pith. sign in

arxiv: 1809.00801 · v3 · pith:HSZ5Z72Nnew · submitted 2018-09-04 · ❄️ cond-mat.mtrl-sci

Enhanced perpendicular magnetocrystalline anisotropy energy in an artificial magnetic material with bulk spin-momentum coupling

classification ❄️ cond-mat.mtrl-sci
keywords magneticanisotropybulkenergyperpendicularbreakingcoptpdcoupling
0
0 comments X
read the original abstract

We systematically investigate the perpendicular magnetocrystalline anisotropy (MCA) in Co$-$Pt/Pd-based multilayers. Our magnetic measurement data shows that the asymmetric Co/Pd/Pt multilayer has a significantly larger perpendicular magnetic anisotropy (PMA) energy compared to the symmetric Co/Pt and Co/Pd multilayer samples. We further support this experiment by first principles calculations on the CoPt$_2$, CoPd$_2$, and CoPtPd, which are composite bulk materials that consist of three atomic layers in a unit cell, Pt/Co/Pt, Pd/Co/Pd, Pt/Co/Pd, respectively. By estimating the contribution of bulk spin-momentum coupling to the MCA energy, we show that the CoPtPd multilayer with the symmetry breaking has a significantly larger perpendicular magnetic anisotropy (PMA) energy than the other multilayers that are otherwise similar but lack the symmetry breaking. This observation thus provides an evidence of the PMA enhancement due to the structural inversion symmetry breaking and highlights the asymmetric CoPtPd as the first artificial magnetic material with bulk spin-momentum coupling, which opens a new pathway toward the design of materials with strong PMA.

This paper has not been read by Pith yet.

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Intrinsic origin of interfacial second-order magnetic anisotropy in ferromagnet/normal metal heterostructures

    cond-mat.mtrl-sci 2019-06 unverdicted novelty 6.0

    K2 scales linearly with work-function difference across Pt/Co/X stacks (X = Pd, Cu, Pt, Mo, Ru, W, Ta), indicating inversion asymmetry as the main source of second-order interfacial anisotropy.