LORENTZIAN EINSTEIN METRICS WITH PRESCRIBED CONFORMAL INFINITY
LORENTZIAN EINSTEIN METRICS WITH PRESCRIBED CONFORMAL INFINITY
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DOI:
10.4310/jdg/1563242472
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发表时间:
2019-07-01
影响因子:
2.5
通讯作者:
Kamran, Niky
中科院分区:
文献类型:
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作者:
Enciso, Alberto;Kamran, Niky
We prove a local well-posedness theorem for the (n + 1)-dimensional Einstein equations in Lorentzian signature, with initial data ((g) over tilde, K) whose asymptotic geometry at infinity is similar to that anti-de Sitter (AdS) space, and compatible boundary data (g) over cap prescribed at the time-like conformal boundary of space-time. More precisely, we consider an n-dimensional asymptotically hyperbolic Riemannian manifold (M, (g) over tilde) such that the conformally rescaled metric x(2)(g) over tilde (with x a boundary defining function) extends to the closure (M) over bar of M as a metric of class Cn-1 ((M) over bar) which is also polyhomogeneous of class C-Polyhom(p)((M) over bar). Likewise we assume that the conformally rescaled symmetric (0, 2)-tensor x(2) K extends to (M) over bar as a tensor field of class Cn-1((M) over bar) which is polyhomogeneous of class C-Polyhom(p-1)((M) over bar). We assume that the initial data ((g) over tilde, K) satisfy the Einstein constraint equations and also that the boundary datum is of class C-P on partial derivative M x (-T-0, T-0) and satisfies a set of natural compatibility conditions with the initial data. We then prove that there exists an integer r(n), depending only on the dimension n, such that if p >= 2q + r(n), 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 (1.1) has a unique (up to a diffeomorphism) solution g on (-T, T) x M with the above initial and boundary data, which is such that x(2)g is an element of Cn-1((-T,T) x (M) over bar) boolean AND C-polyhom(q) ((-T,T) x (M) over bar). Furthermore, if x(2)(g) over tilde, x(2) K are polyhomogeneous of class C infinity and (g) over cap is in C infinity((-T-0,T-0) x partial derivative M), then x(2)g is in C-polyhom(infinity)((-T, T) x (M) over bar).