{ "id": "1103.5516", "version": "v2", "published": "2011-03-29T00:41:29.000Z", "updated": "2011-06-11T02:14:37.000Z", "title": "$J/Ψ$-nuclear bound states", "authors": [ "K. Tsushima", "D. H. Lu", "G. Krein", "A. W. Thomas" ], "comment": "11 pages, 4 figures, 1 table, to appear in Phys. Rev. C. Further comments on the width of J/Psi-nuclear states, effective Lagrangians, and new references", "journal": "Phys.Rev.C83:065208,2011", "doi": "10.1103/PhysRevC.83.065208", "categories": [ "nucl-th", "hep-ex", "hep-lat", "hep-ph", "nucl-ex" ], "abstract": "$J/\\Psi$-nuclear bound state energies are calculated for a range of nuclei by solving the Proca (Klein-Gordon) equation. Critical input for the calculations, namely the medium-modified $D$ and $D^*$ meson masses, as well as the nucleon density distributions in nuclei, are obtained from the quark-meson coupling model. The attractive potential originates from the $D$ and $D^*$ meson loops in the $J/\\Psi$ self-energy in nuclear medium. It appears that $J/\\Psi$-nuclear bound states should produce a clear experimental signature provided that the $J/\\Psi$ meson is produced in recoilless kinematics.", "revisions": [ { "version": "v2", "updated": "2011-06-11T02:14:37.000Z" } ], "analyses": { "subjects": [ "24.85.+p", "13.75.Gx", "14.40.Lb", "21.85.+d" ], "keywords": [ "nuclear bound state energies", "clear experimental signature", "nucleon density distributions", "nuclear medium", "meson loops" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review C", "year": 2011, "month": "Jun", "volume": 83, "number": 6, "pages": "065208" }, "note": { "typesetting": "TeX", "pages": 11, "language": "en", "license": "arXiv", "status": "editable", "inspire": 894368, "adsabs": "2011PhRvC..83f5208T" } } }