Abstract
A key result in the proof of black hole uniqueness in 4-dimensions is that a stationary black hole that is “rotating”—i.e., is such that the stationary Killing field is not everywhere normal to the horizon—must be axisymmetric. The proof of this result in 4-dimensions relies on the fact that the orbits of the stationary Killing field on the horizon have the property that they must return to the same null geodesic generator of the horizon after a certain period, P. This latter property follows, in turn, from the fact that the cross-sections of the horizon are two-dimensional spheres. However, in spacetimes of dimension greater than 4, it is no longer true that the orbits of the stationary Killing field on the horizon must return to the same null geodesic generator. In this paper, we prove that, nevertheless, a higher dimensional stationary black hole that is rotating must be axisymmetric. No assumptions are made concerning the topology of the horizon cross-sections other than that they are compact. However, we assume that the horizon is non-degenerate and, as in the 4-dimensional proof, that the spacetime is analytic.
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References
Bunting, G.L.: Proof of the uniqueness conjecture for black holes. Ph.D. Thesis, Univ. of New England, Armidale, N.S.W., 1983
Carter B. (1971). Axisymmetric black hole has only two degrees of freedom. Phys. Rev. Lett. 26: 331–333
Charmousis C. and Gregory R. (2004). Axisymmetric metrics in arbitrary dimensions. Class. Quant. Grav. 21: 527
Chruściel P.T. (1997). On rigidity of analytic black holes. Commun. Math. Phys. 189: 1–7
Chruściel P.T. and Wald R.M. (1994). Maximal hypersurfaces in asymptotically stationary space-times. Commun. Math. Phys. 163: 561
Emparan R. and Reall H.S. (2002). Generalized Weyl solutions. Phys. Rev. D 65: 084025
Emparan R. and Reall H.S. (2002). A rotating black ring in five dimensions. Phys. Rev. Lett. 88: 101101
Friedrich H. (1991). On the global existence and the asymptotic behavior of solutions to the Einstein-Maxwell-Yang-Mills equations. J. Diff. Geom. 34: 275
Friedrich H., Racz I. and Wald R.M. (1999). On the rigidity theorem for spacetimes with a stationary event horizon or a compact Cauchy horizon. Commun. Math. Phys. 204: 691–707
Galloway G.J., Schleich K., Witt D.M. and Woolgar E. (1999). Topological censorship and higher genus black holes. Phys. Rev. D 60: 104039
Galloway G.J., Schleich K., Witt. D. and Woolgar E. (2001). The AdS/CFT correspondence conjecture and topological censorship. Phys. Lett. B 505: 255
Gibbons G.W., Hartnoll S.A. and Pope C.N. (2003). Bohm and Einstein-Sasaki metrics, black holes and cosmological event horizons. Phys. Rev. D 67: 084024
Gibbons G.W., Ida D. and Shiromizu T. (2002). Uniqueness of (dilatonic) charged black holes and black p-branes in higher dimensions. Phys. Rev. D 66: 044010
Gibbons G.W., Ida D. and Shiromizu T. (2002). Uniqueness and non-uniqueness of static black holes in higher dimensions. Phys. Rev. Lett. 89: 041101
Gibbons G.W., Lu H., Page D.N. and Pope C.N. (2004). Rotating black holes in higher dimensions with a cosmological constant. Phys. Rev. Lett. 93: 171102
Harmark T. (2004). Stationary and axisymmetric solutions of higher-dimensional general relativity. Phys. Rev. D 70: 124002
Harmark T. and Olesen P. (2005). Structure of stationary and axisymmetric metrics. Phys. Rev. D 72: 124017
Hawking S.W. (1972). Black holes in general relativity. Commun. Math. Phys. 25: 152–166
Hawking S.W., Ellis G.F.R. (1973). The large scale structure of space-time. Cambridge, Cambridge University Press
