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Exact Solutions and Scalar Fields in Gravity - Instituto Avanzado de ...

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On maximally symmetric <strong>and</strong> totally geo<strong>de</strong>sic spaces 37<br />

Consequently, the metric (75), allows locally for the locally<br />

maximally symmetric subspace BTZ, but because of the presence<br />

of the factor <strong>in</strong> equation (75) <strong>in</strong> front of this subspace metric, the space<br />

BTZ is not a totally geo<strong>de</strong>sic hypersurface.<br />

On may consi<strong>de</strong>r the BTZ metric as a spatial slice of the W0PC metric<br />

given as<br />

<strong>in</strong> the sense of limit<strong>in</strong>g transition, namely by sett<strong>in</strong>g tends to zero<br />

<strong>in</strong> (77), <strong>in</strong> the slice the metric becomes the metric.<br />

8.1. THE STATIC BTZ SOLUTION AS ANTI–<br />

DE–SITTER METRIC<br />

Consi<strong>de</strong>r the BTZ metric (76), equate <strong>in</strong> it J to zero, <strong>and</strong> replace<br />

by the result<strong>in</strong>g metric is the so called static BTZ:<br />

Accomplish<strong>in</strong>g <strong>in</strong> the above expression the coord<strong>in</strong>ate transformations<br />

one arrives at<br />

The <strong>in</strong>verse transformations are given by<br />

where <strong>and</strong> are restricted to the values

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