Lorentzian Einstein metrics with prescribed conformal infinity

Abstract

We prove a local well-posedness theorem for the (n+1)-dimensional Einstein equations in Lorentzian signature, with initial data ( g, K) whose asymptotic geometry at infinity is similar to that anti-de Sitter (AdS) space, and compatible boundary data g prescribed at the time-like conformal boundary of space-time. More precisely, we consider an n-dimensional asymptotically hyperbolic Riemannian manifold (M, g) such that the conformally rescaled metric x2 g (with x a boundary defining function) extends to the closure M of M as a metric of class Cn-1 which is also polyhomogeneous of class Cp on M. Likewise we assume that the conformally rescaled symmetric (0,2)-tensor x2K extends to the closure as a tensor field of class Cn-1 which is polyhomogeneous of class Cp-1. We assume that the initial data ( g, K) satisfy the Einstein constraint equations and also that the boundary datum is of class Cp on ∂ M× (-T0,T0) and satisfies a set of natural compatibility conditions with the initial data. We then prove that there exists an integer rn, depending only on the dimension n, such that if p ≥ 2q+rn, with q a positive integer, then there is T>0, depending only on the norms of the initial and boundary data, such that the Einstein equations have a unique (up to a diffeomorphism) solution g on (-T,T)× M with the above initial and boundary data, which is such that x2g is of class Cn-1 and polyhomogeneous of class Cq. Furthermore, if x2 g and x2K are polyhomogeneous of class C∞ and g is in C∞, then x2g is polyhomogeneous of class C∞.

0

Turn this paper into a lesson

ArcXiv compiles a structured reading guide from this paper's metadata: plain-English importance, contributions, prerequisite concepts, which sections to read first, flashcards, and a quiz. Grounded in the abstract, never invented.

Discussion (0)

Sign in to join the discussion.

Loading comments…