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量子点中偶数个电子的自旋分数化

Spin fractionalization of an even number of electrons in a quantum Dot.

作者信息

Giuliano D, Tagliacozzo A

机构信息

Istituto Nazionale di Fisica della Materia (INFM), Unita di Napoli, Napoli, Italy and Department of Physics, Stanford University, Stanford, California 94305, USA.

出版信息

Phys Rev Lett. 2000 May 15;84(20):4677-80. doi: 10.1103/PhysRevLett.84.4677.

Abstract

We find that Kondo resonant conductance can occur in a quantum dot in the Coulomb blockade regime with an even number of electrons N. The contacts are attached to the dot in a pillar configuration, and a magnetic field B( perpendicular) along the axis is applied. B( perpendicular) lifts the spin degeneracy of the dot energies. Usually, this prevents the system from developing the Kondo effect. Tuning B( perpendicular) to the value B(*) where levels with different total spin cross restores both the degeneracy and the Kondo effect. We analyze a dot charged with N = 2 electrons. Coupling to the contacts is antiferromagnetic due to a spin selection rule and, in the Kondo state, the charge is unchanged while the total spin on the dot is S = 1/2.

摘要

我们发现,在库仑阻塞区中具有偶数个电子N的量子点中会出现近藤共振电导。触点以柱状配置连接到量子点,并施加沿轴方向的磁场B(垂直)。B(垂直)消除了量子点能量的自旋简并性。通常,这会阻止系统产生近藤效应。将B(垂直)调谐到不同总自旋的能级交叉的B(*)值时,简并性和近藤效应都会恢复。我们分析了一个带有N = 2个电子的量子点。由于自旋选择规则,与触点的耦合是反铁磁性的,并且在近藤态中,电荷不变,而量子点上的总自旋为S = 1/2。

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