Quantum versus thermal fluctuations in the fcc antiferromagnet: alternative routes to order by disorder
arXiv:2011.11621 · doi:10.1103/PhysRevB.102.220405
Abstract
In frustrated magnetic systems with competing interactions fluctuations can lift the residual accidental degeneracy. We argue that the state selection may have different outcomes for quantum and thermal order by disorder. As an example, we consider the semiclassical Heisenberg fcc antiferromagnet with only the nearest-neighbor interactions. Zero-point oscillations select the type 3 collinear antiferromagnetic state at T=0. Thermal fluctuations favor instead the type 1 antiferromagnetic structure. The opposite tendencies result in a finite-temperature transition between the two collinear states. Competition between effects of quantum and thermal order by disorder is a general phenomenon and is also realized in the J1-J2 square-lattice antiferromagnet at the critical point J2 = 0.5 J1.
6 pages, 3 figures (accepted PRB Rapid Comm.)
References in corpus (11)
- Order by disorder and spiral spin liquid in frustrated diamond lattice antiferromagnets
- Quantum order by disorder and accidental soft mode Er2Ti2O7
- Frustrated two dimensional quantum magnets
- Quantum Selection of Order in an Antiferromagnet on a Kagomé Lattice
- Kitaev materials beyond iridates: order by quantum disorder and Weyl magnons in rare-earth double perovskites
- Quantum order by disorder in frustrated diamond lattice antiferromagnets
- Cubic symmetry and magnetic frustration on the spin lattice in KIrCl
- Order-by-disorder near criticality in pyrochlore magnets
- Monte Carlo study of first-order transition in Heisenberg fcc antiferromagnet
- Frustrated antiferromagnets at high fields: the Bose-Einstein condensation in degenerate spectra
- Magnetic excitations in frustrated fcc type-III antiferromagnet MnS