Chirikov criterion explained
The Chirikov criterion or Chirikov resonance-overlap criterionwas established by the Russian physicist Boris Chirikov.Back in 1959, he published a seminal article,[1] where he introduced the very first physical criterion for the onset of chaotic motion in deterministic Hamiltonian systems. He then applied such a criterion to explainpuzzling experimental results on plasma confinement in magnetic bottlesobtained by Rodionov at the Kurchatov Institute.
Description
According to this criterion a deterministic trajectory will begin to movebetween two nonlinear resonances in a chaotic and unpredictable manner, in the parameter range
Here
is the perturbation parameter,while
is the resonance-overlap parameter, given by the ratio of theunperturbed resonance width in frequency
(often computed in the pendulumapproximation and proportional to the square-root of perturbation),and the frequency difference
between two unperturbed resonances. Since its introduction, the Chirikov criterion has become an important analytical tool for the determination of the chaos border.
See also
References
- B.V.Chirikov, "Research concerning the theory of nonlinear resonance and stochasticity", Preprint N 267, Institute of Nuclear Physics, Novosibirsk (1969), (Engl. Trans., CERN Trans. 71-40 (1971))
- B.V.Chirikov, "A universal instability of many-dimensional oscillator systems", Phys. Rep. 52: 263 (1979)
- Book: A.J.Lichtenberg and M.A.Lieberman . Regular and Chaotic Dynamics . Springer, Berlin . 1992 . 978-0-387-97745-4. Springer link
External links
Notes and References
- http://www.quantware.ups-tlse.fr/chirikov/refs/chi1959.pdf