Phase diagram of a lattice fermion model with symmetric mass generation

arXiv:2602.18360 · hep-lat, cond-mat.str-el, hep-th · Submitted 2026-02-20 · Read on arXiv

hep-lat, cond-mat.str-el, hep-th

Submitted: 2026-02-20

Updated: 2026-10-11

Comments: Published in Physical Review D; 19 pages, 12 figures, 4 tables

Journal ref: Phys. Rev. D 114, 074504 (2026)

DOI: 10.1103/tjwn-p6jc

License: http://creativecommons.org/licenses/by/4.0/

The gist: We study the phase structure of a model containing two flavors of massless staggered fermions interacting through two independent four-fermion couplings, UI and UB, formulated on a three-dimensional

Terminology

Abstract

We study the phase structure of a model containing two flavors of massless staggered fermions interacting through two independent four-fermion couplings, UI and UB, formulated on a three-dimensional Euclidean space-time lattice. At UB = 0, this model is known to exhibit a direct second-order quantum phase transition between a massless fermion (MF) phase and a phase in which fermions acquire masses through the mechanism commonly referred to as symmetric mass generation (SMG). We demonstrate that introducing a small nonzero value of UB qualitatively alters this structure: the single exotic transition at UB = 0 splits into two distinct, conventional transitions, separated by an intermediate phase in which fermion masses arise through the standard mechanism of spontaneous symmetry breaking (SSB). The first of these is a Gross-Neveu transition separating the MF phase from the SSB-induced massive phase, while the second is a three-dimensional XY transition between the SSB phase and the SMG phase. Using the fermion-bag Monte Carlo method, we verify that the critical exponents associated with both transitions are consistent with the literature, thereby yielding a quantitative characterization of the resulting phase structure of the model.

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