Analytic continuation of Spacetime Metrics
Analytic continuation of Spacetime Metrics
Analytic continuation of Spacetime Metrics
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Black holes overview<br />
-for bodies <strong>of</strong> too large a mass, concentrated in too small a volume, unstoppable collapse<br />
will lead to a singularity in the structure <strong>of</strong> space-time.<br />
-the term ‘singularity’ refers to a region where the conventional classical picture <strong>of</strong> spacetime<br />
breaks down<br />
-standard picture <strong>of</strong> collapse to a BH (Penrose 1978)- the singularities are not visible to<br />
observers at a large distance from the hole, being ‘shielded’ from view by an absolute EH.<br />
solutions <strong>of</strong> the vacuum field equations <strong>of</strong> GR (1915) G mn<br />
= 0<br />
BH types<br />
schwarzschild - 1916 (static, neutral)<br />
reissner-nordstrøm - 1918 (static,<br />
electrically charged)<br />
kerr - 1963 (rotating, neutral)<br />
kerr-newman 1965 (rotating, charged)<br />
all are Petrov type-D space-times<br />
BH mass hidden in (point or ring)<br />
singularity