Anderson Localization Phenomenon in One-dimensional Elastic Systems

R. A. Méndez-Sánchez, L. Gutiérrez, A. Morales, J. Flores, A. Díaz-de-Anda, G. Monsivais
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引用次数: 2

Abstract

The phenomenon of Anderson localization of waves in elastic systems is studied. We analyze this phenomenon in two different set of systems: disordered linear chains of harmonic oscillators and disordered rods which oscillate with torsional waves. The first set is analyzed numerically whereas the second one is studied both experimentally and theoretically. In particular, we discuss the localization properties of the waves as a function of the frequency. In doing that we have used the inverse participation ratio, which is related to the localization length. We find that the normal modes localize exponentially according to Anderson theory. In the elastic systems, the localization length decreases with frequency. This behavior is in contrast with what happens in analogous quantum mechanical systems, for which the localization length grows with energy. This difference is explained by means of the properties of the re ection coefficient of a single scatterer in each case.
一维弹性系统中的安德森局部化现象
研究了弹性系统中波的安德森局部化现象。我们在两种不同的系统中分析了这种现象:谐波振子的无序线性链和随扭波振荡的无序棒。对第一组进行了数值分析,对第二组进行了实验和理论研究。特别地,我们讨论了作为频率函数的波的局部化特性。在此过程中,我们使用了逆参与率,它与定位长度有关。根据Anderson理论,我们发现了正态模态的指数局域化。在弹性系统中,局部化长度随频率的增加而减小。这种行为与在类似的量子力学系统中发生的情况相反,在量子力学系统中,局部化长度随着能量的增长而增长。这种差异可以用每种情况下单个散射体的反射系数的性质来解释。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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