for
, where
R
is the radius of the surface of the star. Here,
r
is an areal radius and
m
(r) is the mass inside radius
r
. Exterior to the surface of the star, the metric is the standard
Schwarzschild metric as in Eq. (59
) with
. Interior to the surface of the star, the metric is
The boundary conditions are that
m
(0)=0,
is some chosen constant
, and
. The solutions of this equation form a one-parameter family,
parameterized by
which determines how relativistic the system is. A method for
solving these equations in both the areal coordinate
r
and an isotropic radial coordinate
can be found in Ref. [32
].
More generally, isolated neutron stars will be rotating. If the neutron stars are uniformly rotating, then, for any given equation of state, the solutions form a two-parameter family. These models can be parameterized by their central density, which determines how relativistic they are, and by the amount of rotation. If the models are allowed to have differential rotation, then some rotation law must be chosen.
To construct a neutron-star model, the equations for a stationary solution of Einstein's equations outlined in Section 2.4 must be solved self-consistently with the equations for hydrostatic equilibrium of the matter outlined above in Section 4.1 . The equations that must be solved depend on the form of the metric chosen, and numerous formalisms and numerical schemes have been used. An incomplete list of references to work on constructing neutron-star models include [103, 22, 34, 32, 35, 33, 52, 62, 63, 43, 45, 44, 98, 21, 56, 16, 19]. Further review information on neutron-star models can be found in Refs. [97, 51, 50].
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Initial Data for Numerical Relativity
Gregory B. Cook http://www.livingreviews.org/lrr-2000-5 © Max-Planck-Gesellschaft. ISSN 1433-8351 Problems/Comments to livrev@aei-potsdam.mpg.de |