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The phase diagram of the multi-dimensional Anderson localization via analytic determination of Lyapunov exponents

机译:Lyapunov指数解析确定的多维Anderson局部化的相图

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The method proposed by the present authors to deal analytically with the problem of Anderson localization via disorder [ J. Phys.: Condens. Matter 14, 13777 ( 2002)] is generalized for higher spatial dimensions D. In this way the generalized Lyapunov exponents for diagonal correlators of the wave function, [psi(n,m)(2)], can be calculated analytically and exactly. This permits to determine the phase diagram of the system. For all dimensions D > 2 one finds intervals in the energy and the disorder where extended and localized states coexist: the metal-insulator transition should thus be interpreted as a first-order transition. The qualitative differences permit to group the systems into two classes: low-dimensional systems ( 2 less than or equal to D less than or equal to 3), where localized states are always exponentially localized and high-dimensional systems ( D greater than or equal to D-c = 4), where states with non-exponential localization are also formed. The value of the upper critical dimension is found to be D-0 = 6 for the Anderson localization problem; this value is also characteristic of a related problem - percolation.
机译:本发明人提出的用于分析性地解决通过障碍的安德森定位问题的方法[J. Phys.:Condens.Chem.Soc.,2004,5,3]。物质14,13777(2002)被推广用于更高的空间尺寸D。这样,可以解析准确地计算出波浪函数对角相关器[psi(n,m)(2)]的广义Lyapunov指数。这允许确定系统的相图。对于所有D> 2的维,人们都发现了能量和无序的间隔,在这些状态中,扩展状态和局部状态共存:因此,金属-绝缘体跃迁应解释为一阶跃迁。定性差异允许将系统分为两类:低维系统(2个小于或等于D小于或等于3),其中局部状态始终是指数局部化的;高维系统(D大于或等于(Dc = 4)时,也会形成具有非指数局部化的状态。对于安德森定位问题,发现上临界尺寸的值是D-0 = 6。该值也是相关问题的特征-渗滤。

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