The diffusion coefficient D in a periodic potential with exponentially
decaying memory friction is studied by the matrix-continued-fraction
method. it is shown that, at sufficiently high static friction, D pres
ents a maximum as a function of the memory decay parameter. This maxim
um is due to the interplay between two oscillatory motions, the first
induced by the periodic potential and the second by the memory. The ma
ximum appears when the frequencies of these motions are in resonance.
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