1995/11/02 by Constantino Tsallis, Dirk Jan Bukman · 2 citations
Physics and Astronomy · #cond-mat
paper · pdf · doi:10.1103/physreve.54.r2197
11 pages, RevTeX, 3 uuencoded postscript figures
arxiv created 1995/11/02 · arxiv updated 2009/11/30
The optimization of the usual entropy S1[p]=-∫ du p(u) ln p(u) under appropriate constraints is closely related to the Gaussian form of the exact time-dependent solution of the Fokker-Planck equation describing an important class of normal diffusions. We show here that the optimization of the generalized entropic form Sq[p]=\1- ∫ du [p(u)]q\/(q-1) (with q=1+μ-ν∈ \bf \calR) is closely related to the calculation of the exact time-dependent solutions of a generalized, nonlinear, Fokker Planck equation, namely (∂)/(∂ t)pμ= -(∂)/(∂ x)[F(x)pμ]+D \frac∂2 ∂ x2pν, associated with anomalous diffusion in the presence of the external force F(x)=k1-k2x. Consequently, paradigmatic types of normal (q=1) and anomalous (q ≠ 1) diffusions occurring in a great variety of physical situations become unified in a single picture.