Static black hole solutions without rotational symmetry

We construct static black hole solutions that have no rotational symmetry. These arise in theories (including the standard electroweak model) that contain charged vector mesons with mass m≠0. In such theories, a magnetically charged Reissner-Nordström black hole with horizon radius less than a critical value of order ${\mathit{m}}^{\mathrm{-}1}$ is classically unstable against the development of a nonzero vector meson field just outside the horizon, indicating the existence of static black hole solutions with vector meson hair. For the case of unit magnetic charge, spherically symmetric solutions of this type have previously been studied. For other values of the magnetic charge, general arguments show that any new solution with hair cannot be spherically symmetric. In this paper we develop and apply a perturbative scheme (which may have applicability in other contexts) for constructing such solutions in the case where the Reissner-Nordström solution is just barely unstable. For a few low values of the magnetic charge the black holes retain a rotational symmetry about a single axis, but this axial symmetry disappears for higher charges. While the vector meson fields vanish exponentially at distances greater than O(${\mathit{m}}^{\mathrm{-}1}$), the magnetic field and the metric have higher multipole components that decrease only as powers of the distance from the black hole.