Lattice Field Theory Analysis of the Chiral Heisenberg Model

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Auteurs principaux: Hands, Simon, Ostmeyer, Johann
Format: Preprint
Publié: 2026
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author Hands, Simon
Ostmeyer, Johann
author_facet Hands, Simon
Ostmeyer, Johann
contents Motivated by ongoing interest in the universal behaviour of the Hubbard model of spinning electrons on honeycomb and $π$-flux lattices at the semi-metal -- Mott insulator phase transition, we formulate the \threeD~chiral Heisenberg model, a theory of relativistic fermions in three spacetime dimensions, as a lattice field theory using domain wall fermions. The contact interaction term preserves an SU(2) global symmetry. We perform numerical simulations using the Rational Hybrid Monte Carlo algorithm on system sizes $L^3\times L_s$ with $L\in\{8,\ldots,24\}$ and domain wall separation $L_s\in\{8,16,24\}$. We locate the phase transition corresponding to spontaneous SU(2)$\to$U(1) breaking, yielding critical exponent estimates $ν^{-1}=0.63(3)$, $η_Φ=1.42(8)$. These values are considerably removed from estimates obtained from simulations performed in (2+1)D, ie. with the time and spatial directions treated differently, but align more closely with analytic estimates obtained using 3D covariant field theory. We also present first results for the fermion correlator, ultimately needed for the determination of the exponent $η_Ψ$, highlighting the need to rotate the fermion source to a common reference direction in isospace in order to obtain a signal.
format Preprint
id arxiv_https___arxiv_org_abs_2603_29461
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Lattice Field Theory Analysis of the Chiral Heisenberg Model
Hands, Simon
Ostmeyer, Johann
High Energy Physics - Lattice
Strongly Correlated Electrons
High Energy Physics - Theory
Motivated by ongoing interest in the universal behaviour of the Hubbard model of spinning electrons on honeycomb and $π$-flux lattices at the semi-metal -- Mott insulator phase transition, we formulate the \threeD~chiral Heisenberg model, a theory of relativistic fermions in three spacetime dimensions, as a lattice field theory using domain wall fermions. The contact interaction term preserves an SU(2) global symmetry. We perform numerical simulations using the Rational Hybrid Monte Carlo algorithm on system sizes $L^3\times L_s$ with $L\in\{8,\ldots,24\}$ and domain wall separation $L_s\in\{8,16,24\}$. We locate the phase transition corresponding to spontaneous SU(2)$\to$U(1) breaking, yielding critical exponent estimates $ν^{-1}=0.63(3)$, $η_Φ=1.42(8)$. These values are considerably removed from estimates obtained from simulations performed in (2+1)D, ie. with the time and spatial directions treated differently, but align more closely with analytic estimates obtained using 3D covariant field theory. We also present first results for the fermion correlator, ultimately needed for the determination of the exponent $η_Ψ$, highlighting the need to rotate the fermion source to a common reference direction in isospace in order to obtain a signal.
title Lattice Field Theory Analysis of the Chiral Heisenberg Model
topic High Energy Physics - Lattice
Strongly Correlated Electrons
High Energy Physics - Theory
url https://arxiv.org/abs/2603.29461