Magnetic quantum dots and magnetic edge states

被引:68
作者
Lee, SJ [1 ]
Souma, S
Ihm, G
Chang, KJ
机构
[1] SUNY Buffalo, Dept Phys, Buffalo, NY 14260 USA
[2] Dongguk Univ, Quantum Funct Semicond Res Ctr, Seoul 100715, South Korea
[3] Chungnam Natl Univ, Dept Phys, Taejon 305764, South Korea
[4] Korea Adv Inst Sci & Technol, Dept Phys, Taejon 305701, South Korea
来源
PHYSICS REPORTS-REVIEW SECTION OF PHYSICS LETTERS | 2004年 / 394卷 / 01期
关键词
two-dimensional electron gases; magnetic edge states; magnetic quantum dots; ballistic transport;
D O I
10.1016/j.physrep.2003.11.004
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Starting with defining the magnetic edge state in a magnetic quantum dot, which becomes quite popular nowadays conjunction with a possible candidate for a high density memory device or spintronic materials, various magnetic nano-quantum structures are reviewed in detail. We study the magnetic edge states of the two dimensional electron gas in strong perpendicular magnetic fields. We find that magnetic edge states are formed along the boundary of the magnetic dot, which is formed by a nonuniform distribution of magnetic fields. These magnetic edge states circulate either clockwise or counterclockwise, depending on the number of missing flux quanta, and exhibit quite different properties, as compared to the conventional ones which are induced by electrostatic confinements in the quantum Hall system. We also find that a close relation between the quantum mechanical eigenstates and the classical trajectories in the magnetic dot. When a magnetic dot is located inside a quantum wire, the edge-channel scattering mechanism by the magnetic quantum dot is very different from that by electrostatic dots. Here, the magnetic dot is formed by two different magnetic fields inside and outside the dot. We study the ballistic edge-channel transport and magnetic edge states in this situation. When the inner field is parallel to the outer one, the two-terminal conductance is quantized and shows the features of a transmission barrier and a resonator. On the other hand, when the inner field-is reversed, the conductance is not quantized and all channels can be completely reflected in some energy ranges. The difference between the above two cases results from the distinct magnetic confinements. We also describe successfully the edge states of magnetic quantum rings and others in detail. (C) 2003 Elsevier B.V. All rights reserved.
引用
收藏
页码:1 / 40
页数:40
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