English

Free field realisation and the chiral universal centraliser

High Energy Physics - Theory 2023-08-10 v2 Mathematical Physics math.MP Quantum Algebra Representation Theory Symplectic Geometry

Abstract

In the TQFT formalism of Moore-Tachikawa for describing Higgs branches of theories of class S\mathcal{S}, the space associated to the unpunctured sphere in type g\mathfrak{g} is the universal centraliser ZG\mathfrak{Z}_G, where g=Lie(G)\mathfrak{g}=Lie(G). In more physical terms, this space arises as the Coulomb branch of pure N=4\mathcal{N}=4 gauge theory in three dimensions with gauge group Gˇ\check{G}, the Langlands dual. In the analogous formalism for describing chiral algebras of class S\mathcal{S}, the vertex algebra associated to the sphere has been dubbed the \emph{chiral universal centraliser}. In this paper, we construct an open, symplectic embedding from a cover of the Kostant-Toda lattice of type g\mathfrak{g} to the universal centraliser of GG, extending a classic result of Kostant. Using this embedding and some observations on the Poisson algebraic structure of ZG\mathfrak{Z}_G, we propose a free field realisation of the chiral universal centraliser for any simple group GG. We exploit this realisation to develop free field realisations of chiral algebras of class S\mathcal{S} of type a1\mathfrak{a}_1 for theories of genus zero with up to six punctures. These realisations make generalised SS-duality completely manifest, and the generalisation to more than six punctures is conceptually clear, though technically burdensome.

Cite

@article{arxiv.2208.09343,
  title  = {Free field realisation and the chiral universal centraliser},
  author = {Christopher Beem and Sujay Nair},
  journal= {arXiv preprint arXiv:2208.09343},
  year   = {2023}
}

Comments

50 pages, one appendix; v2 corresponds to journal version

R2 v1 2026-06-25T01:49:21.370Z