State selection in frustrated magnets

TL;DR

This paper explores how quantum fluctuations select specific ground states in frustrated magnets, distinguishing between potential-induced localization ('order by potential') and geometry-induced localization ('order by singularity'), with implications for various magnetic systems.

Contribution

It introduces a unified framework for understanding state selection in frustrated magnets via localization mechanisms on the classical ground-state space, emphasizing the roles of potential and geometry.

Findings

ObS arises from self-intersecting CGSS structures in the Kitaev model.

ObP occurs when quantum fluctuations generate a potential on a simplified CGSS.

Different mechanisms dominate depending on the magnetic model and interactions.

Abstract

Magnets with frustration often show accidental degeneracies, characterized by a large classical ground-state space (CGSS). Quantum fluctuations may `select' one of these ground states -- a phenomenon labeled `order by (quantum) disorder' in literature. In this article, we examine the mechanism(s) by which such state selection takes place. We argue that a magnet, at low energies, maps to a particle moving on the CGSS. State selection corresponds to localization of the particle at a certain point on this space. We distinguish two mechanisms that can bring about localization. In the first, quantum fluctuations generate a potential on the CGSS. If the potential has a deep enough minimum, then the particle localizes in its vicinity. We denote this as `order by potential' (ObP). In the second scenario, the particle localizes at a self-intersection point due to bound-state formation -- a consequence of geometry and quantum interference. Following recent studies by the present authors, we denote this scenario as `order by singularity' (ObS). We place our discussion within the context of the one-dimensional spin-$S$ Kitaev model. We map out its CGSS which grows systematically with increasing system size. It resembles a network where the number of nodes increases exponentially. In addition, the number of wires that cross at each node also grows exponentially. This self-intersecting structure leads to ObS, with the low-energy physics determined by a small subset of the CGSS, consisting of `Cartesian' states. A contrasting picture emerges when an additional XY antiferromagnetic coupling is introduced. The CGSS simplifies dramatically, taking the form of a circle. Spin-wave fluctuations generate a potential on this space, giving rise to state selection by ObP under certain conditions. Apart from contrasting ObS and ObP, we discuss the possibility of ObS in macroscopic magnets.