Abstract

For a power-law dispersion relation w(k) cc k, corresponding to an absolutely continuous spectrum of plane waves in spatial dimension d~, it is shown that the condition a m 2 d~ leads to the divergence of the time of permanence in the initial region of localization. We define this regime as quasi-absence of dfljfusion. Another interesting case, defined as quasi- d#jfusion, turns out to be d~ < a < 2 d~, for which the mean time of permanence is finite, but with divergingly large statistical fluctuations. These quantum regimes are discussed in connection with classical anomalous diffusion, Anderson localization in disordered systems and van Hove singularities in crystals.

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