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Global Monopole-BTZ black hole

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Type
Preprint
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Submission Date
Identifiers
arXiv ID: 1408.3008
Source
arXiv
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Abstract

In order to obtain the geometry of a global monopole we introduce the broken $O(2)$ symmetry in $2+1-$dimensions. Adding a negative cosmological constant yields the extension of BTZ black hole in a global monopole background. In the absence of an exact solution and to the first order of approximation the global monopole adds $\frac{1}{r^{2}}$ and $\ln r$ potentials to the metric functions.

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