Perturbations of higher-dimensional spacetimes
arXiv:1009.0015 · doi:10.1088/0264-9381/28/3/035011
Abstract
We discuss linearized gravitational perturbations of higher dimensional spacetimes. For algebraically special spacetimes (e.g. Myers-Perry black holes), we show that there exist local gauge invariant quantities linear in the metric perturbation. These are the higher dimensional generalizations of the 4d Newman-Penrose scalars that (in an algebraically special vacuum spacetime) satisfy decoupled equations of motion. We show that decoupling occurs in more than four dimensions if, and only if, the spacetime admits a null geodesic congruence with vanishing expansion, rotation and shear. Decoupling of electromagnetic perturbations occurs under the same conditions. Although these conditions are not satisfied in black hole spacetimes, they are satisfied in the near-horizon geometry of an extreme black hole.
21 pages (v2:Minor corrections, accepted by CQG.)
References in corpus (10)
- Near-horizon symmetries of extremal black holes
- A field-theory motivated approach to symbolic computer algebra
- An instability of higher-dimensional rotating black holes
- A classification of near-horizon geometries of extremal vacuum black holes
- Robinson-Trautman spacetimes in higher dimensions
- Extremal vacuum black holes in higher dimensions
- Generalization of the Geroch-Held-Penrose formalism to higher dimensions
- Type D Einstein spacetimes in higher dimensions
- Ultraspinning instability of rotating black holes
- Kerr-NUT-de Sitter Curvature in All Dimensions