Isenberg J. and Moncrief V. (1985). Symmetries of cosmological Cauchy horizons with exceptonal orbits. J. Math. Phys. 26: 1024–1027
Isenberg J. and Moncrief V. (1992). On spacetimes containing Killing vector fields with non-closed orbits. Class. Quantum Grav. 9: 1683–1691
Isenberg, J., Moncrief, V.: Work in progress
Israel W. (1967). Event horizons in static vacuum space-times. Phys. Rev. 164: 1776–1779
Israel W. (1968). Event horizons in electrovac vacuum space-times. Commun. Math. Phys. 8: 245–260
Mazur P.O. (1982). Proof of uniqueness of the Kerr-Newman black hole solution. J. Phys. A 15: 3173–3180
Mishima T. and Iguchi H. (2006). New axisymmetric stationary solutions of five-dimensional vacuum Einstein equations with asymptotic flatness. Phys. Rev. D 73: 044030
Moncrief V. and Isenberg J. (1983). Symmetries of cosmological Cauchy horizons. Commun. Math. Phys. 89: 387–413
Morisawa Y. and Ida D. (2004). A boundary value problem for the five-dimensional stationary rotating black holes. Phys. Rev. D 69: 124005
Müller zum Hagen H. (1990). Characteristic initial value problem for hyperbolic systems of second order differential systems. Ann. Inst. Henri Poincaré 53: 159–216
Myers R.C. and Perry M.J. (1986). Black holes in higher dimensional space-times. Ann. Phys. 172: 304
Nomizu K. (1960). On local and global existence of Killing vector fields. Ann. Math. 72: 105–120
Racz I. (2000). On further generalization of the rigidity theorem for spacetimes with a stationary event horizon or a compact Cauchy horizon. Class. Quant. Grav. 17: 153
Racz I. and Wald R.M. (1992). Extensions of spacetimes with Killing horizons. Class. Quantum Grav. 9: 2643–2656
Racz I. and Wald R.M. (1996). Global extensions of spacetimes describing asymptotic final states of black holes. Class. Quantum Grav. 13: 539–552
Rendall A. (1990). Reduction of the characteristic initial value problem to the Cauchy problem and its application to the Einstein equations. Proc. Roy. Soc. Lond. A 427: 211–239
Robinson D.C. (1975). Uniqueness of the Kerr black hole. Phys. Rev. Lett. 34: 905–906
Rogatko M. (2002). Uniqueness theorem for static black hole solutions of sigma models in higher dimensions. Class. Quant. Grav. 19: L151
Rogatko M. (2003). Uniqueness theorem of static degenerate and non-degenerate charged black holes in higher dimensions. Phys. Rev. D 67: 084025
Rogatko M. (2004). Uniqueness theorem for generalized Maxwell electric and magnetic black holes in higher dimensions. Phys. Rev. D 70: 044023
Rogatko M. (2004). Uniqueness theorem for stationary black hole solutions of sigma-models in five dimensions. Phys. Rev. D 70: 084025
Rogatko M. (2005). Staticity theorem for higher dimensional generalized Einstein-Maxwell system. Phys. Rev. D 71: 024031
Sudarsky D. and Wald R.M. (1992). Extrema of mass, stationarity and staticity, and solutions to the Einstein Yang-Mills equations. Phys. Rev. D 46: 1453–1474
Tomizawa S., Morisawa Y. and Yasui Y. (2006). Vacuum solutions of five dimensional Einstein equations generated by inverse scattering method. Phys. Rev. D 73: 064009
Walters P. (1982). An Introduction to Ergodic Theory. Springer-Verlag, New York
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Hollands, S., Ishibashi, A. & Wald, R.M. A Higher Dimensional Stationary Rotating Black Hole Must be Axisymmetric. Commun. Math. Phys. 271, 699–722 (2007). https://doi.org/10.1007/s00220-007-0216-4
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DOI: https://doi.org/10.1007/s00220-007-0216-4