{ "id": "0804.1210", "version": "v1", "published": "2008-04-08T08:36:11.000Z", "updated": "2008-04-08T08:36:11.000Z", "title": "On the nature of the $Λ(1405)$ and $Λ(1670)$ from their $N_c$ behavior in chiral dynamics", "authors": [ "L. Roca", "T. Hyodo", "D. Jido" ], "comment": "29 pages, 8 figures", "journal": "Nucl.Phys.A809:65-87,2008", "doi": "10.1016/j.nuclphysa.2008.05.014", "categories": [ "hep-ph" ], "abstract": "We study the behavior with the number of colors ($N_c$) of the $\\Lambda(1405)$ and $\\Lambda(1670)$ resonances obtained dynamically within the chiral unitary approach. The leading order meson-baryon interaction, used as the kernel of the unitarization procedure, manifests a nontrivial $N_c$ dependence of the flavor SU(3) representation for baryons. As a consequence, the SU(3) singlet (or $\\bar{K}N$) component of the $\\Lambda(1405)$ states remains bound in the large $N_c$ limit, while the other components dissolve into the continuum. Introducing explicit SU(3) breaking, we obtain the $N_c$ dependence of the excitation energy, masses and widths of the physical $\\Lambda(1405)$ and $\\Lambda(1670)$ resonance. The $N_c$ behavior of the decay width is found to be different from the general counting rule for a $qqq$ state, indicating the dynamical origin of these resonances.", "revisions": [ { "version": "v1", "updated": "2008-04-08T08:36:11.000Z" } ], "analyses": { "subjects": [ "11.30.Rd", "14.20.-c", "11.15.Pg" ], "keywords": [ "chiral dynamics", "chiral unitary approach", "states remains bound", "leading order meson-baryon interaction", "dependence" ], "tags": [ "journal article" ], "publication": { "publisher": "Elsevier", "journal": "Nuclear Physics A", "year": 2008, "month": "Aug", "volume": 809, "number": 1, "pages": 65 }, "note": { "typesetting": "TeX", "pages": 29, "language": "en", "license": "arXiv", "status": "editable", "inspire": 783016, "adsabs": "2008NuPhA.809...65R" } } }