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abstract

We study equilibrium conditions between a static, spherically symmetric black hole and classical matter in terms of the radial pressure to density ratio p_r/\rho = w(u), where u is the radial coordinate. It is shown that such an equilibrium is possible in two cases: (i) the well-known case w\to -1 as $u\to u_h (the horizon), i.e., "vacuum" matter, for which \rho(u_h) can be nonzero; (ii) w \to -1/(1+2k) and \rho \sim (u-u_h)^k as u\to u_h, where k>0 is a positive integer (w=-1/3 in the generic case k=1). A non-interacting mixture of these two kinds of matter can also exist. The whole reasoning is local, hence the results do not depend on any global or asymptotic conditions. They mean, in particular, that a static black hole cannot live inside a star with nonnegative pressure and density. As an example, an exact solution for an isotropic fluid with w = -1/3 (that is, a fluid of disordered cosmic strings), with or without vacuum matter, is presented.

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2025 1

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representative citing papers

Naked and truly naked rotating black holes

gr-qc · 2025-01-23 · conditional · novelty 6.0

For rotating stationary axisymmetric horizons, the paper derives expansion conditions on the metric that make the horizon regular, naked, or truly naked in a freely falling frame.

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  • Naked and truly naked rotating black holes gr-qc · 2025-01-23 · conditional · none · ref 10 · internal anchor

    For rotating stationary axisymmetric horizons, the paper derives expansion conditions on the metric that make the horizon regular, naked, or truly naked in a freely falling frame.