材料科学
正交晶系
铁磁性
反铁磁性
自旋电子学
凝聚态物理
带隙
磁性半导体
基态
磁性
结晶学
晶体结构
光电子学
化学
原子物理学
物理
作者
Yangyang Li,Yakui Weng,Xinmao Yin,Xiaojiang Yu,Sandeep Kumar,Nimer Wehbe,Haijun Wu,Husam N. Alshareef,Stephen J. Pennycook,Mark B. H. Breese,Jingsheng Chen,Shuai Dong,Tom Wu
标识
DOI:10.1002/adfm.201705657
摘要
Abstract Magnetic semiconductors are highly sought in spintronics, which allow not only the control of charge carriers like in traditional electronics, but also the control of spin states. However, almost all known magnetic semiconductors are featured with bandgaps larger than 1 eV, which limits their applications in long‐wavelength regimes. In this work, the discovery of orthorhombic‐structured Ti 2 O 3 films is reported as a unique narrow‐bandgap (≈0.1 eV) ferromagnetic oxide semiconductor. In contrast, the well‐known corundum‐structured Ti 2 O 3 polymorph has an antiferromagnetic ground state. This comprehensive study on epitaxial Ti 2 O 3 thin films reveals strong correlations between structure, electrical, and magnetic properties. The new orthorhombic Ti 2 O 3 polymorph is found to be n‐type with a very high electron concentration, while the bulk‐type trigonal‐structured Ti 2 O 3 is p‐type. More interestingly, in contrast to the antiferromagnetic ground state of trigonal bulk Ti 2 O 3 , unexpected ferromagnetism with a transition temperature well above room temperature is observed in the orthorhombic Ti 2 O 3 , which is confirmed by X‐ray magnetic circular dichroism measurements. Using first‐principles calculations, the ferromagnetism is attributed to a particular type of oxygen vacancies in the orthorhombic Ti 2 O 3 . The room‐temperature ferromagnetism observed in orthorhombic‐structured Ti 2 O 3 , demonstrates a new route toward controlling magnetism in epitaxial oxide films through selective stabilization of polymorph phases.
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