The Fractional Langevin Equation: Brownian Motion Revisited

نویسنده

  • Francesco MAINARDI
چکیده

It is well known that the concept of diffusion is associated with random motion of particles in space, usually denoted as Brownian motion, see e.g. [1-3]. Diffusion is considered normal when the mean squared displacement of the particle during a time interval becomes, for sufficiently long intervals, a linear function of it. When this linearity breaks down, degenerating in a power law with exponent α > 0 different from one, diffusion is referred to be anomalous: slow if 0 < α < 1 , fast if α > 1 ; see e.g. [4].

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تاریخ انتشار 2008