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The dynamics of an electron described by the one-dimensional tight-binding Hamiltonian with quasiperiodic (Fibonacci) modulation is studied numerically. The width of an initially localized wave packet is found to increase with time t in an overall power-law form {~}t^α (0<{α}<1). The exponent {α} continuously decreases with increasing strength of quasiperiodic modulation. Moreover, prominent hierarchical oscillations are found to occur in the case of strong modulation. These results are explained well by a renormalization-group argument.
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Abe et al. (1987) studied this question.
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