Abstract

Material realization of the non-Abelian Kitaev spin liquid phase - an example of Ising topological order (ITO) - has been the subject of intense research in recent years. The $4d$ honeycomb Mott insulator $\alpha$-RuCl$_3$ has emerged as a leading candidate, as it enters a field-induced magnetically disordered state where a half-integer quantized thermal Hall conductivity $\kappa_{xy}$ was reported. Further, a recent report of a sign change in the quantized $\kappa_{xy}$ across a certain crystallographic direction is strong evidence for a topological phase transition between two ITOs with opposite Chern numbers. Although this is a fascinating result, independent verification remains elusive, and one may ask if there is a thermodynamic quantity sensitive to the phase transition. Here we propose that the magnetotropic coefficient $k$ under in-plane magnetic fields would serve such a purpose. We report a singular feature in $k$ that indicates a topological phase transition across the $\hat{b}$-axis where ITO is prohibited by a $C_2$ symmetry. If the transition in $\alpha$-RuCl$_3$ is indeed a direct transition between ITOs, then this feature in $k$ should be observable.

Highlights

  • The Kitaev honeycomb model [1] is an important example of an exactly solvable spin-1 2 system displaying topological order

  • The in-plane magnetic field direction is parametrized as h = cos(φ)a + sin(φ)b, and the c∗ component of the torque and the corresponding magnetotropic coefficient k are obtained by differentiating the free energy F with respect to φ, τc∗

  • We propose the magnetotropic coefficient k as a sensitive probe of a direct transition between Ising topological order (ITO), which we expect to appear under in-plane magnetic fields in α-RuCl3 between the zigzag and polarized phases

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Summary

INTRODUCTION

The Kitaev honeycomb model [1] is an important example of an exactly solvable spin-. 1 2 system displaying topological order. The resulting gapped phase exhibits Ising topological order (ITO), which hosts non-Abelian anyon excitations and a chiral edge MF that manifests in a half-integer quantized thermal Remarkable properties of this model have incited a flurry of research into its material realization. A follow-up study [28] reported a varied sign structure in the quantized κxy when the field is rotated in the honeycomb plane, suggesting a topological phase transition between ITOs with opposite Chern number. While this is an exciting development, the thermal transport measurements have been notoriously hard to reproduce, and other interesting probes [29] may be out of reach for some time. This statement is valid so long as the reported intermediate phase is a realization of ITO, independent of the microscopic realization

Ising topological order
MAGNETOTROPIC COEFFICIENT
Continuum Dirac fermion
Kitaev model in a perturbative magnetic field
Magnons in the polarized phase
SUMMARY AND OPEN ISSUES
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