Synchronization in the quaternionic Kuramoto model

Abstract

In this paper, we propose an NN oscillators Kuramoto model with quaternions H\mathbb{H}. In case the coupling strength is strong, a sufficient condition of synchronization is established for general N⩾2N\geqslant 2. On the other hand, we analyze the case when the coupling strength is weak. For N=2N=2, when coupling strength is weak (below the critical coupling strength λc\lambda_c), we show that new periodic orbits emerge near each equilibrium point, and hence phase-locking state exists. This phenomenon is different from the real Kuramoto system since it is impossible to arrive at any synchronization when λ<λc\lambda<\lambda_c. A theorem is proved which states that the closed contours form a set of "Baumkuchen" that is dense near each equilibrium point. In other words, the trajectory of phase difference lies on a 4D4D-torus surface. Therefore, this implies that the phase-locking state is Lyapunov stable but not asymptotically stable. The proof uses a new infinite buffer method ("δ/n\delta/n criterion") and a Lyapunov function argument. This has been studied both analytically and numerically. For N=3N=3, we consider Lion Dance flow, the analog of Cherry flow, to demonstrate that the quaternionic synchronization exists even when the coupling strength is "super weak" (when λ/ω3\lambda/\omega 3, the stable manifold of Lion Dance flow exists, and the number of these equilibria is ⌊N−12⌋\lfloor \frac{N-1}{2}\rfloor. Therefore, we conjecture that quaternionic synchronization always exists.Comment: 35 pages, 6 figure

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