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This research presents a minimal toy model of strong interactions using qubit-regularized SU(3) lattice gauge theory, successfully demonstrating a continuum limit with massive gauge-invariant excitations. By mapping the system to a three-state quantum clock model, the study identifies a $\mathbb{Z}_3$ parafermion conformal field theory as the ultraviolet fixed point and computes universal mass ratios for relativistic particles in the infrared regime. The work advances theoretical understanding of quantum field theories relevant to high-energy physics and quantum simulation without relying on quarks.
Continuum limit of a qubit-regularized SU(3) lattice gauge theory on a plaquette chain
arXiv:2603.01215v2 Announce Type: replace-cross Abstract: We show that a simple qubit-regularized $\mathrm{SU}(3)$ lattice gauge theory on a plaquette chain admits a continuum limit with massive gauge-invariant excitations, providing a minimal toy model of strong interactions without quarks. By mapping the plaquette-chain Hamiltonian to the three-state quantum clock model in a magnetic field, we demonstrate that the theory can be tuned to a continuum limit governed at short distances by the $\mathbb{Z}_3$ parafermion conformal field theory, which serves as the ultraviolet fixed point. A small relevant magnetic perturbation then drives the system to a massive continuum quantum field theory in the infrared, featuring relativistic particles. In this continuum theory we compute two universal ratios: the mass ratio of the lightest massive particles with opposite charge conjugation, $m^{-}/m^{+} = 1.459(2)$, and $\sqrt{\sigma}/m^{+} = 0.2648(2)$, where $\sigma$ denotes the string tension between a static quark and antiquark.
Abstract:We show that a simple qubit-regularized $\mathrm{SU}(3)$ lattice gauge theory on a plaquette chain admits a continuum limit with massive gauge-invariant excitations, providing a minimal toy model of strong interactions without quarks. By mapping the plaquette-chain Hamiltonian to the three-state quantum clock model in a magnetic field, we demonstrate that the theory can be tuned to a continuum limit governed at short distances by the $\mathbb{Z}_3$ parafermion conformal field theory, which serves as the ultraviolet fixed point. A small relevant magnetic perturbation then drives the system to a massive continuum quantum field theory in the infrared, featuring relativistic particles. In this continuum theory we compute two universal ratios: the mass ratio of the lightest massive particles with opposite charge conjugation, $m^{-}/m^{+} = 1.459(2)$, and $\sqrt{\sigma}/m^{+} = 0.2648(2)$, where $\sigma$ denotes the string tension between a static quark and antiquark.
Accepted for publication in Physical Review D. 7 pages of main text with 5 figures; 25 pages of Supplementary Material
High Energy Physics - Lattice (hep-lat); Strongly Correlated Electrons (cond-mat.str-el); High Energy Physics - Theory (hep-th); Nuclear Theory (nucl-th); Quantum Physics (quant-ph)
arXiv:2603.01215 [hep-lat]
(or arXiv:2603.01215v2 [hep-lat] for this version)
Full text under the publisher's open licence · 189 words
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