{ "id": "nucl-th/9906016", "version": "v1", "published": "1999-06-07T14:54:47.000Z", "updated": "1999-06-07T14:54:47.000Z", "title": "The properties of \\bar{K} in the nuclear medium", "authors": [ "A. Ramos", "E. Oset" ], "comment": "23 pages, 7 figures, ReVTeX", "journal": "Nucl.Phys. A671 (2000) 481-502", "doi": "10.1016/S0375-9474(99)00846-5", "categories": [ "nucl-th" ], "abstract": "The self-energy of the K^- meson in nuclear matter is calculated in a self-consistent microscopic approach, using a \\bar{K}N interaction obtained from the lowest-order meson-baryon chiral Lagrangian. The effective \\bar{K}N interaction in the medium is derived by solving the coupled-channel Bethe-Salpeter equation including Pauli blocking on the nucleons, mean-field binding potentials for the baryons and the self-energy of the \\pi and \\bar{K} mesons. The incorporation of the self-consistent {\\bar K} self-energy in the description, in addition to the Pauli blocking effects, yields a weaker attractive in-medium {\\bar K}N interaction and a \\Lambda(1405) which dissolves faster with increasing matter density, as a result of the {\\bar K} spectral function being spread out over a wide range of energies. These effects are further magnified when the intermediate pions are dressed.", "revisions": [ { "version": "v1", "updated": "1999-06-07T14:54:47.000Z" } ], "analyses": { "subjects": [ "12.38.Lg", "13.75.Jz", "14.20.Gk", "14.20.Jn", "14.40.Aq", "21.65.+f", "25.80.Nv" ], "keywords": [ "nuclear medium", "lowest-order meson-baryon chiral lagrangian", "properties", "interaction", "self-consistent microscopic approach" ], "tags": [ "journal article" ], "publication": { "publisher": "Elsevier", "journal": "Nucl. Phys. A" }, "note": { "typesetting": "RevTeX", "pages": 23, "language": "en", "license": "arXiv", "status": "editable", "inspire": 501356 } } }