Abstract

We consider the effective theory of large D stationary black holes. By solving the Einstein equations with a cosmological constant using the 1/D expansion in near zone of the black hole we obtain the effective equation for the stationary black hole. The effective equation describes the Myers-Perry black hole, bumpy black holes and, possibly, the black ring solution as its solutions. In this effective theory the black hole is represented as an embedded membrane in the background, e.g., Minkowski or Anti-de Sitter spacetime and its mean curvature is given by the surface gravity redshifted by the background gravitational field and the local Lorentz boost. The local Lorentz boost property of the effective equation is observed also in the metric itself. In fact we show that the leading order metric of the Einstein equation in the 1/D expansion is generically regarded as a Lorentz boosted Schwarzschild black hole. We apply this Lorentz boost property of the stationary black hole solution to solve perturbation equations. As a result we obtain an analytic formula for quasinormal modes of the singly rotating Myers-Perry black hole in the 1/D expansion.

Highlights

  • Large D stationary black holesWe study the D dimensional stationary black hole solution and its large D effective theory

  • We study the effective theory of the large D stationary black hole in asymptotically flat or

  • We show that the leading order metric of the Einstein equation in the 1/D expansion is generically regarded as a Lorentz boosted Schwarzschild black hole

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Summary

Large D stationary black holes

We study the D dimensional stationary black hole solution and its large D effective theory. The following analysis is performed in the similar way with static case [9].1. We use the small expansion parameter 1/n where n = D − 3,

Set up
Solving the leading order equation
Effective equation
Ellipsoidal embedding
Boost representation
Perturbation
Schwarzschild black hole
Stationary solution
QNMs of Myers-Perry black hole
QNM frequency
Scalar type perturbation
Summary
A Singly rotating AdS Myers-Perry black hole
B Next-to-leading order analysis
C Spheroidal harmonics at large D
D Detail analysis on the vector type perturbation
F Explicit form of δωS
Full Text
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