The rotor Jackiw-Rebbi model: a cold-atom approach to chiral symmetry restoration and quark confinement

TL;DR

This paper introduces the rotor Jackiw-Rebbi model, a (1+1)-D quantum field theory simulated with cold atoms, demonstrating phenomena like chiral symmetry breaking/restoration and quark confinement analogies relevant to high-energy physics.

Contribution

It presents a cold-atom quantum simulation of a (1+1)-D field theory exhibiting chiral symmetry dynamics and confinement, providing a platform to study non-perturbative phenomena.

Findings

Dirac fermions acquire dynamical mass via chiral symmetry breaking

Quantum and thermal fluctuations restore chiral symmetry

Identifies a confinement-deconfinement phase transition with fractionalization

Abstract

Understanding the nature of confinement, as well as its relation with the spontaneous breaking of chiral symmetry, remains one of the long-standing questions in high-energy physics. The difficulty of this task stems from the limitations of current analytical and numerical techniques to address non-perturbative phenomena in non-Abelian gauge theories. In this work, we show how similar phenomena emerge in simpler models, and how these can be further investigated using state-of-the-art cold-atom quantum simulators. More specifically, we introduce the rotor Jackiw-Rebbi model, a (1+1)-dimensional quantum field theory where interactions between Dirac fermions are mediated by quantum rotors. Starting from a mixture of ultracold atoms in an optical lattice, we show how this quantum field theory emerges in the long-wavelength limit. For a wide and experimentally-relevant parameter regime, the Dirac fermions acquire a dynamical mass via the spontaneous breakdown of chiral symmetry. Moreover, we study the effect of both quantum and thermal fluctuations, which lead to the phenomenon of chiral symmetry restoration. Finally, we uncover a confinement-deconfinement quantum phase transition, where meson-like fermions fractionalise into quark-like quasi-particles bound to topological solitons of the rotor field. The proliferation of these solitons at finite chemical potentials again serves to restore the chiral symmetry, yielding a clear analogy with the quark-gluon plasma in quantum chromodynamics, where this symmetry coexists with the deconfined fractional charges. Our results show how the interplay between these phenomena could be analyse in realistic atomic experiments.