English

Z_2-vortex lattice in the ground state of the triangular Kitaev-Heisenberg model

Strongly Correlated Electrons 2016-03-22 v3

Abstract

The triangular-lattice Heisenberg antiferromagnet (HAF) is known to carry topological Z_2 vortex excitations which form a gas at finite temperatures. Here we show that the spin-orbit interaction, introduced via a Kitaev term in the exchange Hamiltonian, condenses these vortices into a triangular Z2Z_2 vortex crystal at zero temperature. The cores of the Z_2 vortices show abrupt, soliton-like magnetization modulations and arise by a special intertwining of three honeycomb superstructures of ferromagnetic domains, one for each of the three sublattices of the 120-degree state of the pure HAF. This is a new example of a nucleation transition, analogous to the spontaneous formation of magnetic domains, Abrikosov vortices in type-II syperconductors, blue phases in cholesteric liquid crystals, and skyrmions in chiral helimagnets. As the mechanism relies on the interplay of geometric frustration and spin-orbital anisotropies, such vortex mesophases can materialize as a ground-state property in spin-orbit coupled correlated systems with nearly hexagonal topology, as in triangular or strongly frustrated honeycomb iridates.

Keywords

Cite

@article{arxiv.1209.5895,
  title  = {Z_2-vortex lattice in the ground state of the triangular Kitaev-Heisenberg model},
  author = {Ioannis Rousochatzakis and Ulrich K. Rössler and Jeroen van den Brink and Maria Daghofer},
  journal= {arXiv preprint arXiv:1209.5895},
  year   = {2016}
}