ hypernucleus, $^7_{\\Lambda}$He is studied within the framework of an $\\alpha +\\Lambda +n+n$ four-body cluster model. We predict second $3/2^+$ and $5/2^+$ states, corresponding to a $0s$ $\\Lambda$ coupled to the second $2^+$ state of $^6$He, as narrow resonant states with widths $\\Gamma \\sim 1$ MeV to be at 0.03 MeV and 0.07 MeV respect to the $\\alpha +\\Lambda +n+n$ threshold. From an estimation of the differential cross section for the $^7{\\rm Li} (\\gamma,K^+) ^7_{\\Lambda}$He reaction, there is a possibility to observe these state at JLab in the future. We also calculate the second $2^+$ state of $^6$He as resonant state within the framework of an $\\alpha +n+n$ three-body cluster model. Our result is $2.81$ MeV with $\\Gamma =$4.63 MeV with respect to the $\\alpha +n+n$ threshold. This energy position is $\\sim 1$ MeV higher, and with a much broader decay width, than the recent SPIRAL data. It is suggested that an experiment at JLab to search for the second $3/2^+$ and $5/2^+$ states of $^7_{\\Lambda}$He would provide an opportunity to confirm the second $2^+$ state of the core nucleus $^6$He.", "revisions": [ { "version": "v1", "updated": "2015-04-29T06:41:48.000Z" } ], "analyses": { "subjects": [ "21.80.+a", "21.60.Gx", "27.20.+n" ], "keywords": [ "hypernucleus", "neutron-rich", "narrow resonant states", "four-body cluster model", "differential cross section" ], "publication": { "doi": "10.1103/PhysRevC.91.054316" }, "note": { "typesetting": "TeX", "pages": 6, "language": "en", "license": "arXiv", "status": "editable", "inspire": 1365339 } } }