For very massive fields, a charged black hole with horizon potential Φ_H greater than Q/M can support the stationary scalar cloud that triggers superradiant instability.
Quasinormal Spectrum and Quantization of Charged Black Holes
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abstract
Black-hole quasinormal modes have been the subject of much recent attention, with the hope that these oscillation frequencies may shed some light on the elusive theory of quantum gravity. We study {\it analytically} the asymptotic quasinormal spectrum of a {\it charged} scalar field in the (charged) Reissner-Nordstr\"om spacetime. We find an analytic expression for these black-hole resonances in terms of the black-hole physical parameters: its Bekenstein-Hawking temperature $T_{BH}$, and its electric potential $\Phi$. We discuss the applicability of the results in the context of black-hole quantization. In particular, we show that according to Bohr's correspondence principle, the asymptotic resonance corresponds to a fundamental area unit $\Delta A=4\hbar\ln2$.
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A sufficient condition for the development of superradiant instabilities in charged black-hole spacetimes
For very massive fields, a charged black hole with horizon potential Φ_H greater than Q/M can support the stationary scalar cloud that triggers superradiant instability.