Abstract
A necessary condition is derived for the emergence of diffusion instability in media in which diffusion does not obey classical Fick laws. The equations derived by Yadav and Horsthemke [Phys. Rev. E 74, 066118 (2006)] using the continuous-time random walk model are employed as equations simulating reaction—diffusion processes. The waiting-time distribution function is represented by the sum of a finite number of exponents. It is shown that passage to the diffusion limit in the time variable is an incorrect operation if it is used to analyze diffusion instability in media with a distribution function that differs from the Poisson distribution function.
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Original Russian Text © V.P. Shkilev, 2010, published in Zhurnal Éksperimental’noĭ i Teoreticheskoĭ-Fiziki, 2010, Vol. 137, No. 1, pp. 183–190.
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Shkilev, V.P. A necessary condition for the emergence of diffusion instability in media with nonclassical diffusion. J. Exp. Theor. Phys. 110, 162–169 (2010). https://doi.org/10.1134/S106377611001019X
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DOI: https://doi.org/10.1134/S106377611001019X