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Spectral gaps of quantum Hall systems with interactions

机译:具有相互作用的量子霍尔系统的谱隙

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A two-dimensional quantum Hall system without disorder for a wide class of interactions including any two-body interaction with finite range is studied by using the Lieb-Schultz-Mattis method [Ann. Phys. (N. Y.) 16:407 (1961)]. The model is defined on an infinitely long strip with a fixed, large width, and the Hilbert space is restricted to the lowest (n(max) + 1) Landau levels with a large integer, n(max). We prove that, for a noninteger filling nu of the Landau levels, either (i) there is a symmetry breaking at zero temperature or (ii) there is only one infinite-volume ground state with a gapless excitation. We also prove the following two theorems: (a) If a pure infinite-volume ground slate has a nonzero excitation gap for a noninteger filling nu, then a translational symmetry breaking occurs at zero temperature. (b) Suppose that there is no non-translationally invariant infinite-volume ground state. Then, if a pure infinite-volume ground state has a nonzero excitation gap, the filling factor nu must be equal to a rational number. Here the ground state is allowed to have a periodic structure which is a consequence of the translational symmetry breaking. We also discuss the relation between our results and the quantized Hall conductance, and phenomenologically explain why odd denominators of filling fractions nu giving the quantized Hall conductance are favored exclusively. [References: 53]
机译:使用Lieb-Schultz-Mattis方法研究了无杂乱的二维量子霍尔系统,该系统对包括相互作用有限范围内的任何两体在内的各种相互作用均无干扰。物理(N.Y.)16:407(1961)]。该模型在具有固定且较大宽度的无限长条带上定义,并且希尔伯特空间限于具有大整数n(max)的最低(n(max)+1)Landau级别。我们证明,对于Landau能级的非整数填充nu,(i)在零温度下对称性破裂,或者(ii)只有一个无隙激励的无限体积基态。我们还证明了以下两个定理:(a)如果纯无限量地基板对于非整数填充nu具有非零激发间隙,那么在零温度下会发生平移对称断裂。 (b)假设不存在非平移不变的无限体积基态。然后,如果纯无穷大基态具有非零的激励间隙,则填充系数nu必须等于有理数。在此,基态具有周期性结构,这是平移对称性破坏的结果。我们还讨论了我们的结果与量化霍尔电导之间的关系,并从现象学上解释了为什么给予量化霍尔电导的填充分数nu的奇数分母是唯一的偏爱。 [参考:53]

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