Magnetocrystalline anisotropy energy for adatoms and monolayers on non-magnetic substrates: where does it comes from?
arXiv:1308.1597 · doi:10.1088/0953-8984/26/19/196002
Abstract
The substrate contribution to the magnetic anisotropy energy (MAE) of supported nanostructures can be quantified by a site-selective manipulation of the spin-orbit coupling (SOC) and the effective exchange field B_ex. A systematic study of Co adatoms and Co monolayers on the (111) surfaces of Cu, Ag, Au, Pd and Pt is performed to study common trends in this class of materials. It is found that for adatoms, the substrate contribution is relatively small (10-30% of the MAE) while for monolayers, the substrate contribution can be substantial. The contribution from the SOC is much more important than the contribution from the exchange field B_ex, except for highly polarizable substrates with a strong SOC (such as Pt). The substrate always promotes the tendency to an out-of-plane orientation of the easy magnetic axis for all the investigated systems.
9 pages, 2 figures, 13 tables
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Cited by in corpus (6)
- Magnetocrystalline anisotropy of FePt: a detailed view
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- Spatial decomposition of magnetic anisotropy in magnets: application for doped Fe16N2
- Illustrative view on the magnetocrystalline anisotropy of adatoms and monolayers
- Influence of spin-orbit coupling on the magnetic dipole term
- Assessing different approaches to ab initio calculations of spin wave stiffness