Interplay of magnetic field and trigonal distortion in the honeycomb model: Occurrence of a spin-flop phase
arXiv:2204.01600 · doi:10.1103/PhysRevB.105.174435
Abstract
In candidate Kitaev materials, the off-diagonal and interactions are identified to come from the spin-orbit coupling and trigonal distortion, respectively. They have generated intense research efforts because of their intimate relation to the field-induced magnetically disordered state reported in -RuCl. Theoretically, while a plethora of field-induced phases has been proposed in the honeycomb lattice, a stable intermediate phase that can survive in a wide parameter region regardless of the underlying phases is still lacking. Here we focus on the interplay of an out-of-plane magnetic field and a symmetry-allowed term due to trigonal distortion in the dominant antiferromagnetic region. By using multifaceted approaches ranging from classical Monte Carlo and semiclassical spin-wave theory to density-matrix renormalization group, we identify an intriguing spin-flop phase in the presence of magnetic field and antiferromagnetic interaction, before it eventually enters into a fully polarized state. As the interaction approaches the size of one, the - model maps to the easy-axis XXZ antiferromagnet, where the spin-flop phase can be understood as a superfluid phase in the extended Bose-Hubbard model. Our finding thus demonstrates an exciting path from the honeycomb model towards a -symmetric XXZ antiferromagnet in a magnetic field.
15+6 pages, 11+9 figures
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Cited by in corpus (6)
- Spontaneous dimerization, spin-nematic order, and deconfined quantum critical point in a spin-1 Kitaev chain with tunable single-ion anisotropy
- Topological phase transitions and thermal Hall effect in a noncollinear spin texture
- Successive topological phase transitions in two distinct spin-flop phases on the honeycomb lattice
- Interplay of Kitaev Interaction and Off-diagonal Exchanges: Exotic Phases and Quantum Phase Diagrams
- Coexistence of static and dynamic local magnetic fields in an S = 3/2 honeycomb lattice antiferromagnet Co2Te3O8
- Understanding the magnetic interactions of the zig-zag honeycomb lattice: Application to -RuCl