Author:
Toldo Chiara,Willett Brian
Abstract
Abstract
The partition function of a three-dimensional
$$ \mathcal{N}=2 $$
N
=
2
theory on the manifold ℳ
g,p
, an S
1 bundle of degree p over a closed Riemann surface Σ
g
, was recently computed via supersymmetric localization. In this paper, we compute these partition functions at large N in a class of quiver gauge theories with holographic M-theory duals. We provide the supergravity bulk dual having as conformal boundary such three-dimensional circle bundles. These configurations are solutions to
$$ \mathcal{N}=2 $$
N
=
2
minimal gauged supergravity and pertain to the class of Taub-NUT-AdS and Taub-Bolt-AdS preserving 1/4 of the supersymmetries. We discuss the conditions for the uplift of these solutions to M-theory, and compute the on-shell action via holographic renormalization. We show that the uplift condition and on-shell action for the Bolt solutions are correctly reproduced by the large N limit of the partition function of the dual superconformal field theory. In particular, the Σ
g
× S
1 = ℳ
g,0 partition function, which was recently shown to match the entropy of AdS4 black holes, and the S
3 ≅ ℳ0,1 free energy, occur as special cases of our formalism, and we comment on relations between them.
Publisher
Springer Science and Business Media LLC
Subject
Nuclear and High Energy Physics
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