Abstract

The extremal Reissner-Nordstr\"om black hole admits a conformal inversion symmetry, in which the metric is mapped into itself under an inversion of the radial coordinate combined with a conformal rescaling. In the rotating generalization, Couch and Torrence showed that the Kerr-Newman metric no longer exhibits a conformal inversion symmetry, but the radial equation arising in the separation of the massless Klein-Gordon equation admits a mode-dependent inversion symmetry, where the radius of inversion depends upon the energy and azimuthal angular momentum of the mode. It was more recently shown that the static four-charge extremal black holes of STU supergravity (i.e., $\mathcal{N}=2$ supergravity in four dimension coupled to three vector multiplets) admit a generalization of the conformal inversion symmetry, in which the conformally inverted metric is a member of the same four-charge black hole family but with transformed charges. In this paper we study further generalizations of these inversion symmetries, within the general class of extremal STU supergravity black holes. For the rotating black holes, where again the massless Klein-Gordon equation is separable, we show that examples with four electric charges exhibit a generalization of the Couch-Torrence symmetry of the radial equation. Now, as in the conformal inversion of the static specializations, the inversion of the radial equation maps it to the radial equation for a rotating black hole with transformed electric charges. We also study the inversion transformations for the general case of extremal Bogomol'nyi-Prasad-Sommerfield STU black holes carrying eight charges (four electric plus four magnetic), and argue that analogous generalizations of the inversion symmetries exist for both the static and the rotating cases.

Highlights

  • It was observed many years ago that the extremal limit of the Reissner-Nordström black hole exhibits a remarkable conformal inversion symmetry, in which an inversion of the radial coordinate, which maps the near-horizon region to the region near infinity, combined with a conformal rescaling, transforms the original metric back into itself [1]

  • Couch and Torrence showed that the Kerr-Newman metric no longer exhibits a conformal inversion symmetry, but the radial equation arising in the separation of the massless Klein-Gordon equation admits a mode-dependent inversion symmetry, where the radius of inversion depends upon the energy and azimuthal angular momentum of the mode

  • It was more recently shown that the static four-charge extremal black holes of STU supergravity (i.e., N 1⁄4 2 supergravity in four dimension coupled to three vector multiplets) admit a generalization of the conformal inversion symmetry, in which the conformally inverted metric is a member of the same four-charge black hole family but with transformed charges

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Summary

INTRODUCTION

It was observed many years ago that the extremal limit of the Reissner-Nordström black hole exhibits a remarkable conformal inversion symmetry, in which an inversion of the radial coordinate, which maps the near-horizon region to the region near infinity, combined with a conformal rescaling, transforms the original metric back into itself [1]. One purpose of the present paper is to investigate whether the observation of Couch and Torrence that the conformal inversion symmetry of the extremal static Reissner-Nordström metric has a corresponding inversion transformation of the radial equation in the rotating case might generalize to rotating versions of the four-charge extremal black holes in STU supergravity. A simple example that was investigated in [4] was the static extremal Kaluza-Klein dyonic black hole, which in the language of STU supergravity corresponds to the case where just one of the four electromagnetic fields is turned on and carries independent electric and magnetic charges, with the other three electromagnetic fields being zero It was shown in [4] that this metric does not map into any metric within the same family, under conformal inversion. Owing to the greater complexity of the general eight-charge non-BPS extremal solutions, we shall not pursue this question further in the present paper

INVERSION SYMMETRY OF RADIAL EQUATION FOR FOUR-CHARGE ROTATING
Conformal inversion in the static limit
Conformal inversion symmetry for static pairwise-equal dyonic black holes
CONFORMAL INVERSION FOR EIGHT-CHARGE EXTREMAL STATIC STU BLACK HOLES
P2i Q2i : ð4:3Þ
INVERSION SYMMETRY OF RADIAL EQUATION FOR EIGHT-CHARGE ROTATING
CONCLUDING REMARKS
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