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A simple model of classical diffusion on a random chain is studied. The velocities to the right and to the left are calculated. When one changes continuously the probability distribution ρ of the hopping rates, a whole region is found where these two velocities vanish. In this region, the distance R covered by a particle during the time t behaves like R~tˣ, where x depends continuously on ρ. The exponent x is calculated for a simple example.
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Derrida et al. (1982) studied this question.
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