Analytic continuation of Spacetime Metrics
Analytic continuation of Spacetime Metrics
Analytic continuation of Spacetime Metrics
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Beyond the Event Horizon<br />
(M′, g′ ab<br />
) is said to be an extension <strong>of</strong> (M, g ab<br />
) if (M, g ab<br />
) can be<br />
isometrically embedded as a proper open subset <strong>of</strong> (M′, g′ ab<br />
)<br />
-Christodoulou proved CC for the spherically symmetric<br />
Einstein-scalar field system->trapped regions. A point in<br />
a trapped region corresponds to a trapped surface in<br />
the 4d space-time manifold<br />
-conditions for predictability for the Einstein equations<br />
are related to the behavior <strong>of</strong> the unique solution <strong>of</strong><br />
the initial value problem on the boundary <strong>of</strong> this<br />
region.<br />
conformal representation <strong>of</strong> the manifold<br />
into 2d Minkowski space<br />
spacetime=future inextendible as a<br />
manifold with continuous Lorentzian metric<br />
-there always exists a maximal region <strong>of</strong> spacetime,<br />
the maximal domain <strong>of</strong> development, for which the<br />
initial value problem uniquely determines the solution.<br />
-consequences <strong>of</strong> curvature singularity at inner horizon: the metric tensor is continuous,<br />
the Riemann tensor diverges at inner horizon<br />
Weak curvature singularity: although curvature diverges, the metric tensor has a welldefined,<br />
continuous, non-singular limit at the singularity (Tipler, 1977)