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arXiv math-ph/0206045math-phcond-mat.mes-hallmath.MP
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量子Hall哈密顿量的谱流和边缘态能级间距

Spectral flow and level spacing of edge states for quantum Hall hamiltonians

Nicolas Macris

摘要:

我们考虑一个非相对论性粒子在一个圆周为$L$的半无限长圆柱体表面上,该圆柱体受到一个强度为$B$的垂直磁场和最大振幅为$w$的杂质势的作用.该模型在整数量子霍尔效应中具有重要意义。在强磁场或弱无序$B>>w$的状态下,已知存在手征边缘态,这些手征边缘态位于靠近圆柱体边界的几个磁长度内,并沿着圆柱体边界延伸,并且其能级位于体系统的间隙中。这些能级具有在$L$中均匀的谱流,作为沿圆柱体的轴穿过圆柱体的磁通量的函数。通过详细的研究,我们证明了两个连续水平的边缘状态之间的间距是有界的$2παL^{-1}$与$α>0$,独立的$L$,和杂质的配置。这意味着手征边缘态的能级排斥比通常的Anderson模型中的扩展态强得多,并且它们的统计不服从高斯系综。我们的分析使用了两个投影之间的相对指数的概念,并表明,水平排斥连接到量子霍尔系统的拓扑方面。

英文摘要:

We consider a non relativistic particle on the surface of a semi-infinite cylinder of circumference $L$ submitted to a perpendicular magnetic field of strength $B$ and to the potential of impurities of maximal amplitude $w$. This model is of importance in the context of the integer quantum Hall effect. In the regime of strong magnetic field or weak disorder $B>>w$ it is known that there are chiral edge states, which are localised within a few magnetic lengths close to, and extended along the boundary of the cylinder, and whose energy levels lie in the gaps of the bulk system. These energy levels have a spectral flow, uniform in $L$, as a function of a magnetic flux which threads the cylinder along its axis. Through a detailed study of this spectral flow we prove that the spacing between two consecutive levels of edge states is bounded below by $2παL^{-1}$ with $α>0$, independent of $L$, and of the configuration of impurities. This implies that the level repulsion of the chiral edge states is much stronger than that of extended states in the usual Anderson model and their statistics cannot obey one of the Gaussian ensembles. Our analysis uses the notion of relative index between two projections and indicates that the level repulsion is connected to topological aspects of quantum Hall systems.

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