Abstract

A recent precise formulation of the hoop conjecture in four spacetime dimensions is that the Birkhoff invariant β\beta (the least maximal length of any sweepout or foliation by circles) of an apparent horizon of energy EE and area AA should satisfy β4πE\beta \le 4 \pi E. This conjecture together with the Cosmic Censorship or Isoperimetric inequality implies that the length \ell of the shortest non-trivial closed geodesic satisfies 2πA\ell^2 \le \pi A. We have tested these conjectures on the horizons of all four-charged rotating black hole solutions of ungauged supergravity theories and find that they always hold. They continue to hold in the the presence of a negative cosmological constant, and for multi-charged rotating solutions in gauged supergravity. Surprisingly, they also hold for the Ernst-Wild static black holes immersed in a magnetic field, which are asymptotic to the Melvin solution. In five spacetime dimensions we define β\beta as the least maximal area of all sweepouts of the horizon by two-dimensional tori, and find in all cases examined that β(g)16π3E \beta(g) \le \frac{16 \pi}{3} E, which we conjecture holds quiet generally for apparent horizons. In even spacetime dimensions D=2N+2D=2N+2, we find that for sweepouts by the product S1×SD4S^1 \times S^{D-4}, β\beta is bounded from above by a certain dimension-dependent multiple of the energy EE. We also find that D2\ell^{D-2} is bounded from above by a certain dimension-dependent multiple of the horizon area AA. Finally, we show that D3\ell^{D-3} is bounded from above by a certain dimension-dependent multiple of the energy, for all Kerr-AdS black holes.Comment: 25 page

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    Last time updated on 11/12/2019