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We study the time evolution of wave packets of noninteracting electrons in a two-dimensional disordered system in strong magnetic field. For wave packets built from states near the metal-insulator transition in the center of the lowest Landau band we find that the return probability to the origin p(t) decays algebraically, p(t){~}t₂^-D/2, with a nonconventional exponent D₂/2. D₂ is the generalized dimension describing the scaling of the second moment of the wave function. We show that the corresponding spectral measure is multifractal and that the exponent D₂/2 equals the generalized dimension D̃ \~₂ of the spectral measure.
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Huckestein et al. (1994) studied this question.
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