Fig. 1

Left: dependence of the geodesic ISCO radius rISCO = rms
on the NS angular momentum j and the oblateness factor
.
The shaded area indicates the Kerr-like region where rISCO
decreases with increasing j. We note that for the concrete NS models we
assume here, a fixed value of
corresponds to a fixed NS central density ρ. Moreover, in the limit of
the NS spacetime
approaches the Kerr spacetime and values of
correspond to the highest possible values of ρ (the oblateness
parameter
is also called the Kerr parameter). Right: dependence of compactness
K on
the NS spin frequency νspin and mass M. The shaded area
indicates the region of K < 1 where the ISCO
does not appear above the NS surface.
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