Expected properties of Yang–Mills plus Chern–Simons theory

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Let GG be a compact Lie group, let e→?e\to\text{?} be the coupling constant, and let λ∈H4(BG;Z)\lambda\in H^4(BG;\mathbb{Z}) be a nondegenerate level. Let Fe,λF_{e,\lambda} be the Wick-rotated Yang–Mills plus Chern–Simons field theory determined semiclassically by the Lagrangian

Le,λ(A)=14e2FA∧∗FA+Γλ(A).L_{e,\lambda}(A)=\frac{1}{4e^2}F_A\wedge *F_A+\Gamma_\lambda(A).

Write FλF_\lambda for the singular limit as e→∞e\to\infty, F‾λ\overline{F}_\lambda for its projectivization, and αλ\alpha_\lambda for the resulting projectivity (anomaly).

Expected properties of Yang–Mills plus Chern–Simons theory. The following assertions are expected: (1) the Lagrangian determines a family of Wick-rotated field theories; (2) the singular limit e→∞e\to\infty exists and defines a field theory; (3) the projectivization F‾λ\overline{F}_\lambda factors through the bordism category without the Riemannian metric and is therefore a projective topological field theory; and (4) the anomaly extends to a 4-dimensional invertible field theory whose partition function on a closed oriented 4-manifold WW is

α~λ(W)=exp⁡(2πic(λ)24⟨p1(W),[W]⟩),\widetilde{\alpha}_\lambda(W)=\exp\left(\frac{2\pi i c(\lambda)}{24}\langle p_1(W),[W]\rangle\right),

where c(λ)∈Qc(\lambda)\in\mathbb{Q} is the central charge associated to λ\lambda.

These are expectations motivated by the anticipated mass gap and singular long-distance limit of the gapped theory, with evidence from the abelian case; the general assertions are presented as conjectural properties of three-dimensional Yang–Mills plus Chern–Simons theories.

References

Primary source

Daniel S. Freed and Constantin Teleman, “The role of p_1-structures in 3-dimensional Chern-Simons theories”, arXiv:2603.11291 (2026).

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