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从反向传播的ν = 1和ν = 1/3态合成ν = 2/3分数量子霍尔效应边缘态。

Synthesizing a ν=2/3 fractional quantum Hall effect edge state from counter-propagating ν=1 and ν=1/3 states.

作者信息

Cohen Yonatan, Ronen Yuval, Yang Wenmin, Banitt Daniel, Park Jinhong, Heiblum Moty, Mirlin Alexander D, Gefen Yuval, Umansky Vladimir

机构信息

Braun Center for Submicron Research, Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot, 76100, Israel.

Department of Physics, Harvard University, Cambridge, MA, 02138, USA.

出版信息

Nat Commun. 2019 Apr 23;10(1):1920. doi: 10.1038/s41467-019-09920-5.

Abstract

Topological edge-reconstruction occurs in hole-conjugate states of the fractional quantum Hall effect. The frequently studied filling factor, ν = 2/3, was originally proposed to harbor two counter-propagating modes: a downstream v = 1 and an upstream v = 1/3. However, charge equilibration between these two modes always led to an observed downstream v = 2/3 charge mode accompanied by an upstream neutral mode. Here, we present an approach to synthetize a v = 2/3 edge mode from its basic counter-propagating charged constituents, allowing a controlled equilibration between the two counter-propagating charge modes. This platform is based on a carefully designed double-quantum-well, which hosts two populated electronic sub-bands (lower and upper), with corresponding filling factors, v and v. By separating the 2D plane to two gated intersecting halves, each with different fillings, counter-propagating chiral modes can be formed along the intersection line. Equilibration between these modes can be controlled with the top gates' voltage and the magnetic field.

摘要

拓扑边缘重构发生在分数量子霍尔效应的空穴共轭态中。经常研究的填充因子ν = 2/3最初被认为包含两种反向传播模式:下游速度v = 1和上游速度v = 1/3。然而,这两种模式之间的电荷平衡总是导致观察到的下游v = 2/3电荷模式伴随着上游中性模式。在这里,我们提出了一种从其基本的反向传播带电成分合成v = 2/3边缘模式的方法,从而实现两种反向传播电荷模式之间的可控平衡。这个平台基于精心设计的双量子阱,它包含两个填充的电子子带(较低和较高),具有相应的填充因子v和v。通过将二维平面分成两个有栅极相交的半平面,每个半平面具有不同的填充,沿交线可以形成反向传播的手性模式。这些模式之间的平衡可以通过顶栅电压和磁场来控制。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f20d/6478935/7ddc408af4af/41467_2019_9920_Fig1_HTML.jpg

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