Large perpendicular magnetic anisotropy of transition metal dimers driven by polarization switching of two-dimensional ferroelectric In2Se3 substrate

TL;DR

This study demonstrates that transition metal dimers on ferroelectric In2Se3 exhibit large perpendicular magnetic anisotropy, which can be tuned by polarization switching, offering potential for atomic-scale magnetic data storage.

Contribution

The paper reveals how polarization reversal in In2Se3 modulates the magnetic anisotropy of transition metal dimers, introducing a novel method for controlling magnetic properties at the atomic scale.

Findings

Co-Os dimer has a magnetic anisotropy energy of ~40 meV.

Os atom contributes up to ~60 meV to MAE.

Polarization switching alters the easy-axis direction of magnetic anisotropy.

Abstract

Large perpendicular magnetic anisotropy (MA) is highly desirable for realizing atomic-scale magnetic data storage which represents the ultimate limit of the density of magnetic recording. In this work, we studied the MA of transition metal dimers Co-Os, Co-Co and Os-Os adsorbed on two-dimensional ferroelectric In2Se3 (In2Se3-CoOs, In2Se3-OsCo, In2Se3-CoCo and In2Se3-OsOs) by first-principles calculations. It is found that the Co-Os dimer in In2Se3-CoOs has large total perpendicular magnetic anisotropy energy (MAE) of ~ 40 meV. In particular, the MAE arising from Os atom is up to ~ 60 meV. The large MAE is attributed to the high spin-orbit coupling constant and the onefold coordination of Os atom. In addition, the MA of the dimers can be tuned by the polarization reversal of In2Se3. When the polarization is upward, the easy-axis directions of MA in In2Se3-OsCo, In2Se3-CoCo and In2Se3-OsOs are all in-plane, while the directions become perpendicular as the polarization is switched to downward. For the In2Se3-CoOs, switching polarization from upward to downward enhance the perpendicular MA from ~ 20 meV to ~ 40 meV. Based on the second-order perturbation theory, we confirm that the exchange splitting of dxy/dx2-y2 and dxz/dyz orbitals as well as the occupation of dz2 orbital at the vicinity of Fermi level play important roles in the changes of MA with the reversal of FE polarization of In2Se3.