## 3. Keplerian models of strange starsWe have computed exact numerical models of strange stars in general relativity using the Stergioulas and Friedman (1995) code (see Stergioulas 1998 for a description). In this code, the equilibrium models are obtained following the KEH (Komatsu et al. 1989) method, in which the field equations are converted to integral equations using appropriate Green's functions. The detailed expected properties of strange stars depend on the
adopted theory of interactions. All models presented here were
constructed using Eq. (1) for the equation of state. For our models of
rotating stars, we find that mass and radial quantities (e.g., the
stellar radius and the height of the ISCO above it) accurately scale
as , just as for the static stars,
while the frequencies scale as . For
the more general e.o.s. , we also
confirm the approximate scalings with
In Figs. 1 through 3, we present the mass, radius and the ISCO
frequencies in our Keplerian models, for three values of
, and compare them with the static
models. In Fig. 4 we present the ISCO angular frequencies as a
function of the central energy density of the strange star, and also
exhibit the (larger) angular frequency of the star itself. The maximal
rotation rate of a strange star is very close to the rotation rate of
the maximum-mass model, i.e., 9522 s
Table 1 presents in detail, the various stellar parameters obtained in our calculation for Keplerian strange stars, modeled with Eq. (1) for the value . In addition to the central density, gravitational mass of the star, its radius and maximal rotation rate, the successive columns list the angular frequency () in the co-rotating ISCO (at height above the surface), the height of the retrograde ISCO, the stellar angular momentum, the moment of inertia, the ratio of the polar to equatorial radii, and the polar and the equatorial (forward and backward) redshifts. The ratio of kinetic to potential energy is much larger for these models than for neutron stars. Note that in all cases, the co-rotating ISCO is above the stellar surface and, as exhibited in Fig. 3, the ISCO frequencies are much lower for the Keplerian models than for static models (at fixed stellar mass) and differ considerably from their lowest-order slow-rotation approximation. The significant departure from the slow-rotation result is explained by the unusually large oblateness of rapidly rotating strange stars, and the fact that the ISCO frequency and height depend not only on the angular momentum, but also on the stationary quadrupole moment, in rapidly rotating stars (Shibata and Sasaki, 1998; Sibgatullin and Sunayev, 1998). © European Southern Observatory (ESO) 1999 Online publication: December 2, 1999 |