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Fig. 1

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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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