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      Instability in cosmological topologically massive gravity at the chiral point

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          Abstract

          We consider cosmological topologically massive gravity at the chiral point with positive sign of the Einstein-Hilbert term. We demonstrate the presence of a negative energy bulk mode that grows linearly in time. Unless there are physical reasons to discard this mode, this theory is unstable. To address this issue we prove that the mode is not pure gauge and that its negative energy is time-independent and finite. The isometry generators L_0 and \bar{L}_0 have non-unitary matrix representations like in logarithmic CFT. While the new mode obeys boundary conditions that are slightly weaker than the ones by Brown and Henneaux, its fall-off behavior is compatible with spacetime being asymptotically AdS_3. We employ holographic renormalization to show that the variational principle is well-defined. The corresponding Brown-York stress tensor is finite, traceless and conserved. Finally we address possibilities to eliminate the instability and prospects for chiral gravity.

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          The Black Hole in Three Dimensional Space Time

          The standard Einstein-Maxwell equations in 2+1 spacetime dimensions, with a negative cosmological constant, admit a black hole solution. The 2+1 black hole -characterized by mass, angular momentum and charge, defined by flux integrals at infinity- is quite similar to its 3+1 counterpart. Anti-de Sitter space appears as a negative energy state separated by a mass gap from the continuous black hole spectrum. Evaluation of the partition function yields that the entropy is equal to twice the perimeter length of the horizon.
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            Three-dimensional Einstein gravity: Dynamics of flat space

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              A Stress Tensor for Anti-de Sitter Gravity

              We propose a procedure for computing the boundary stress tensor associated with a gravitating system in asymptotically anti-de Sitter space. Our definition is free of ambiguities encountered by previous attempts, and correctly reproduces the masses and angular momenta of various spacetimes. Via the AdS/CFT correspondence, our classical result is interpretable as the expectation value of the stress tensor in a quantum conformal field theory. We demonstrate that the conformal anomalies in two and four dimensions are recovered. The two dimensional stress tensor transforms with a Schwarzian derivative and the expected central charge. We also find a nonzero ground state energy for global AdS_5, and show that it exactly matches the Casimir energy of the dual N=4 super Yang-Mills theory on S^3 x R.
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                Author and article information

                Journal
                19 May 2008
                2009-10-22
                Article
                10.1088/1126-6708/2008/07/134
                0805.2610
                314fbba6-d61c-4dbd-95c9-a79ea870fb18

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                MIT-CTP 3949, UUITP-08/08
                JHEP 0807:134,2008
                19 pages. v3: corrected sign mistake in (4.1) and related equations, v4: corrected e-print number in Ref. [53]
                hep-th gr-qc

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