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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

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