Abstract

We investigate the S3 free energy of mathcal{N} = 3 Chern-Simons-matter quiver gauge theories with gauge group U(N)r (r ≥ 2) where the sum of Chern-Simons levels does not vanish, beyond the leading order in the large-N limit. We take two different approaches to explore the sub-leading structures of the free energy. First we evaluate the matrix integral for the partition function in the ’t Hooft limit using a saddle point approximation. Second we use an ideal Fermi-gas model to compute the same partition function, but in the limit of fixed Chern-Simons levels. The resulting expressions for the free energy F = − log Z are then compared in the overlapping parameter regime. The Fermi-gas approach also hints at a universal frac{1}{6} log N correction to the free energy. Since the quiver gauge theories we consider are dual to massive Type IIA theory, we expect the sub-leading correction of the planar free energy in the large ’t Hooft parameter limit to match higher-derivative corrections to the tree-level holographic dual free energy, which have not yet been fully investigated.

Highlights

  • Are compared in the overlapping parameter regime

  • We investigate the S3 free energy of N = 3 Chern-Simons-matter quiver gauge theories with gauge group U(N )r (r ≥ 2) where the sum of Chern-Simons levels does not vanish, beyond the leading order in the large-N limit

  • First we evaluate the matrix integral for the partition function in the ’t Hooft limit using a saddle point approximation

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Summary

Introduction

Are compared in the overlapping parameter regime. The Fermi-gas approach hints at a universal. Since the result is valid even in the strong coupling limit, it can be compared with the holographic dual free energy F = − log Z in the weak curvature limit. This technical development motivates the calculation of supersymmetric partition functions of a wide class of SCFTs with holographic duals. In the strong ’t Hooft coupling limit, the resulting free energy matches the holographic dual free energy at leading order [5], or equivalently the regularized on-shell action of Type IIA string theory in an AdS4 × CP3 background [8, 9]

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