Three-dimensional $\operatorname{SL}(2,\mathbb R)$ Yang-Mills theory is three-dimensional gravity with background sources
Chern-Simons theory with certain gauge groups is known to be equivalent to a first-order formulation of three-dimensional Einstein gravity with a cosmological constant, where both are purely topological. Here, we extend this correspondence to theories with dynamical degrees of freedom. We show that...
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Main Authors | , , |
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Format | Journal Article |
Language | English |
Published |
26.08.2024
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Subjects | |
Online Access | Get full text |
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Summary: | Chern-Simons theory with certain gauge groups is known to be equivalent to a
first-order formulation of three-dimensional Einstein gravity with a
cosmological constant, where both are purely topological. Here, we extend this
correspondence to theories with dynamical degrees of freedom. We show that
three-dimensional Yang-Mills theory with gauge group
$\operatorname{SL}(2,\mathbb R)$ is equivalent to the first-order formulation
of three-dimensional Einstein gravity with no cosmological constant coupled to
a background stress-energy tensor density (which breaks the diffeomorphism
symmetry). The local degree of freedom of three-dimensional Yang-Mills theory
corresponds to degenerate "gravitational waves" in which the metric is
degenerate and the spin connection is no longer completely determined by the
metric. Turning on a cosmological constant produces the third-way (for
$\Lambda<0$) or the imaginary third-way (for $\Lambda>0$) gauge theories with a
background stress-energy tensor density. |
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DOI: | 10.48550/arxiv.2408.14228 |