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The 3d $A$-model and generalised symmetries, Part I: bosonic Chern-Simons theories

Cyril Closset, Elias Furrer, Adam Keyes, Osama Khlaif

TL;DR

The paper develops a systematic framework to study generalized 3d $\mathcal N=2$ gauge theories using the 3d $A$-model, focusing on one-form symmetry gauging and pure Chern–Simons dynamics for simple groups. It constructs Seifert fibering operators for $G_K=(\widetilde G/\Gamma)_K$ theories and proves that, for bosonic gaugings, the SUSY partition functions on Seifert manifolds match the 3d TQFT results up to a framing counterterm proportional to the WZW central charge, confirming a deep link between the 2d $A$-model and infrared TQFT data. The work develops an explicit anyon-condensation (condensing abelian bosons) perspective, showing how the torus Hilbert space and modular data descend to the gauged theory via orbit sums and orbifold-flux sums, with detailed treatment for SU$(N)$ cases. It further extends the analysis to supersymmetric Chern–Simons theories with gauged one-form symmetry, defining the GK Seifert fibering operator as an orbit-averaged object $\mathcal{G}^G_{q,p}(\hat{\omega})$ and providing concrete partition-function formulas on Seifert manifolds, lens spaces, and torus bundles, validated against known TQFT results. The results illuminate the interplay between 2d $\,A$-model topology, 3d CS TQFT, and generalized symmetries, and lay groundwork for future exploration of spin-TQFTs and non-invertible symmetries.

Abstract

The 3d $A$-model is a two-dimensional approach to the computation of supersymmetric observables of three-dimensional $\mathcal{N}=2$ supersymmetric gauge theories. In principle, it allows us to compute half-BPS partition functions on any compact Seifert three-manifold (as well as of expectation values of half-BPS lines thereon), but previous results focussed on the case where the gauge group $\widetilde G$ is a product of simply-connected and/or unitary gauge groups. We are interested in the more general case of a compact gauge group $G=\widetilde G/Γ$, which is obtained from the $\widetilde G$ theory by gauging a discrete one-form symmetry. In this paper, we discuss in detail the case of pure $\mathcal{N}=2$ Chern-Simons theories (without matter) for simple groups $G$. When $G=\widetilde G$ is simply-connected, we demonstrate the exact matching between the supersymmetric approach in terms of Seifert fibering operators and the 3d TQFT approach based on topological surgery in the infrared Chern-Simons theory $\widetilde G_k$, including through the identification of subtle counterterms that relate the two approaches. We then extend this discussion to the case where the Chern-Simons theory $G_k$ can be obtained from $\widetilde G_k$ by the condensation of abelian anyons which are bosonic. Along the way, we revisit the 3d $A$-model formalism by emphasising its 2d TQFT underpinning.

The 3d $A$-model and generalised symmetries, Part I: bosonic Chern-Simons theories

TL;DR

The paper develops a systematic framework to study generalized 3d gauge theories using the 3d -model, focusing on one-form symmetry gauging and pure Chern–Simons dynamics for simple groups. It constructs Seifert fibering operators for theories and proves that, for bosonic gaugings, the SUSY partition functions on Seifert manifolds match the 3d TQFT results up to a framing counterterm proportional to the WZW central charge, confirming a deep link between the 2d -model and infrared TQFT data. The work develops an explicit anyon-condensation (condensing abelian bosons) perspective, showing how the torus Hilbert space and modular data descend to the gauged theory via orbit sums and orbifold-flux sums, with detailed treatment for SU cases. It further extends the analysis to supersymmetric Chern–Simons theories with gauged one-form symmetry, defining the GK Seifert fibering operator as an orbit-averaged object and providing concrete partition-function formulas on Seifert manifolds, lens spaces, and torus bundles, validated against known TQFT results. The results illuminate the interplay between 2d -model topology, 3d CS TQFT, and generalized symmetries, and lay groundwork for future exploration of spin-TQFTs and non-invertible symmetries.

Abstract

The 3d -model is a two-dimensional approach to the computation of supersymmetric observables of three-dimensional supersymmetric gauge theories. In principle, it allows us to compute half-BPS partition functions on any compact Seifert three-manifold (as well as of expectation values of half-BPS lines thereon), but previous results focussed on the case where the gauge group is a product of simply-connected and/or unitary gauge groups. We are interested in the more general case of a compact gauge group , which is obtained from the theory by gauging a discrete one-form symmetry. In this paper, we discuss in detail the case of pure Chern-Simons theories (without matter) for simple groups . When is simply-connected, we demonstrate the exact matching between the supersymmetric approach in terms of Seifert fibering operators and the 3d TQFT approach based on topological surgery in the infrared Chern-Simons theory , including through the identification of subtle counterterms that relate the two approaches. We then extend this discussion to the case where the Chern-Simons theory can be obtained from by the condensation of abelian anyons which are bosonic. Along the way, we revisit the 3d -model formalism by emphasising its 2d TQFT underpinning.
Paper Structure (42 sections, 309 equations, 2 tables)