Abstract
We consider the usual one-dimensional tight-binding Anderson model with the random potential taking only two values, 0 andλ, with probabilityp and 1−p, 0<p<1. We show that the Liapunov exponentγ λ (E), E ε R. diverges asλ → ∞ uniformly in the energyE. Using a result of Carmona, Klein, and Martinelli, this proves that forλ large enough, the integrated density of states is singular continuous. We also compute explicitly the exact asymptotics for a dense set of energies and we compare the results with numerical simulations.
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Martinelli, F., Micheli, L. On the large-coupling-constant behavior of the Liapunov exponent in a binary alloy. J Stat Phys 48, 1–18 (1987). https://doi.org/10.1007/BF01010397
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DOI: https://doi.org/10.1007/BF01010397