{ "id": "1305.0786", "version": "v2", "published": "2013-05-03T17:29:10.000Z", "updated": "2013-05-07T16:12:14.000Z", "title": "Hidden beauty baryon states in the local hidden gauge approach with heavy quark spin symmetry", "authors": [ "C. W. Xiao", "E. Oset" ], "comment": "misprint corrected", "categories": [ "hep-ph" ], "abstract": "Using a coupled channel unitary approach, combining the heavy quark spin symmetry and the dynamics of the local hidden gauge, we investigate the meson-baryon interaction with hidden beauty and obtain several new states of $N^*$ around 11 GeV. We consider the basis of states $\\eta_b N$, $\\Upsilon N$, $B \\Lambda_b$, $B \\Sigma_b$, $B^* \\Lambda_b$, $B^* \\Sigma_b$, $B^* \\Sigma_b^*$ and find four basic bound states which correspond to $B \\Sigma_b$, $B \\Sigma_b^*$, $B^* \\Sigma_b$ and $B^* \\Sigma_b^*$, decaying mostly into $\\eta_b N$ and $\\Upsilon N$ and with a binding energy about 50-130 MeV with respect to the thresholds of the corresponding channel. All of them have isospin $I=1/2$, and there are no bound states or resonances in $I=3/2$. The $B \\Sigma_b$ state appears in $J=1/2$, the $B \\Sigma_b^*$ in $J=3/2$, the $B^* \\Sigma_b$ appears nearly degenerate in $J=1/2, ~3/2$ and the $B^* \\Sigma_b^*$ appears nearly degenerate in $J=1/2, ~3/2, ~5/2$. These states have a width from $6 \\sim 45 \\mev$ except for the one in $J=5/2$ which has zero width since it cannot decay into any of the states of the basis chosen.", "revisions": [ { "version": "v2", "updated": "2013-05-07T16:12:14.000Z" } ], "analyses": { "keywords": [ "heavy quark spin symmetry", "local hidden gauge approach", "hidden beauty baryon states" ], "tags": [ "journal article" ], "publication": { "doi": "10.1140/epja/i2013-13139-y", "journal": "European Physical Journal A", "year": 2013, "month": "Nov", "volume": 49, "pages": 139 }, "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "inspire": 1231967, "adsabs": "2013EPJA...49..139X" } } }