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We study the nature of electronic states in a tight-binding one-dimensional model with the on-site energies exhibiting long-range correlated disorder and nonrandom hopping amplitudes. The site energies describe the trace of a fractional Brownian motion with a specified spectral density S(k)∝1/k^α. Using a renormalization group technique, we show that for long-range correlated energy sequences with persistent increments ( α>2) the Lyapunov coefficient (inverse localization length) vanishes within a finite range of energy values revealing the presence of an Anderson-like metal-insulator transition.
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Moura et al. (1998) studied this question.
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