# Chirikov criterion

The Chirikov criterion or Chirikov resonance-overlap criterion was 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 explain puzzling experimental results on plasma confinement in magnetic bottles obtained by Rodionov at the Kurchatov Institute.

## Description

According to this criterion a deterministic trajectory will begin to move between two nonlinear resonances in a chaotic and unpredictable manner, in the parameter range

${\displaystyle K\approx S^{2}=(\Delta \omega _{r}/\Delta _{d})^{2}>1.}$

Here ${\displaystyle K}$  is the perturbation parameter, while ${\displaystyle S=\Delta \omega _{r}/\Delta _{d}}$  is the resonance-overlap parameter, given by the ratio of the unperturbed resonance width in frequency ${\displaystyle \Delta \omega _{r}}$  (often computed in the pendulum approximation and proportional to the square-root of perturbation), and the frequency difference ${\displaystyle \Delta _{d}}$  between two unperturbed resonances. Since its introduction, the Chirikov criterion has become an important analytical tool for the determination of the chaos border.