Evidence for the first-order topological phase transition in a Kitaev spin liquid candidate $\hat{I}\pm$-RuCl${}_3$

Abstract

The Kitaev quantum spin liquid (QSL) on the two-dimensional honeycomb lattice epitomizes an entangled topological state, where the spins fractionalize into Majorana fermions. This state has aroused tremendous interest because it harbors non-Abelian anyon excitations. The half-integer quantized thermal Hall (HIQTH) conductance observed in $\hat{I}\pm$-RuCl${}_3$ is a key signature of these excitations. However, the fate of this topologically nontrivial state at intense fields remains largely elusive. Here, we report the thermal conductivity $\hat{I}º$ and specific heat $C$ of $\hat{I}\pm$-RuCl${}_3$ with in-plane magnetic fields $H$. For the field direction perpendicular to the Ru-Ru bond, where the HIQTH effect is observed, we find a discontinuous jump in $\hat{I}º(H)$ and a peak anomaly in $C(H)$ at $\hat{I}{¼}_0{H}^{\ast }\approx 11$\,T, evidencing a weak first-order phase transition. Remarkably, the HIQTH effect vanishes close to $H^{\ast }$. Furthermore, we find that the spin-fractionalization feature is retained well above $H^{\ast }$. These imply the emergence of the phase transition that separates two QSL phases with distinct topological properties.

6 pages, 4 figures