{ "id": "1607.02058", "version": "v1", "published": "2016-07-07T15:50:09.000Z", "updated": "2016-07-07T15:50:09.000Z", "title": "On the structure observed in the in-flight ${}^{3}\\text{He} ( K^{-} , \\, Λp ) n$ reaction at J-PARC", "authors": [ "Takayasu Sekihara", "Eulogio Oset", "Angels Ramos" ], "comment": "27 pages, 18 EPS figures", "categories": [ "hep-ph", "nucl-ex", "nucl-th" ], "abstract": "A theoretical investigation is done to clarify the origin of the peak structure observed near the $K^{-} p p$ threshold in the in-flight ${}^{3}\\text{He} ( K^{-}, \\, \\Lambda p ) n$ reaction of the J-PARC E15 experiment, which could be a signal of the lightest kaonic nuclei, that is, the $\\bar{K} N N (I=1/2)$ state. For the investigation, we evaluate the $\\Lambda p$ invariant mass spectrum assuming two possible scenarios to interpret the experimental peak. One assumes that the $\\Lambda (1405)$ resonance is generated after the emission of an energetic neutron from the absorption of the initial $K^-$, not forming a bound state with the remaining proton. This uncorrelated $\\Lambda (1405) p$ system subsequently decays into the final $\\Lambda p$. The other scenario implies that, after the emission of the energetic neutron, a $\\bar{K} N N$ bound state is formed, decaying eventually into a $\\Lambda p$ pair. Our results show that the experimental signal observed in the in-flight ${}^{3}\\text{He} ( K^{-} , \\, \\Lambda p ) n$ reaction at J-PARC is qualitatively well reproduced by the assumption that a $\\bar{K} N N$ bound state is generated in the reaction, definitely discarding the interpretation in terms of an uncorrelated $\\Lambda (1405) p$ state.", "revisions": [ { "version": "v1", "updated": "2016-07-07T15:50:09.000Z" } ], "analyses": { "keywords": [ "bound state", "energetic neutron", "j-parc e15 experiment", "lightest kaonic nuclei", "invariant mass spectrum assuming" ], "note": { "typesetting": "TeX", "pages": 27, "language": "en", "license": "arXiv", "status": "editable" } } }