4.6 Article

Topological magnons for thermal Hall transport in frustrated magnets with bond-dependent interactions

Journal

PHYSICAL REVIEW B
Volume 103, Issue 17, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.103.174402

Keywords

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Funding

  1. Natural Sciences and Engineering Research Council of Canada (NSERC)
  2. NSERC Canada Graduate Scholarships-Doctoral (CGS-D)
  3. Ontario Graduate Scholarship
  4. Killam Research Fellowship from the Canada Council for the Arts
  5. Center for Quantum Materials at the University of Toronto

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Thermal transport in topologically-ordered phases provides valuable insights by detecting charge-neutral quasiparticles that do not couple directly to electromagnetic probes. The half-quantized thermal Hall conductivity observed in alpha-RuCl3 under external magnetic fields is evidence of the presence of the non-Abelian Kitaev spin liquid. In the case of tilted magnetic fields, the plateau-like behavior and sign change of the thermal Hall conductivity arise in the partially polarized state.
Thermal transport in topologically-ordered phases of matter provides valuable insights as it can detect the charge-neutral quasiparticles that would not directly couple to electromagnetic probes. An important example is the edge heat transport of the Majorana fermions in a chiral spin liquid, which leads to a half-quantized thermal Hall conductivity. This signature is precisely what has recently been measured in alpha-RuCl3 under external magnetic fields. The plateau-like behavior of the half-quantized thermal Hall conductivity as a function of external magnetic field, and the peculiar sign change depending on the magnetic field orientations, have been proposed to be strong evidence for the non-Abelian Kitaev spin liquid. On the other hand, for in-plane magnetic fields, it has been theoretically shown that such a sign structure can also arise from topological magnons in the field-polarized state. In this paper, we investigate the full implications of topological magnons as heat carriers on thermal transport measurements. We first prove analytically that for any commensurate order with a finite magnetic unit cell, reversing the field direction leads to a sign change in the magnon thermal Hall conductivity in two-dimensional systems. We corroborate this proof numerically with nontrivial magnetic orders as well as the field-polarized state in Kitaev magnets subjected to an in-plane field. In the case of the tilted magnetic field, in which there exists both finite in-plane and out-of-plane field components, we find that the plateau-like behavior of the thermal Hall conductivity and the sign change upon the reversal of the in-plane component of the magnetic field arises in the partially polarized state, as long as the in-plane field contribution to the Zeeman energy is significant. While these results are consistent with the experimental observations, we comment on other aspects that require further investigation in future studies.

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