Fe contribution to the magnetic anisotropy of $L{1}_0$-ordered FePt thin films studied by angle-dependent x-ray magnetic circular dichroism

Abstract

Among magnetic thin films with perpendicular magnetic anisotropy (PMA), $L{1}_0$-ordered FePt has attracted significant attention because of its exceptionally strong PMA. However, the microscopic origin of its strong PMA has not been elucidated experimentally. We have investigated the contribution of the Fe $3d$ electrons to its magnetic anisotropy energy by angle-dependent x-ray magnetic circular dichroism at the Fe $L_{2,3}$ edge. By this technique, one can deduce the magnetic dipole moment $m_{\text{T}}$, which represents the anisotropic spatial distribution of spin-polarized electrons, and the orbital moment anisotropy (OMA) of Fe $3d$ electrons. Detected finite $m_{\text{T}}$ indicates that the spin-polarized Fe $3d$ electrons are distributed preferentially in the out-of-plane direction of the films. This $m_{\text{T}}$ of Fe overwhelms the positive contribution of OMA to PMA, and reduces the PMA of $L{1}_0$-ordered FePt thin films, consistent with a previous first-principles calculation. The present result implies that a large positive contribution of the non-magnetic element Pt rather than Fe governs the PMA of $L{1}_0$-ordered FePt thin films.

17 pages, 4 figures, 2 supplementary figures

References in corpus (4)

• Anisotropic spin-density distribution and magnetic anisotropy of strained La${}_{1-x}$Sr${}_x$MnO${}_3$ thin films: Angle-dependent x-ray magnetic circular dichroism
• Anisotropic spin distribution and perpendicular magnetic anisotropy in the layered ferromagnetic semiconductor (Ba,K)(Zn,Mn)${}_2$As${}_2$
• Large Orbital Magnetic Moment and Strong Perpendicular Magnetic Anisotropy in Heavily Intercalated Fe${}_x$TiS${}_2$
• Reduced magnetocrystalline anisotropy of CoFe${}_2$O${}_4$ thin films studied by angle-dependent x-ray magnetic circular dichroism