8 research outputs found

    Back reaction, covariant anomaly and effective action

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    In the presence of back reaction, we first produce the one-loop corrections for the event horizon and Hawking temperature of the Reissner-Nordstr\"om black hole. Then, based on the covariant anomaly cancelation method and the effective action technique, the modified expressions for the fluxes of gauge current and energy momentum tensor, due to the effect of back reaction, are obtained. The results are consistent with the Hawking fluxes of a (1+1)-dimensional blackbody at the temperature with quantum corrections, thus confirming the robustness of the covariant anomaly cancelation method and the effective action technique for black holes with back reaction.Comment: 17 page

    Two Virasoro symmetries in stringy warped AdS3_3

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    41 pages, 1 figureInternational audienceWe study three-dimensional consistent truncations of type IIB supergravity which admit warped AdS3_3 solutions. These theories contain subsectors that have no bulk dynamics. We show that the symplectic form for these theories, when restricted to the non-dynamical subsectors, equals the symplectic form for pure Einstein gravity in AdS3_3. Consequently, for each consistent choice of boundary conditions in AdS3_3, we can define a consistent phase space in warped AdS3_3 with identical conserved charges. This way, we easily obtain a Virasoro X Virasoro asymptotic symmetry algebra in warped AdS3_3; two different types of Virasoro X Kac-Moody symmetries are also consistent alternatives. Next, we study the phase space of these theories when propagating modes are included. We show that, as long as one can define a conserved symplectic form without introducing instabilities, the Virasoro X Virasoro asymptotic symmetries can be extended to the entire (linearized) phase space. This implies that, at least at semi-classical level, consistent theories of gravity in warped AdS3_3 are described by a two-dimensional conformal field theory, as long as stability is not an issue

    The Kerr/CFT correspondence and its extensions

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