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Black holes: from event horizons to trapping horizons - LUTH ...

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Concept of black hole and <strong>event</strong> horizon<br />

Drawbacks of the classical definition<br />

not applicable in cosmology, for in general (M , g) is not asymp<strong>to</strong>tically flat<br />

even when applicable, this definition is highly non-local:<br />

Determination of ˙<br />

Moreover this is not locally linked with the notion of strong gravitational field:<br />

[Ashtekar & Krishnan, LRR 7, 10 (2004)]<br />

J − (I + ) requires the knowledge of the entire future null infinity.<br />

Example of <strong>event</strong> horizon in a flat region of<br />

spacetime:<br />

Vaidya metric, describing incoming radiation<br />

<strong>from</strong> infinity:<br />

ds 2 = −<br />

<br />

1 − 2m(v)<br />

<br />

dv 2 + 2dv dr + r 2 (dθ 2 +<br />

r<br />

sin 2 θdϕ 2 )<br />

with m(v) = 0 for v < 0<br />

dm/dv > 0 for 0 ≤ v ≤ v0<br />

m(v) = M0 for v > v0<br />

Eric Gourgoulhon (<strong>LUTH</strong>) <strong>Black</strong> <strong>holes</strong>: <strong>trapping</strong> <strong>horizons</strong> CERN, 17 March 2010 6 / 38

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