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强磁场中未掺杂石墨烯边缘的卢廷格液体

Luttinger liquid at the edge of undoped graphene in a strong magnetic field.

作者信息

Fertig H A, Brey L

机构信息

Department of Physics, Indiana University, Bloomington, Indiana 47405, USA.

出版信息

Phys Rev Lett. 2006 Sep 15;97(11):116805. doi: 10.1103/PhysRevLett.97.116805. Epub 2006 Sep 13.

Abstract

We demonstrate that an undoped two-dimensional carbon plane (graphene) whose bulk is in the integer quantum Hall regime supports a nonchiral Luttinger liquid at an armchair edge. This behavior arises due to the unusual dispersion of the noninteracting edge states, causing a crossing of bands with different valley and spin indices at the edge. We demonstrate that this stabilizes a domain wall structure with a spontaneously ordered phase degree of freedom. This coherent domain wall supports gapless charged excitations, and has a power law tunneling I-V with a nonintegral exponent. In proximity to a bulk lead, the edge may undergo a quantum phase transition between the Luttinger liquid phase and a metallic state.

摘要

我们证明,在整数量子霍尔效应区域的未掺杂二维碳平面(石墨烯)在其扶手椅形边缘处支持一种非手性的卢廷格液体。这种行为源于非相互作用边缘态的异常色散,导致边缘处具有不同谷和自旋指标的能带发生交叉。我们证明,这稳定了一种具有自发有序相自由度的畴壁结构。这种相干畴壁支持无隙带电激发,并且具有非整数指数的幂律隧穿电流-电压关系。在靠近体引线时,边缘可能会在卢廷格液体相和金属态之间经历量子相变。

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