Source: Duke Math. J. Volume 146, Number 2
(2009), 331-360.
Consider the three-dimensional Anderson model with a zero mean and bounded independent, identically distributed random potential. Let $\lambda$ be the coupling constant measuring the strength of the disorder, and let $\sigma(E)$ be the self-energy of the model at energy $E$. For any $\epsilon{>}0$ and sufficiently small $\lambda$, we derive almost-sure localization in the band $E\le -\sigma(0)-\lambda^{4-\epsilon}$. In this energy region, we show that the typical correlation length $\xi_E$ behaves roughly as $O\big((|E|-\sigma(E))^{-1/2}\big)$, completing the argument outlined in the preprint of T. Spencer [18]
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References
M. Aizenman, Localization at weak disorder: Some elementary bounds, Rev. Math. Phys. 6 (1994), 1163--1182.
M. Aizenman and S. Molchanov, Localization at large disorder and at extreme energies: An elementary derivation, Comm. Math. Phys. 157 (1993), 245--278.
M. Aizenman, J. H. Schenker, R. M. Friedrich, and D. Hundertmark, Finite-volume fractional-moment criteria for Anderson localization, Comm. Math. Phys. 224 (2001), 219--253.
T. Chen, Localization lengths and Boltzmann limit for the Anderson model at small disorders in dimension $3$, J. Stat. Phys. 120 (2005), 279--337.
C. De Calan and V. Rivasseau, Local existence of the Borel transform in Euclidean $\Phi_4^4$, Comm. Math. Phys. 82 (1981/82), 69--100.
R. Del Rio, S. Jitomirskaya, Y. Last, and B. Simon, Operators with singular continuous spectrum, IV: Hausdorff dimensions, rank one perturbations, and localization, J. Anal. Math. 69 (1996), 153--200.
L. ErdőS and H.-T. Yau, Linear Boltzmann equation as the weak coupling limit of a random Schrödinger equation, Comm. Pure Appl. Math. 53 (2000), 667--735.
J. Feldman, J. Magnen, V. Rivasseau, and R. SéNéOr, Bounds on completely convergent Euclidean Feynman graphs, Comm. Math. Phys. 98 (1985), 273--288.
J. FröHlich and T. Spencer, Absence of diffusion in the Anderson tight binding model for large disorder or low energy, Comm. Math. Phys. 88 (1983), 151--184.
S. Katsura and S. Inawashiro, Asymptotic form of the lattice Green's function of the simple cubic lattice, Progr. Theoret. Phys. 50 (1973), 82--94.
F. Klopp, Weak disorder localization and Lifshitz tails, Comm. Math. Phys. 232 (2002), 125--155.
E. Kolley and W. Kolley, Conductivity in Anderson-type models: A comparative study of critical disorder, J. Phys. C 21 (1988), 6099--6109.
G. F. Lawler, Intersection of Random Walks, Probab. Appl., Birkhäuser, Boston, 1991.
I. M. Lifshitz, Energy spectrum structure and quantum states of disordered condensed systems, Soviet Physics Uspekhi 7 (1965), 549--573.
—, Theory of fluctuations in disordered systems, Sov. Phys. JETP 26 (1968), 462--469.
N. Minami, Local fluctuation of the spectrum of a multidimensional Anderson tight binding model, Comm. Math. Phys. 177 (1996), 709--725.
C. M. Soukoulis, A. D. Zdetsis, and E. N. Economou, Localization in three-dimensional systems by a Gaussian random potential, Phys. Rev. B 34 (1986), 2253--2257.
T. Spencer, Lifshitz tails and localization, preprint, 1993.
P. Stollmann, Caught by Disorder: Bound States in Random Media, Prog. Math. Phys. 20, Birkhäuser, Boston, 2001.
W.-M. Wang, Localization and universality of Poisson statistics for the multidimensional Anderson model at weak disorder, Invent. Math. 146 (2001), 365--398. \endthebibliography