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

K \approx S^2 = (\Delta \omega_r/\Delta_d)^2 > 1 .Here

K

is the perturbation parameter,while

S=\Delta\omegar/\Deltad

is the resonance-overlap parameter, given by the ratio of theunperturbed resonance width in frequency

\Delta\omegar

(often computed in the pendulumapproximation and proportional to the square-root of perturbation),and the frequency difference

\Deltad

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

External links

Notes and References

  1. http://www.quantware.ups-tlse.fr/chirikov/refs/chi1959.pdf