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Conservative dynamics in phase oscillator networks

Arkady Pikovsky

Abstract

The interaction between phase oscillators is conservative if the phase volume is conserved throughout the dynamics. We derive a general condition, based on the notion of a pair-Hamiltonian, for the pairwise couplings to be conservative. The conservative networks with Winfree-type and Kuramoto-Daido-type couplings are also discussed. It is demonstrated that although, in contradistinction to genuine Hamiltonian dynamics, there is no exact pairwise symmetry of the Lyapunov exponents, the Lyapunov spectrum for a large network is nearly symmetric. The concept is also generalized to triplet and quadruplet couplings.

Conservative dynamics in phase oscillator networks

Abstract

The interaction between phase oscillators is conservative if the phase volume is conserved throughout the dynamics. We derive a general condition, based on the notion of a pair-Hamiltonian, for the pairwise couplings to be conservative. The conservative networks with Winfree-type and Kuramoto-Daido-type couplings are also discussed. It is demonstrated that although, in contradistinction to genuine Hamiltonian dynamics, there is no exact pairwise symmetry of the Lyapunov exponents, the Lyapunov spectrum for a large network is nearly symmetric. The concept is also generalized to triplet and quadruplet couplings.

Paper Structure

This paper contains 15 sections, 27 equations, 5 figures.

Figures (5)

  • Figure 1: Trajectories at the conservative Winfree-type coupling of two oscillators. Parameters are given in text.
  • Figure 2: Poincaré map at the conservative Winfree-type coupling of three oscillators. Parameters are given in text. For some initial conditions, the trajectory forms a closed curve (torus in the phase space), while at other initial conditions, chaotic sets are produced.
  • Figure 3: Cumulative distributions of the largest Lyapunov exponent for $N=3,4$ and different coupling strengths $\varepsilon$ (lines of different colors), calculated from $1000$ independent runs as described in the text.
  • Figure 4: The sums of the largest and of the smallest Lyapunov exponents vs the largest exponent for conservative networks of 5 phase oscillators.
  • Figure 5: Spectra of Lyapunov exponents for several values of $N$, for random networks with Kuramoto-type coupling \ref{['eq:12']}. The spectrum appears nearly anti-symmetric with respect to the midpoint $i=N/2$.