材料科学
四方晶系
外延
凝聚态物理
磁各向异性
钴
尖晶石
各向异性
晶体结构
薄膜
格子(音乐)
磁化
结晶学
核磁共振
图层(电子)
纳米技术
磁场
冶金
光学
化学
量子力学
物理
声学
作者
Hiroshige Onoda,Hiroaki Sukegawa,Jun-ichiro Inoue,Hideto Yanagihara
标识
DOI:10.1002/admi.202101034
摘要
Abstract Perpendicular magnetic anisotropy (PMA) energy up to K u = 6.1 ± 0.8 MJm −3 is demonstrated in this study by inducing large lattice distortion exceeding 3% at room temperature in epitaxially distorted cobalt ferrite Co 0.73 Fe 2.18 O 4 (001) thin films. Although the thin film materials include no rare‐earth elements or noble metals, the observed K u is larger than that of the neodymium‐iron‐boron compounds for high‐performance permanent magnets. The large PMA is attributed to the significantly enhanced magneto‐elastic effects, which are pronounced in distorted films with epitaxial lattice structures upon introducing a distortion control layer of composition Mg 2− x Sn 1+ x O 4 . Surprisingly, the induced K u can be quantitatively explained in terms of the agreement between the local crystal field of Co 2+ and the phenomenological magneto‐elastic model, indicating that the linear response of induced K u is sufficiently valid even under lattice distortions as large as 3.2%. Controlling tetragonal lattice deformation using a non‐magnetic spinel layer for ferrites could be a promising protocol for developing materials with large magnetic anisotropies.
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