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Are there explicit AdS$_3$ soliton solution?

in the sense of Witten's Anti De Sitter Space And Holography and Hawking-Page transition paper, by doing a $$\tau_E, y ,r \to y, \tau_E ,r$$

from a geometry with a Euclidean time $\tau_E$ cigar space and a compactified $y$ circle

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to a geometry with a $y$ cigar space and a compactified Euclidean time $\tau_E$ circle

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If yes, with a AdS3 soliton solution, what are the form of solutions?

If not, without a AdS3 soliton solution, what are the obstructions?

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1 Answer 1

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There is an explicitly three-dimensional version of a Hawking-Page transition in AdS space. It is given by a transition between an asymptotically $AdS_3$ spacetime and the BTZ (Bañados-Teitelboim-Zanelli) black hole. The line element of thermal (euclidean) $AdS_3$ space is given by

$$ds^2=\left(1+r^2/L^2\right)dt^2+\left(1+r^2/L^2\right)^{-1}dr^2+r^2d\phi^2,$$

where the periodicity of $t$ is given by the inverse temperature and $L$ is the $AdS$ radius. At a temperature that is determined by the point when the compact circles of both geometries match, the system undergoes a phase transition to the BTZ black hole geometry given by

$$ds^2=\left(-M+r^2/L^2\right)dt^2+\left(-M+r^2/L^2\right)^{-1}dr^2+r^2d\phi^2,$$

with $M$ as the mass of the black hole.

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