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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)

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