Competing Antiferromagnetic-Ferromagnetic States in Kitaev Honeycomb Magnet
arXiv:2006.03724 · doi:10.1103/PhysRevB.102.224411
Abstract
The Kitaev model is a rare example of an analytically solvable and physically instantiable Hamiltonian yielding a topological quantum spin liquid ground state. Here we report signatures of Kitaev spin liquid physics in the honeycomb magnet , built of high-spin () ions, in contrast to the more typical low-spin electron configurations in the presence of large spin-orbit coupling. Neutron powder diffraction measurements, heat capacity, and magnetization studies support the development of a long-range antiferromagnetic order space group of , below = 11 K at = 0 T. The magnetic entropy recovered between = 2 K and 50 K is estimated to be 0.6Rln2, in good agreement with the value expected for systems close to a Kitaev quantum spin liquid state. The temperature-dependent magnetic order parameter demonstrates a value of 0.19(3), consistent with XY anisotropy and in-plane ordering, with Ising-like interactions between layers. Further, we observe a spin-flop driven crossover to ferromagnetic order with space group of under an applied magnetic field of 0.7 T at = 2 K. Magnetic structure analysis demonstrates these magnetic states are competing at finite applied magnetic fields even below the spin-flop transition. Both the compass model, a quantitative comparison of the specific heat of , and related honeycomb cobaltates to the anisotropic Kitaev model further support proximity to a Kitaev spin liquid state. This material demonstrates the rich playground of high-spin systems for spin liquid candidates, and complements known Ir- and Ru-based materials.
arXiv comment16 pages, 8 figures
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