$\bar{K}NN$ quasi-bound state and the $\bar{K}N$ interaction: coupled-channel Faddeev calculations of the $\bar{K}NN - πΣN$ system

dc.creatorShevchenko, N. V.
dc.creatorGal, A.
dc.creatorMareš, J.
dc.creatorRévai, J.
dc.date2007-06-29
dc.date2007-09-27
dc.date.accessioned2026-07-07T10:56:31Z
dc.date.available2026-07-07T10:56:31Z
dc.descriptionCoupled-channel three-body calculations of an $I=1/2$, $J^π=0^-$ $\bar{K}NN$ quasi-bound state in the $\bar{K}NN - πΣN$ system were performed and the dependence of the resulting three-body energy on the two-body $\bar{K}N - πΣ$ interaction was investigated. Earlier results of binding energy $B_{K^-pp} \sim 50 -70$ MeV and width $Γ_{K^-pp} \sim 100$ MeV are confirmed [N.V. Shevchenko {\it et al.}, Phys. Rev. Lett. {\bf 98}, 082301 (2007)]. It is shown that a suitably constructed energy-independent complex $\bar{K}N$ potential gives a considerably shallower and narrower three-body quasi-bound state than the full coupled-channel calculation. Comparison with other calculations is made.
dc.description22 pages, 7 figures, 4 tables; minor corrections, accepted for publication in Phys. Rev. C
dc.identifierhttps://arxiv.org/abs/0706.4393
dc.identifierhttp://arxiv.org/abs/0706.4393
dc.identifierPhys.Rev.C76:044004,2007
dc.identifierdoi:10.1103/PhysRevC.76.044004
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/186440
dc.subjectNuclear Theory
dc.title$\bar{K}NN$ quasi-bound state and the $\bar{K}N$ interaction: coupled-channel Faddeev calculations of the $\bar{K}NN - πΣN$ system
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