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A simple approach to Anderson localization inone-dimensional disordered lattices

机译:一种简单的安德森定位一维无序晶格的方法

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We present a simple approach to Anderson localization in one-dimensional disordered lattices. We introduce the tight-binding model in which one orbital and a single random energy are assigned to each lattice site, and the hopping integrals are constant and restricted to nearest-neighbor sites. The localization of eigenstates is explained by two-parameter scaling arguments. We compare the size scaling of the level spacing in the bare energy spectrum of the quasi-particle (in the ideal lattice) with the size scaling of the renormalized disorder seen by the quasi-particle. The former decreases faster than the latter with increasing system size, giving rise to mixing and to the localization of the bare quasi-particle wave functions in the thermodynamic limit. We also provide a self-consistent calculation of the localization length and show how this length can be obtained from optical absorption spectra for Frenkel excitons. (C) 2004 American Association of Physics Teachers. [References: 22]
机译:我们为一维无序晶格中的安德森定位提供一种简单的方法。我们介绍了一个紧密绑定模型,其中一个轨道能量和一个随机能量分配给每个晶格位置,并且跳跃积分是恒定的,并且局限于最近邻位置。本征态的本地化由两参数缩放参数解释。我们将准粒子的裸能量谱(在理想晶格中)的能级间距的大小缩放与准粒子所看到的重归一化无序的大小缩放进行比较。随着系统尺寸的增加,前者的降速快于后者,从而导致混合和准热力学极限中的裸准粒子波函数定位。我们还提供了定位长度的自洽计算,并显示了如何从Frenkel激子的吸收光谱中获得该长度。 (C)2004年美国物理教师协会。 [参考:22]

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