Abstract
Chaotic dynamics of Hamiltonian systems can be described by the random process which resembles the Lévy-type flights and trappings in the phase space of a system. The probability distribution function satisfies the fractional in space and time generalization of the Fokker-Planck-Kolmogorov equation. Orders of the fractional derivatives in space and time can be connected to the Pesin's dimensions of the trajectories. A new look on the problem of Maxwell's Demon is discussed in the context of the anomalous (“strange”) kinetics.
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Zaslavsky, G.M. (1995). From Lévy flights to the fractional kinetic equation for dynamical chaos. 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_36
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DOI: https://doi.org/10.1007/3-540-59222-9_36
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