Magnetic proximity effect at the three-dimensional topological insulator/magnetic insulator interface

被引:152
作者
Eremeev, S. V. [1 ,2 ]
Men'shov, V. N. [2 ,3 ]
Tugushev, V. V. [2 ,3 ,4 ]
Echenique, P. M. [5 ,6 ,7 ]
Chulkov, E. V. [2 ,5 ,6 ,7 ]
机构
[1] Inst Strength Phys & Mat Sci, Tomsk 634021, Russia
[2] Tomsk State Univ, Tomsk 634050, Russia
[3] NRC Kurchatov Inst, Moscow 123182, Russia
[4] Prokhorov Gen Phys Inst, Moscow 119991, Russia
[5] Donostia Int Phys Ctr, San Sebastian 20018, Basque Country, Spain
[6] Ctr Fis Mat CFM MPC, Dept Fis Mat UPV EHU, San Sebastian 20080, Basque Country, Spain
[7] Ctr Mixto CSIC UPV EHU, San Sebastian 20080, Basque Country, Spain
来源
PHYSICAL REVIEW B | 2013年 / 88卷 / 14期
关键词
AUGMENTED-WAVE METHOD; DIRAC CONE; SURFACE; METALS; STATES;
D O I
10.1103/PhysRevB.88.144430
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The magnetic proximity effect is a fundamental feature of heterostructures composed of layers of topological insulators and magnetic materials since it underlies many potential applications in devices with novel quantum functionality. Within density functional theory we study magnetic proximity effect at the three-dimensional topological insulator/magnetic insulator (TI/MI) interface in the Bi2Se3/MnSe(111) system as an example. We demonstrate that a gapped ordinary bound state caused by the interface potential arises in the immediate region of the interface. The gapped topological Dirac state also arises in the system owing to relocation to deeper atomic layers of topological insulator. The gap in the Dirac cone originates from an overlapping of the topological and ordinary interfacial states. This result being also corroborated by the analytic model, is a key aspect of the magnetic proximity effect mechanism in the TI/MI structures.
引用
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页数:5
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