{ "id": "0704.0605", "version": "v2", "published": "2007-04-04T16:12:31.000Z", "updated": "2007-08-27T13:21:54.000Z", "title": "Reconciling the X(3872) with the near-threshold enhancement in the D^0\\bar{D}^{*0} final state", "authors": [ "C. Hanhart", "Yu. S. Kalashnikova", "A. E. Kudryavtsev", "A. V. Nefediev" ], "comment": "RevTeX4, 17 pages, some references updated and corrected, version published in Phys. Rev. D", "journal": "Phys.Rev.D76:034007,2007", "doi": "10.1103/PhysRevD.76.034007", "categories": [ "hep-ph", "hep-ex" ], "abstract": "We investigate the enhancement in the D^0\\bar{D}^0\\pi^0 final state with the mass M=3875.2\\pm 0.7^{+0.3}_{-1.6}\\pm 0.8 MeV found recently by the Belle Collaboration in the B\\to K D^0\\bar{D}^0\\pi^0 decay and test the possibility that this is yet another manifestation of the well-established resonance X(3872). We perform a combined Flatte analysis of the data for the D^0\\bar{D}^0\\pi^0 mode, and for the \\pi^+\\pi^- J/\\psi mode of the X(3872). Only if the X(3872) is a virtual state in the D^0\\bar{D}^{*0} channel, the data on the new enhancement comply with those on the X(3872). In our fits, the mass distribution in the D^0\\bar{D}^{*0} mode exhibits a peak at 2-3 MeV above the D^0\\bar{D}^{*0} threshold, with a distinctive non-Breit-Wigner shape.", "revisions": [ { "version": "v2", "updated": "2007-08-27T13:21:54.000Z" } ], "analyses": { "subjects": [ "13.25.Gv", "14.40.Gx", "12.39.Pn", "12.39.Mk" ], "keywords": [ "final state", "near-threshold enhancement", "belle collaboration", "reconciling", "flatte analysis" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review D", "year": 2007, "month": "Aug", "volume": 76, "number": 3, "pages": "034007" }, "note": { "typesetting": "RevTeX", "pages": 17, "language": "en", "license": "arXiv", "status": "editable", "inspire": 747969, "adsabs": "2007PhRvD..76c4007H" } } }