Abstract
An application of an effective numerical algorithm for solving eigenvalue problems which arise in modeling electronic properties of quantum disordered systems is considered. We study the electron states at the localization-delocalization transition induced by a random potential in the framework of the Anderson lattice model. The computation of the interior of the spectrum and corresponding wavefunctions for very sparse, Hermitian matrices of sizes exceeding 106×106 is performed by the Lanczos-type method especially modified for investigating statistical properties of energy levels and eigenfunction amplitudes.
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