Multiferroic magnetic spirals induced by random magnetic exchanges
arXiv:1610.00783 · doi:10.1103/PhysRevX.8.011005
Abstract
Multiferroism can originate from the breaking of inversion symmetry caused by magnetic-spiral order. The usual mechanism for stabilizing a magnetic spiral is competition between magnetic exchange interactions differing by their range and sign, such as nearest-neighbor and next-nearest- neighbor interactions. Since the latter are usually weak the onset temperatures for multiferroism via this mechanism are typically low. By considering a realistic model for YBaCuFeO we propose an alternative mechanism for magnetic-spiral order, and hence for multiferroism, that occurs at much higher temperatures. We show using Monte-Carlo simulations and electronic structure calculations based on density functional theory that the Heisenberg model on a geometrically non-frustrated lattice with only nearest-neighbor interactions can have a spiral phase up to high temperature when frustrating bonds are introduced randomly along a single crystallographic direction as caused, e.g., by a particular type of chemical disorder. This long-range correlated pattern of frustration avoids ferroelectrically inactive spin glass order. Finally, we provide an intuitive explanation for this mechanism and discuss its generalization to other materials.
7 pages, 4 figures and supplemental material (8 pages and 6 figures)
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- Tuning the tilting of the spiral plane by Mn doping in YBaCuFeO5 multiferroic
- Spiral order from orientationally correlated random bonds in classical XY models
- Nature of the spiral state, electric polarisation and magnetic transitions in Sr-doped YBaCuFeO: A first-principles study
- Counterroating incommensurate magnetic order and strong quantum fluctuations in the honeycomb layers of
- Magnetic properties of a highly ordered single crystal of the layered perovskite YBaCuFeMnO
- Weak ferromagnetism linked to the high-temperature spiral phase of YBaCuFeO5