Control of magnetic properties of materials by an applied electric field, known as magnetoelectric coupling, is interesting for low-power spintronics. There are several known mechanisms responsible for magnetoelectric coupling including intrinsic effects in single-phase materials, strain induced coupling in two-phase composites, and electronically-driven interface magnetoelectric effects.
The latter are especially interesting from the fundamental point of view and applications due to the range of possibilities offered by artificially structured systems and non-trivial physical mechanisms that control the interface magnetoelectric phenomena. In particular, the magnetoelectric coupling may occur at the ferromagnet/insulator interface due to spin-dependent screening, where an applied electric field produces accumulation or depletion of spin-polarized electrons resulting in a change of the interface magnetization. At ferromagnet/ferroelectric interfaces the magnetoelectric effect may also be caused by the interface bonding mechanism, as the result of the change in the overlap between atomic orbitals at the interface induced by ferroelectric switching. The interface magnetoelectric effects may involve magnetic reconstruction, i.e. a change in how magnetic moments are ordered near the interface, leading to a significant change of the interface magnetization. In addition, the field effect may affect the exchange splitting of the spin bands and even induce the interface magnetization on otherwise non-magnetic material.
A relevant magnetoelectric phenomenon is the effect of an applied electric field on the surface (interface) magnetocrystalline anisotropy. The magnetic anisotropy determines the preferential direction of the magnetization in a magnetic thin film and thus affecting the magnetocrystalline anisotropy by may allow switching the magnetic moment which is very interesting for applications. Within these projects we elucidate new physics and explore new possibilities to affect the magnetic properties by electric fields and by ferroelectric polarization.
References
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Change in the minority-spin density at the Fe/BaTiO3 interface with ferroelectric polarization reversal.
Electric-field induced spin density on the Fe (001) surface.
Electric-field induced charge density at the Fe/MgO(001) interface affecting the interface magnetocrystalline anisotropy.
Magnetic reconstruction at the BaTiO3/La0.5Sr0.5MnO3 interface driven by ferroelectric polarization reversal.