Abstract

We consider the most general asymptotically anti-de Sitter boundary conditions in three-dimensional Einstein gravity with negative cosmological constant. The metric contains in total twelve independent functions, six of which are interpreted as chemical potentials (or non-normalizable fluctuations) and the other half as canonical boundary charges (or normalizable fluctuations). Their presence modifies the usual Fefferman-Graham expansion. The asymptotic symmetry algebra consists of two sl(2)_k current algebras, the levels of which are given by k=l/(4G_N), where l is the AdS radius and G_N the three-dimensional Newton constant.

Highlights

  • Case the asymptotic symmetry algebra (ASA) consists of two copies of the Virasoro algebra with central charge c = 3l/(2GN ), i.e., the two-dimensional (2D) conformal algebra

  • The asymptotic symmetry algebra consists of two sl(2)k current algebras, the levels of which are given by k = l/(4GN ), where l is the AdS radius and GN the threedimensional Newton constant

  • A few years ago Troessaert constructed more general bc’s for 3D Einstein gravity that involve four state-dependent functions [17]. His ASA consists of two Virasoro and two u(1)k current algebras, which contains the other ASA’s as special cases

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Summary

Boundary conditions in Chern-Simons formulation

Our goal is achieved more in the CS formulation, which is why we start with this formulation.

Notations and conventions
Asymptotic symmetry algebra
Boundary conditions in metric formulation
Generalized Fefferman-Graham gauge
Boundary conditions on the metric
Discussion
Checks
Previous special cases
Brown-Henneaux
Compere-Song-Strominger
Troessaert
Avery-Poojary-Suryanarayana
Loophole to generality
Holographic interpretation
Towards applications and generalizations to other dimensions
Full Text
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