Classical dipoles on the kagome lattice
arXiv:1502.05960 · doi:10.1103/PhysRevB.91.184407
Abstract
Motivated by recent developments in magnetic materials, frustrated nanoarrays and cold atomic systems, we investigate the behaviour of dipolar spins on the frustrated two-dimensional kagome lattice. By combining the Luttinger-Tisza approach, numerical energy minimization, spin-wave analysis and parallel tempering Monte-Carlo, we study long-range ordering and finite-temperature phase transitions for a Hamiltonian containing both dipolar and nearest-neighbor interactions. For both weak and moderate dipolar interactions, the system enters a three-sublattice long-range ordered state, with each triangle having vanishing dipole and quadrupole moments; while for dominating dipolar interactions we uncover ferrimagnetic three-sublattice order. These are also the ground states for XY spins. We discuss excitations of, as well as phase transitions into, these states. We find behaviour consistent with Ising criticality for the 120-degree state, while the ferrimagnetic state appears to be associated with drifting exponents. The celebrated flat band of zero-energy excitations of the kagome nearest-neighbour Heisenberg model is lifted to finite energies but acquires only minimal dispersion as dipolar interactions are added.
9 pages, 8 figures
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Cited by in corpus (6)
- Persistence of the flat band in a kagome magnet with dipolar interactions
- Continuous ground-state degeneracy of classical dipoles on regular lattices
- Zero-energy excitation in the classical kagome antiferromagnet NaBaMnF
- Effects of exchange distortions in the magnetic Kagome lattice
- Molecular dipoles in designer honeycomb lattices
- Magnetic order in the chemically-substituted frustrated antiferromagnet CsCrF