首页> 外文期刊>The European physical journal, B. Condensed matter physics >Delocalization in one-dimensional tight-binding models with fractal disorder II: existence of mobility edge
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Delocalization in one-dimensional tight-binding models with fractal disorder II: existence of mobility edge

机译:分形紊乱的一维紧密结合模型中的离域II:流动性边缘的存在

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摘要

In the previous work, we investigated the correlation-induced localization-delocalization transition (LDT) of the wavefunction at the band center (E = 0) in the one-dimensional tight-binding model with fractal disorder [H.S. Yamada, Eur. Phys. J. B 88, 264 (2015)]. In the present work, we study the energy (E not equal 0) dependence of the normalized localization length (NLL) and the delocalization of the wavefunction at different energy in the same system. The mobility edges in the LDT arise when the fractal dimension of the potential landscape is larger than the critical value depending on the disorder strength, which is consistent with the previous result. In addition, we present the distribution of individual NLL and Lyapunov exponents in the system with LDT.
机译:在先前的工作中,我们研究了一维具有分形紊乱的一维紧束缚模型中波函数在带中心(E = 0)的相关诱导的局域-离域跃迁(LDT)。山田E物理J.B 88,264(2015)]。在当前的工作中,我们研究归一化定位长度(NLL)的能量(E不等于0)依赖性以及在同一系统中不同能量下波函数的离域。当潜在势态的分形维数大于临界值(取决于无序强度)时,LDT中的迁移率边缘就会出现,这与先前的结果一致。此外,我们介绍了带有LDT的系统中各个NLL和Lyapunov指数的分布。

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