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Unification of integrability in supersymmetric gauge theories

Kevin Costello, Junya Yagi

TL;DR

This work reveals that a six-dimensional topological--holomorphic theory, subjected to an $\Omega$-deformation, furnishes a common origin for four-dimensional Chern--Simons theory and a wide class of integrable lattice models. By embedding the construction in string theory and applying dualities, the authors unify appearances of the eight-vertex/XYZ models and their variants across supersymmetric gauge theories, via dynamical R-matrices, vertex–face correspondences and L-operators. The framework yields concrete realizations of spin chains (XXX/XXZ/XYZ) through brane tilings, class-S_k theories, and Nekrasov–Shatashvili-type correspondences, and explains the appearance of Q-operators as gauge-theoretic determinants. The results illuminate how topological and holomorphic twists, together with brane dynamics, generate a robust, duality-driven bridge between quantum field theory and integrable systems with rich mathematical structure. The approach provides a platform for exploring open spin chains and higher-genus spectral curves, highlighting the deep role of higher-dimensional gauge dynamics in integrable phenomena.

Abstract

A four-dimensional analog of Chern-Simons theory produces integrable lattice models from Wilson lines and surface operators. We show that this theory describes a quasi-topological sector of maximally supersymmetric Yang-Mills theory in six dimensions, topologically twisted and subjected to an Ω-deformation. By realizing the six-dimensional theory in string theory and applying dualities, we unify various phenomena in which the eight-vertex model and the XYZ spin chain, as well as variants thereof, emerge from supersymmetric gauge theories.

Unification of integrability in supersymmetric gauge theories

TL;DR

This work reveals that a six-dimensional topological--holomorphic theory, subjected to an -deformation, furnishes a common origin for four-dimensional Chern--Simons theory and a wide class of integrable lattice models. By embedding the construction in string theory and applying dualities, the authors unify appearances of the eight-vertex/XYZ models and their variants across supersymmetric gauge theories, via dynamical R-matrices, vertex–face correspondences and L-operators. The framework yields concrete realizations of spin chains (XXX/XXZ/XYZ) through brane tilings, class-S_k theories, and Nekrasov–Shatashvili-type correspondences, and explains the appearance of Q-operators as gauge-theoretic determinants. The results illuminate how topological and holomorphic twists, together with brane dynamics, generate a robust, duality-driven bridge between quantum field theory and integrable systems with rich mathematical structure. The approach provides a platform for exploring open spin chains and higher-genus spectral curves, highlighting the deep role of higher-dimensional gauge dynamics in integrable phenomena.

Abstract

A four-dimensional analog of Chern-Simons theory produces integrable lattice models from Wilson lines and surface operators. We show that this theory describes a quasi-topological sector of maximally supersymmetric Yang-Mills theory in six dimensions, topologically twisted and subjected to an Ω-deformation. By realizing the six-dimensional theory in string theory and applying dualities, we unify various phenomena in which the eight-vertex model and the XYZ spin chain, as well as variants thereof, emerge from supersymmetric gauge theories.

Paper Structure

This paper contains 37 sections, 323 equations, 16 figures, 3 tables.

Figures (16)

  • Figure 1: (a) A lattice formed by line operators on $T^2$. (b) Decomposition of the lattice into square pieces. (c) A single square piece with boundary conditions specified on the corners.
  • Figure 2: (a) A monodromy matrix and (b) a transfer matrix.
  • Figure 3: (a) The unitarity relation and (b) the Yang--Baxter equation.
  • Figure 4: (a) A Dirac string emanating from a monopole. (b) The motion of the monopole creates an 't Hooft operator bounding a surface operator. (c) A surface operator formed by a Dirac string stretched between a monopole--antimonopole pair. Here the antimonopole is represented as a monopole moving in the reverse direction.
  • Figure 5: A lattice of Wilson lines in the presence of surface operators.
  • ...and 11 more figures