Neutron star equilibrium configurations within a fully relativistic theory with strong, weak, electromagnetic, and gravitational interactions

被引:71
|
作者
Belvedere, Riccardo [1 ,2 ,3 ]
Pugliese, Daniela [1 ,2 ,5 ]
Rueda, Jorge A. [1 ,2 ,3 ]
Ruffini, Remo [1 ,2 ,3 ,4 ]
Xue, She-Sheng [1 ,2 ,3 ]
机构
[1] Univ Roma La Sapienza, Dipartimento Fis, I-00185 Rome, Italy
[2] Univ Roma La Sapienza, ICRA, I-00185 Rome, Italy
[3] ICRANet, I-65122 Pescara, Italy
[4] Univ Nice Sophia Antipolis, ICRANet, F-06103 Nice 2, France
[5] Queen Mary Univ London, Sch Math Sci, London E1 4NS, England
关键词
Neutron stars; Nuclear matter equation of state; General relativity; MEAN-FIELD-THEORY; NUCLEAR SYMMETRY ENERGY; THOMAS-FERMI MODEL; MATTER; STABILITY; DENSITY;
D O I
10.1016/j.nuclphysa.2012.02.018
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
We formulate the equations of equilibrium of neutron stars taking into account strong, weak, electromagnetic, and gravitational interactions within the framework of general relativity. The nuclear interactions are described by the exchange of the sigma, omega, and rho virtual mesons. The equilibrium conditions are given by our recently developed theoretical framework based on the Einstein-Maxwell-Thomas-Fermi equations along with the constancy of the general relativistic Fermi energies of particles, the "Klein potentials", throughout the configuration. The equations are solved numerically in the case of zero temperatures and for selected parameterizations of the nuclear models. The solutions lead to a new structure of the star: a positively charged core at supranuclear densities surrounded by an electronic distribution of thickness similar to(h) over bar/(m(e)c) similar to 10(2)(h) over bar/(m(pi)c) of opposite charge, as well as a neutral crust at lower densities. Inside the core there is a Coulomb potential well of depth similar to m(pi)c(2)/e. The constancy of the Klein potentials in the transition from the core to the crust, imposes the presence of an overcritical electric field similar to(m(pi)/m(e))E-2(c), the critical field being E-c = m(e)(2)c(3)/(e (h) over bar). The electron chemical potential and the density decrease, in the boundary interface, until values mu(crust)(e) < mu(core)(e) and rho(crust) < rho(core). For each central density, an entire family of core crust interface boundaries and, correspondingly, an entire family of crusts with different mass and thickness, exist. The configuration with rho(crust) = rho(drip) similar to 4.3 x 10(11) gcm(-3) separates neutron stars with and without inner crust. We present here the novel neutron star mass radius for the especial case rho(crust) = rho(drip) and compare and contrast it with the one obtained from the traditional Tolman-Oppenheimer-Volkoff treatment. (C) 2012 Elsevier B.V. All rights reserved.
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页码:1 / 24
页数:24
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