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arXiv:1612.04489math.AP

Non-linear stability of the Kerr-Newman-de Sitter family of charged black holes

Peter Hintz

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Abstract

We prove the global non-linear stability, without symmetry assumptions, of slowly rotating charged black holes in de Sitter spacetimes in the context of the initial value problem for the Einstein-Maxwell equations: If one perturbs the initial data of a slowly rotating Kerr-Newman-de Sitter (KNdS) black hole, then in a neighborhood of the exterior region of the black hole, the metric and the electromagnetic field decay exponentially fast to their values for a possibly different member of the KNdS family. This is a continuation of recent work of the author with Vasy on the stability of the Kerr-de Sitter family for the Einstein vacuum equations. Our non-linear iteration scheme automatically finds the final black hole parameters as well as the gauge in which the global solution exists; we work in a generalized wave coordinate/Lorenz gauge, with gauge source functions lying in a suitable finite-dimensional space. We include a self-contained proof of the linear mode stability of Reissner-Nordström-de Sitter black holes, building on work by Kodama-Ishibashi. In the course of our non-linear stability argument, we also obtain the first proof of the linear (mode) stability of slowly rotating KNdS black holes using robust perturbative techniques.

arXiv comments
112 pages, 8 figures. v2 is the published version, with typos corrected
Journal reference
Annals of PDE, 4(1):11, Apr 2018
DOI
doi:10.1007/s40818-018-0047-y
Subjects
math.APAnalysis of PDEs gr-qcGeneral Relativity and Quantum Cosmology math-phMathematical Physics math.DGDifferential Geometry

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    • > where do we get a black hole to poke As qubex suggests, this is really about confirming that asymptotically Schwarzschild spacetime (and its close relatives) is mathematically robust [1]. Asymptotically here means that if we perturb (gravitationally or electromagnetically) a…

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