Abstract

Chern-Simons gravities are theories with a lagrangian given by a Chern-Simons form constructed from a space-time gauge group. In previous investigations we showed that, for some special field configurations that are solutions of the field equations, the extension from Chern-Simons to Transgression forms as lagrangians, motivated by gauge invariance, automatically yields the boundary terms required to regularize the theory, giving finite conserved charges and black hole thermodynamics. Further work by other researchers showed that one of the action functionals considered in the above mentioned work yields a well defined action principle in the metric (zero torsion) case and for asymptotically Anti de Sitter (AdS) space-times. In the present work we consider several action functionals for Chern-Simons AdS gravity constructed from Transgression forms, and show the action principles to be well defined and the Noether charges and Euclidean action to be finite for field configurations satisfying only that the gauge field curvature (field strength) for the AdS gauge group is asymptotically finite. For that purpose we consider an asymptotic expansion of the vielbein and spin connection that may be regarded as a perturbation of an AdS space-time, but allowing a non zero torsion. Our results are of potential interest for Lovelock gravity theories, as it has been shown that the boundary terms dictated by the transgressions for Chern-Simons gravities are also suitable to regularize Lovelock theories.

Highlights

  • Chern-Simons (CS) gravities in 2+1 dimensions were introduced and studied in ref. [1, 2], extended to higher dimensions by Chamseddine in refs. [3, 4] and to the supersymmetric case in refs. [5, 6]

  • In the present work we consider several action functionals for Chern-Simons Anti de Sitter (AdS) gravity constructed from Transgression forms, and show the action principles to be well defined and the Noether charges and Euclidean action to be finite for field configurations satisfying only that the gauge field curvature for the AdS gauge group is asymptotically finite

  • Chern-Simons AdS gravities, which are the subject of the present article, are Chern-Simons gauge theories with the Anti de Sitter (AdS) group as their gauge group

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Summary

Introduction

Chern-Simons (CS) gravities in 2+1 dimensions were introduced and studied in ref. [1, 2], extended to higher dimensions by Chamseddine in refs. [3, 4] and to the supersymmetric case in refs. [5, 6]. [21, 22] it was shown that the extensions of Chern-Simons AdS gravities dictated by the transgressions have the built-in boundary terms that regularize the action, in the sense of giving a finite action, finite Noether conserved charges and the right black hole thermodynamics, unlike what happens in CS theories, where those quantities are infinite unless one regularizes them by hand. We will discuss possible action functionals for Chern-Simons AdS gravity constructed from Transgression forms, along the lines of refs.

Transgressions
Transgression forms and actions
Chern-Simons and Transgression AdS gravity
Asymptotically locally AdS space-times and Fefferman-Graham metric
Conditions on the fields for a finite AdS gauge curvature at the boundary
Goal of this section and the next
Basic ingredients and setup
Action principle
Finite conserved charges
Finiteness of the action
Action principle and boundary conditions II
Examples of configurations in radially simple coordinates
Black holes in arbitrary dimension
Some calculations of Noether’s charges
Mass of Chern-Simons black holes in arbitrary dimension: backgrounds
Mass of Chern-Simons black holes in arbitrary dimension
Mass and angular momentum of rotating BTZ black hole
Discussion and comments
Full Text
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