Gravitational instability of static spherically symmetric Einstein-Gauss-Bonnet black holes in five and six dimensions
arXiv:hep-th/0703074 · doi:10.1103/PhysRevD.76.024012
Abstract
Five and six dimensional static, spherically symmetric, asymptotically Euclidean black holes, are unstable under gravitational perturbations if their mass is lower than a critical value set by the string tension. The instability is due to the Gauss-Bonnet correction to Einstein's equations, and was found in a previous work on linear stability of Einstein-Gauss-Bonnet black holes with constant curvature horizons in arbitrary dimensions. We study the unstable cases and calculate the values of the critical masses. The results are relevant to the issue of black hole production in high energy collisions.
9 pages, 2 figures
References in corpus (1)
Cited by in corpus (11)
- The Lovelock Black Holes
- Lovelock black holes with a nonlinear Maxwell field
- Generalized Vaidya Spacetime in Lovelock Gravity and Thermodynamics on Apparent Horizon
- Exact solutions for the Einstein-Gauss-Bonnet theory in five dimensions: Black holes, wormholes and spacetime horns
- Higher order gravity theories and their black hole solutions
- Stability of higher dimensional Reissner-Nordstrom-anti-de Sitter black holes
- Gravitational instability of simply rotating AdS black holes in higher dimensions
- Stability of Lovelock Black Holes under Tensor Perturbations
- Looking at the Gregory-Laflamme instability through quasi-normal modes
- Evolution of Brane-Localised Standard Model Fields in Gauss-Bonnet theory
- Negative modes of Schwarzschild black hole in Einstein-Gauss-Bonnet Theory