paper

Anderson localization transition with long-ranged hoppings : analysis of the strong multifractality regime in terms of weighted Levy sums

arXiv:1006.1510 · doi:10.1088/1742-5468/2010/09/P09015

Abstract

For Anderson tight-binding models in dimension with random on-site energies and critical long-ranged hoppings decaying typically as , we show that the strong multifractality regime corresponding to small can be studied via the standard perturbation theory for eigenvectors in quantum mechanics. The Inverse Participation Ratios , which are the order parameters of Anderson transitions, can be written in terms of weighted Lévy sums of broadly distributed variables (as a consequence of the presence of on-site random energies in the denominators of the perturbation theory). We compute at leading order the typical and disorder-averaged multifractal spectra and as a function of . For , we obtain the non-vanishing limiting spectrum as . For , this method yields the same disorder-averaged spectrum of order as obtained previously via the Levitov renormalization method by Mirlin and Evers [Phys. Rev. B 62, 7920 (2000)]. In addition, it allows to compute explicitly the typical spectrum, also of order , but with a different -dependence for all . As a consequence, we find that the corresponding singularity spectra and differ even in the positive region , and vanish at different values , in contrast to the standard picture. We also obtain that the saddle value of the Legendre transform reaches the termination point where only in the limit .

13 pages, 2 figures, v2=final version

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