Dynamical Spin Chains in 4D $\mathcal{N}=2$ SCFTs

TL;DR

This paper introduces dynamical spin chains with a quasi-Hopf symmetry algebra for 4d $ abla=2$ SCFTs, revealing new integrable structures and mapping sectors to known models, with solutions verified numerically.

Contribution

It uncovers the first example of dynamical spin chains in 4d $ abla=2$ SCFTs, demonstrating their algebraic structure and mapping to known integrable models.

Findings

Discovered a quasi-Hopf symmetry algebra from the superpotential.

Mapped the holomorphic SU(3) sector to a dynamical 15-vertex model.

Solved the one- and two-magnon problems using Bethe ansatz and confirmed numerically.

Abstract

This is the first in a series of papers devoted to the study of spin chains capturing the spectral problem of 4d $\mathcal{N}=2$ SCFTs in the planar limit. At one loop and in the quantum plane limit, we discover a quasi-Hopf symmetry algebra, defined by the $R$-matrix read off from the superpotential. This implies that when orbifolding the $\mathcal{N}=4$ symmetry algebra down to the $\mathcal{N}=2$ one and then marginaly deforming, the broken generators are not lost, but get upgraded to quantum generators. Importantly, we demonstrate that these chains are dynamical, in the sense that their Hamiltonian depends on a parameter which is dynamically determined along the chain. At one loop we map the holomorphic SU(3) scalar sector to a dynamical 15-vertex model, which corresponds to an RSOS model, whose adjacency graph can be read off from the gauge theory quiver/brane tiling. One scalar SU(2) sub-sector is described by an alternating nearest-neighbour Hamiltonian, while another choice of SU(2) sub-sector leads to a dynamical dilute Temperley-Lieb model. These sectors have a common vacuum state, around which the magnon dispersion relations are naturally uniformised by elliptic functions. Concretely, for the $\mathbb{Z}_2$ quiver theory we study these dynamical chains by solving the one- and two-magnon problems with the coordinate Bethe ansatz approach. We confirm our analytic results by numerical comparison with the explicit diagonalisation of the Hamiltonian for short closed chains.