{ "id": "hep-ph/0605019", "version": "v5", "published": "2006-05-01T04:56:51.000Z", "updated": "2007-01-03T03:02:33.000Z", "title": "New Heavy-Light Mesons $Q\\bar q$", "authors": [ "Takayuki Matsuki", "Toshiyuki Morii", "Kazutaka Sudoh" ], "comment": "14 pages, 4 figures, references corrected", "journal": "Prog.Theor.Phys.117:1077-1098,2007", "doi": "10.1143/PTP.117.1077", "categories": [ "hep-ph", "hep-ex" ], "abstract": "We succeed in reproducing the $\\ell=1$ $B$ mesons, $B_1(5720)$, $B_2^*(5745)$, and $B_{s2}^*(5839)$ that are recently reported by D0 and CDF, by using our semirelativistic quark potentila model, which also succeeded in predicting the mass spectra of the narrow $D_{sJ}$ as well as broad $D_0^*(0^+)$ and $D_1'(1^+)$ particles a couple of years ago. Mass of higher excited states ($\\ell=1, 2$) of $B$ and $B_s$ mesons, which are not yet observed, is also predicted at the first order in $p/m_b$. We find the corresponding $B_{sJ}$ are below $BK/B^*K$ threshold and should have narrow decay widths contrary to most other predictions. Also already established states ($\\ell=0$ and $\\ell=1$) of $D$, $D_s$, $B$, and $B_s$ heavy mesons are simultaneously reproduced in good agreement with experimental data within one percent of accuracy. To calculate these $D/D_s$ and $B/B_s$ heavy mesons we use different values of strong coupling $\\alpha_s$ which conforms to a notion of running coupling.", "revisions": [ { "version": "v5", "updated": "2007-01-03T03:02:33.000Z" } ], "analyses": { "subjects": [ "12.40.Yx", "14.40.Lb", "12.39.Pn", "12.39.Hg", "14.40.Nd" ], "keywords": [ "heavy-light mesons", "semirelativistic quark potentila model", "narrow decay widths contrary", "heavy mesons", "higher excited states" ], "tags": [ "journal article" ], "note": { "typesetting": "TeX", "pages": 14, "language": "en", "license": "arXiv", "status": "editable", "inspire": 715646 } } }