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Автор Monthus, Cécile
Автор Garel, Thomas
Дата выпуска 2011-05-01
dc.description A Dyson hierarchical model for Anderson localization, containing non-random hierarchical hoppings and random on-site energies, has been studied in the mathematical literature since its introduction by Bovier (1990 J. Stat. Phys. 59 745), with the conclusion that this model is always in the localized phase. Here we show that if one introduces alternating signs in the hoppings along the hierarchy (instead of choosing all hoppings of the same sign), it is possible to reach an Anderson localization critical point presenting multifractal eigenfunctions and intermediate spectral statistics. The advantage of this model is that one can write exact renormalization equations for some observables. In particular, we obtain that the renormalized on-site energies have the Cauchy distributions for exact fixed points. Another output of this renormalization analysis is that the typical exponent of critical eigenfunctions is always α<sub>typ</sub> = 2, independently of the disorder strength. We present numerical results concerning the whole multifractal spectrum f(α) and the compressibility χ of the level statistics, for both the box and the Cauchy distributions of the random on-site energies. We discuss the similarities and differences with the ensemble of ultrametric random matrices introduced recently by Fyodorov, Ossipov and Rodriguez (2009 J. Stat. Mech. L12001).
Формат application.pdf
Издатель Institute of Physics Publishing
Копирайт IOP Publishing Ltd
Название A critical Dyson hierarchical model for the Anderson localization transition
Тип paper
DOI 10.1088/1742-5468/2011/05/P05005
Electronic ISSN 1742-5468
Журнал Journal of Statistical Mechanics: Theory and Experiment
Том 2011
Первая страница P05005
Последняя страница 26
Аффилиация Monthus, Cécile; Institut de Physique Théorique, CNRS and CEA Saclay, 91191 Gif-sur-Yvette, France
Аффилиация Garel, Thomas; Institut de Physique Théorique, CNRS and CEA Saclay, 91191 Gif-sur-Yvette, France
Выпуск 05

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