Analytic stability boundaries for pinned, split-pinned, sync-dot, and phase-locked states are derived for forced swarmalators in 2D and 3D periodic domains, extending previous 1D results.
Global synchronization theorem for coupled swarmalators
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abstract
The global stability of oscillator networks has attracted much recent attention. Ordinarily, the oscillators in such studies are motionless; their spatial degrees of freedom are either ignored (e.g. mean field models) or inactive (e.g geometrically embedded networks like lattices). Yet many real-world oscillators are mobile, moving around in space as they synchronize in time. Here we prove a global synchronization theorem for such swarmalators for a simple model where the units' movements are confined to a 1d ring. This can be thought of as a generalization from oscillators connected on random networks to oscillators connected on temporal networks, where the edges are determined by the oscillators' movements.
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On forced swarmalators that move in higher-dimensional spaces
Analytic stability boundaries for pinned, split-pinned, sync-dot, and phase-locked states are derived for forced swarmalators in 2D and 3D periodic domains, extending previous 1D results.