Constructing Emergent U(1) Symmetries in the Gamma-prime $\left(\bf \Gamma^{\prime} \right)$ model

TL;DR

This paper systematically constructs classical spin models on various lattices that exhibit emergent continuous U(1) symmetries despite having Hamiltonians with minimal symmetry, revealing insights into symmetry emergence and fluctuation effects.

Contribution

It introduces a family of models demonstrating emergent U(1) symmetry across different lattice geometries with minimal underlying symmetry.

Findings

Emergent U(1) symmetry observed in models on kagome and hyperkagome lattices.

Thermal and quantum fluctuations influence ground state degeneracy via order-by-disorder.

Monte Carlo simulations confirm analytical predictions of thermodynamic behavior.

Abstract

Frustrated magnets can elude the paradigm of conventional symmetry breaking and instead exhibit signatures of emergent symmetries at low temperatures. Such symmetries arise from "accidental" degeneracies within the ground state manifold and have been explored in a number of disparate models, in both two and three dimensions. Here we report the systematic construction of a family of classical spin models that, for a wide variety of lattice geometries with triangular motifs in one, two and three spatial dimensions, such as the kagome or hyperkagome lattices, exhibit an emergent, continuous U(1) symmetry. This is particularly surprising because the underlying Hamiltonian actually has very little symmetry - a bond-directional, off-diagonal exchange model inspired by the microscopics of spin-orbit entangled materials (the $\Gamma^{\prime}$-model). The construction thus allows for a systematic study of the interplay between the emergent continuous U(1) symmetry and the underlying discrete Hamiltonian symmetries in different lattices across different spatial dimensions. We discuss the impact of thermal and quantum fluctuations in lifting the accidental ground state degeneracy via the thermal and quantum order-by-disorder mechanisms, and how spatial dimensionality and lattice symmetries play a crucial role in shaping the physics of the model. Complementary Monte Carlo simulations, for representative one-, two-, and three-dimensional lattice geometries, provide a complete account of the thermodynamics and confirm our analytical expectations.