{ "id": "nucl-th/9510045", "version": "v1", "published": "1995-10-23T07:28:17.000Z", "updated": "1995-10-23T07:28:17.000Z", "title": "Muons and emissivities of neutrinos in neutron star cores", "authors": [ "O. Elgaroy", "L. Engvik", "E. Osnes", "F. V. De Blasio", "M. Hjorth-Jensen", "G. Lazzari" ], "comment": "14 pages, Revtex style, 3 uuencoded figs included", "journal": "Phys.Rev.Lett. 76 (1996) 1994-1997", "doi": "10.1103/PhysRevLett.76.1994", "categories": [ "nucl-th" ], "abstract": "In this work we consider the role of muons in various URCA processes relevant for neutrino emissions in the core region of neutron stars. The calculations are done for $\\beta$--stable nuclear matter with and without muons. We find muons to appear at densities $\\rho = 0.15$ fm$^{-3}$, slightly around the saturation density for nuclear matter $\\rho_0 =0.16$ fm$^{-3}$. The direct URCA processes for nucleons are forbidden for densities below $\\rho = 0.5$ fm$^{-3}$, however the modified URCA processes with muons $(n+N\\rightarrow p+N +\\mu +\\overline{\\nu}_{\\mu}, p+N+\\mu \\rightarrow n+N+\\nu_{\\mu}$), where $N$ is a nucleon, result in neutrino emissivities comparable to those from $(n+N\\rightarrow p+N +e +\\overline{\\nu}_e, p+N+e \\rightarrow n+N+\\nu_e$). This opens up for further possibilities to explain the rapid cooling of neutrons stars. Superconducting protons reduce however these emissivities at densities below $0.4$ fm$^{-3}$.", "revisions": [ { "version": "v1", "updated": "1995-10-23T07:28:17.000Z" } ], "analyses": { "keywords": [ "neutron star cores", "direct urca processes", "urca processes relevant", "neutrino emissivities", "superconducting protons reduce" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. Lett." }, "note": { "typesetting": "RevTeX", "pages": 14, "language": "en", "license": "arXiv", "status": "editable", "inspire": 401275 } } }