The large-mass limit of cloudy black holes
arXiv:1607.00003 · doi:10.1088/0264-9381/32/13/134002
Abstract
The interplay between black holes and fundamental fields has attracted much attention over the years from both physicists and mathematicians. In this paper we study {\it analytically} a physical system which is composed of massive scalar fields linearly coupled to a rapidly-rotating Kerr black hole. Using simple arguments, we first show that the coupled black-hole-scalar-field system may possess stationary bound-state resonances (stationary scalar `clouds') in the bounded regime , where and are respectively the mass and azimuthal harmonic index of the field, and is the angular velocity of the black-hole horizon. We then show explicitly that these two bounds on the dimensionless ratio can be saturated in the asymptotic limit. In particular, we derive a remarkably simple analytical formula for the resonance mass spectrum of the stationary bound-state scalar clouds in the regime of large field masses: , where is the dimensionless temperature of the rapidly-rotating (near-extremal) black hole, is a constant, and is the resonance parameter. In addition, it is shown that, contrary to the flat-space intuition, the effective lengths of the scalar field configurations in the curved black-hole spacetime approach a {\it finite} asymptotic value in the large mass limit. In particular, we prove that in the large mass limit, the characteristic length scale of the scalar clouds scales linearly with the black-hole temperature.
arXiv comment21 pages. Invited contribution to the Focus Issue on "Black holes and fundamental fields", Classical and Quantum Gravity
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