LPTMC, CNRS-UMR 7600, Université Pierre et Marie Curie, boîte 121, 75252 Paris cédex 05, France.
Institut de physique théorique, Université Paris Saclay, CEA, CNRS, F-91191 Gif-sur-Yvette, France.
Phys Rev Lett. 2016 Jan 8;116(1):010601. doi: 10.1103/PhysRevLett.116.010601.
This work provides a thorough study of Lévy, or heavy-tailed, random matrices (LMs). By analyzing the self-consistent equation on the probability distribution of the diagonal elements of the resolvent we establish the equation determining the localization transition and obtain the phase diagram. Using arguments based on supersymmetric field theory and Dyson Brownian motion we show that the eigenvalue statistics is the same one as of the Gaussian orthogonal ensemble in the whole delocalized phase and is Poisson-like in the localized phase. Our numerics confirm these findings, valid in the limit of infinitely large LMs, but also reveal that the characteristic scale governing finite size effects diverges much faster than a power law approaching the transition and is already very large far from it. This leads to a very wide crossover region in which the system looks as if it were in a mixed phase. Our results, together with the ones obtained previously, now provide a complete theory of Lévy matrices.
这项工作对 Lévy 或重尾随机矩阵 (LMs) 进行了深入研究。通过分析关于解算符对角元素概率分布的自洽方程,我们建立了确定局域化转变的方程,并得到了相图。利用基于超对称场论和狄森布朗运动的论证,我们表明在整个离域相中的本征值统计与高斯正交系综相同,而在局域相中则是泊松型的。我们的数值计算证实了这些在无限大 LMs 极限下成立的发现,并且还表明控制有限尺寸效应的特征尺度比趋近于转变的幂律快得多,并且在远离转变时已经非常大。这导致了一个非常宽的交叉区域,在这个区域中,系统看起来好像处于混合相。我们的结果与之前获得的结果一起,现在提供了 Lévy 矩阵的完整理论。