Abstract

We have investigated the thermal-transport properties of the kagome antiferromagnet Cd-kapellasite (Cd-K). We find that a field suppression effect on the longitudinal thermal conductivity k_xx sets in below ~25 K, suggesting a large spin contribution k_xx^sp in k_xx. We also find clear thermal Hall signals in the spin liquid phase in all Cd-K samples. The magnitude of the thermal Hall conductivity k_xy shows a significant dependence on the sample's scattering time. On the other hand, the temperature dependence of k_xy is similar in all Cd-K samples; k_xy shows a peak at almost the same temperature of the peak of the phonon thermal conductivity k_xy^ph which is estimated by k_xx at 15 T. These results indicate the presence of a dominant phonon thermal Hall k_xy^ph at 15 T. In addition to k_xy^ph, we find that the field dependence of k_xy at low fields turns out to be non-linear at low temperatures, concomitantly with the appearance of the field suppression of k_xx, indicating the presence of a spin thermal Hall k_xy^sp at low fields. Remarkably, by assembling the k_xx dependene of k_xy^sp data of other kagome antiferromagnets, we find that, whereas k_xy^sp stays a constant in the low-k_xx region, k_xy^sp starts to increase as k_xx does in the high-k_xx region. This k_xx dependence of k_xy^sp indicates the presence of both intrinsic and extrinsic mechanisms in the spin thermal Hall effect in kagome antiferromagnets. Furthermore, both k_xy^ph and k_xy^sp disappear in the antiferromagnetic ordered phase at low fields, showing that phonons alone do not exhibit the thermal Hall effect. A high field above ~7 T induces k_xy^ph, concomitantly with a field-induced increase of k_xx and the specific heat, suggesting a coupling of the phonons to the field-induced spin excitations as the origin of k_xy^ph.

Highlights

  • The magnetic ground state of a two-dimensional (2D) kagome structure has been attracting tremendous attention, because the strong frustration effect caused by the cornersharing network of the triangles has been expected to suppress the magnetic order even at absolute zero temperature

  • The largest value of D=J 1⁄4 0.65 is more than 3 times larger than the value of D=J ∼ 0.19 estimated from the deviation of the g factor from 2 [48]. This large mismatch is in sharp contrast to the good agreement found in Ca-K [26] in which both J and D determined by the Schwinger-boson mean-field theory (SBMFT) fit of κxy well coincide with the value estimated from the temperature dependence of χ and that from the deviation of the g factor, respectively. These results indicate that the origin of the thermal Hall effect in Cd-K is different from the spin thermal Hall effect observed in Ca-K [26]

  • 7 T, we find a field-induced increase both in the specific heat and in the thermal Hall effect

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Summary

Introduction

The magnetic ground state of a two-dimensional (2D) kagome structure has been attracting tremendous attention, because the strong frustration effect caused by the cornersharing network of the triangles has been expected to suppress the magnetic order even at absolute zero temperature. A lot of QSLs are theoretically suggested as the ground state of the KHA such as Z2 spin liquids [2,9,10], topological spin liquids [3], Dirac spin liquids [4,6,7,8], and chiral spin liquids [11]. These different QSLs are characterized by different elementary excitations. An experimental challenge to pin down the QSL realized in the KHA by clarifying the elementary excitation

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