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Delocalization effects and charge reorganizations induced by repulsive interactions in strongly disordered chains

机译:强烈无序链中的排斥相互作用引起的离域效应和电荷重组

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We study the delocalization effect of a short-range repulsive interaction on the ground state of a finite density of spinless fermions in strongly disordered one dimensional lattices. The density matrix renormalization group method is used to explore the charge density and the sensitivity of the ground state energy with respect to the boundary condition (the persistent current) for a wide range of parameters (carrier density, interaction and disorder). Analytical approaches are developed and allow to understand some mechanisms and limiting conditions. For weak interaction strength, one has a Fermi glass of Anderson localized states, while in the opposite limit of strong interaction, one has a correlated array of charges (Mott insulator). In the two cases, the system is strongly insulating and the ground state energy is essentially invariant under a twist of the boundary conditions. Reducing the interaction strength from large to intermediate values, the quantum melting of the solid array gives rise to a more homogeneous distribution of charges, and the ground state energy changes when the boundary conditions are twisted. In individual chains, this melting occurs by abrupt steps located at sample-dependent values of the interaction where an (avoided) level crossing between the ground state and the first excitation can be observed. Important charge reorganizations taken place at the avoided crossings and the persistent currents are strongly enhanced around the corresponding interaction value. These large delocalization effects become smeared and reduced after ensemble averaging. They mainly characterize half filling and strong disorder, but they persist away of this optimal condition.
机译:我们研究了在强无序一维晶格中有限密度的无旋费米子的短程排斥相互作用对基态的离域效应。密度矩阵重归一化群方法用于针对各种参数(载流子密度,相互作用和无序度)探索边界条件(持续电流)的电荷密度和基态能量的敏感性。分析方法得到发展,并允许了解一些机制和限制条件。对于弱的相互作用强度,一个具有安德森局部状态的费米玻璃,而在强相互作用的相反极限中,一个具有相关的电荷阵列(莫特绝缘子)。在这两种情况下,系统是高度绝缘的,基态能量在边界条件的扭曲下基本上是不变的。将相互作用强度从大值降低到中间值,固体阵列的量子熔化导致电荷的分布更加均匀,并且当边界条件发生扭曲时,基态能量也会发生变化。在单个链中,这种熔化是通过位于相互作用的依赖于样本的值上的突变步骤发生的,其中可以观察到基态和第一次激发之间的(避免的)能级交叉。在避免的交叉处发生了重要的电荷重组,并且在相应的相互作用值附近,持续电流得到了显着增强。合奏平均后,这些大的离域效应变得模糊不清,并且减弱了。它们主要表现为半充盈和强烈紊乱,但仍坚持最佳状态。

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