Abstract
The robustness and ubiquity of the macroscopic normal diffusion is well known to be derivable within Boltzmann-Gibbs statistical mechanics. It is essentially founded on (i) a variational principle applied to S = − f dxp(x)ln[p(x)] with simple a priori constraints, and (ii) the central limit theorem. Its basic characterization consists in the time evolution < x2 > ∝ t. A recently generalized statistical mechanics enables the extension of the same program in order to also cover the long-tail Lévy-like anomalous superdiffusion, a phenomenon frequently encountered in Nature. By so doing, this formalism succeeds where standard statistical mechanics and thermodynamics are known to fail.
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Tsallis, C., de Souza, A.M.C., Maynard, R. (1995). Derivation of Lévy-type anomalous superdiffusion from generalized statistical mechanics. In: Shlesinger, M.F., Zaslavsky, G.M., Frisch, U. (eds) Lévy Flights and Related Topics in Physics. Lecture Notes in Physics, vol 450. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-59222-9_40
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DOI: https://doi.org/10.1007/3-540-59222-9_40
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