{ "id": "1909.03236", "version": "v1", "published": "2019-09-07T10:07:39.000Z", "updated": "2019-09-07T10:07:39.000Z", "title": "Generation of strong magnetic fields in old neutron stars accounting for continuous chiral magnetic effect", "authors": [ "Maxim Dvornikov", "V. B. Semikoz", "D. D. Sokoloff" ], "comment": "14 pages in LaTeX2e, JCAP LaTeX style, 6 eps figures", "categories": [ "astro-ph.HE", "hep-ph" ], "abstract": "We suggest a new mean field dynamo model in anomalous MagnetoHydroDynamics (AMHD) accounting for the mean spin (polarization) of the magnetized chiral (ultrarelativistic) plasma of a neutron star (NS). For simplicity we consider a non-superfluid NS with its rigid rotation neglecting also any matter turbulence (convection) within a star. On this way, we recover the Chiral Magnetic Effect (CME) as a possible source for the amplification of a seed, sufficiently strong magnetic field, $B\\sim 10^{13}\\,\\text{G}$, up to values $B\\gtrsim 10^{18}\\,\\text{G}$ in old NS's, having ages $t\\gtrsim 10^6\\,\\text{yr}$. The important issue in AMHD model suggested is the continuous evolution of the chiral imbalance providing the CME for these ages, $\\partial_t\\mu_5 (t)\\neq 0$, in spite of the fast spin-flip in Coulomb collisions in the dense NS plasma that leads to vanishing $\\mu_5\\to 0$ at an earlier epoch in the corresponding protoneutron star. In contrast to the conventional mean-field dynamos, the dynamo drivers in the model are produced due to magnetic field generated at the previous stages of stellar evolution. It makes our model basically nonlinear.", "revisions": [ { "version": "v1", "updated": "2019-09-07T10:07:39.000Z" } ], "analyses": { "keywords": [ "strong magnetic field", "continuous chiral magnetic effect", "old neutron stars accounting", "mean field dynamo model" ], "note": { "typesetting": "LaTeX", "pages": 14, "language": "en", "license": "arXiv", "status": "editable" } } }