{ "id": "nucl-th/0112034", "version": "v1", "published": "2001-12-12T17:21:53.000Z", "updated": "2001-12-12T17:21:53.000Z", "title": "Asymmetric nuclear matter:the role of the isovector scalar channel", "authors": [ "B. Liu", "V. Greco", "V. Baran", "M. Colonna", "M. Di Toro" ], "comment": "12 pages, 10 Postscript figures", "journal": "Phys.Rev.C65:045201,2002", "doi": "10.1103/PhysRevC.65.045201", "categories": [ "nucl-th" ], "abstract": "We try to single out some qualitative new effects of the coupling to the $\\delta$-isovector-scalar meson introduced in a minimal way in a phenomenological hadronic field theory. Results for the equation of state ($EOS$) and the phase diagram of asymmetric nuclear matter ($ANM$) are discussed. We stress the consistency of the $\\delta$-coupling introduction in a relativistic approach. New contributions to the slope and curvature of the symmetry energy and the neutron-proton effective mass splitting appear particularly interesting. A more repulsive $EOS$ for neutron matter at high baryon densities is expected. Effects on new critical properties of warm $ANM$, mixing of mechanical and chemical instabilities and isospin distillation, are also presented. The $\\delta$ influence is mostly on the {\\it isovectorlike} collective response. The results are largely analytical and this makes the physical meaning quite transparent. Implications for nuclear structure properties of drip-line nuclei and for reaction dynamics with Radioactive Beams are finally pointed out.", "revisions": [ { "version": "v1", "updated": "2001-12-12T17:21:53.000Z" } ], "analyses": { "subjects": [ "21.30.Fe", "21.65.+f", "25.70.Pq", "24.10.Jv" ], "keywords": [ "asymmetric nuclear matter", "isovector scalar channel", "effective mass splitting appear", "splitting appear particularly interesting" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. C" }, "note": { "typesetting": "TeX", "pages": 12, "language": "en", "license": "arXiv", "status": "editable", "inspire": 568236 } } }