铁磁性
居里温度
材料科学
凝聚态物理
反铁磁性
顺磁性
杂质
磁性
极化子
旋转玻璃
磁性半导体
交换互动
电子
化学
物理
有机化学
量子力学
作者
J. M. D. Coey,M. Venkatesan,C. B. Fitzgerald
出处
期刊:Nature Materials
[Springer Nature]
日期:2005-01-16
卷期号:4 (2): 173-179
被引量:2934
摘要
Dilute ferromagnetic oxides having Curie temperatures far in excess of 300 K and exceptionally large ordered moments per transition-metal cation challenge our understanding of magnetism in solids. These materials are high-k dielectrics with degenerate or thermally activated n-type semiconductivity. Conventional super-exchange or double-exchange interactions cannot produce long-range magnetic order at concentrations of magnetic cations of a few percent. We propose that ferromagnetic exchange here, and in dilute ferromagnetic nitrides, is mediated by shallow donor electrons that form bound magnetic polarons, which overlap to create a spin-split impurity band. The Curie temperature in the mean-field approximation varies as (xdelta)(1/2) where x and delta are the concentrations of magnetic cations and donors, respectively. High Curie temperatures arise only when empty minority-spin or majority-spin d states lie at the Fermi level in the impurity band. The magnetic phase diagram includes regions of semiconducting and metallic ferromagnetism, cluster paramagnetism, spin glass and canted antiferromagnetism.
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