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Analytic continuation of Spacetime Metrics

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Cross-section <strong>of</strong> a Kerr black hole<br />

Event horizon at (∆=0) and angular momentum between<br />

0≤a all stationary BH solutions <strong>of</strong> Einstein-Maxwell equations are uniquely<br />

determined by 3 parameters: M, Q, and J with<br />

for extreme BH.<br />

-solutions for which have no EH; exposed singularities (naked)<br />

-subsitute<br />

solution.<br />

->Kerr-Newman metric. for a=0 ->Reissner-Nordstrom

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