Abstract
Complex systems are based on interacting local computational units may show non-trivial emerging behaviors. Examples are the time evolution of an infectious disease in a certain city that is mutually influenced by an ongoing outbreak of the same disease in another city, or the case of a neuron firing spontaneously while processing the effects of afferent axon potentials.
A fundamental question is whether the time evolutions of interacting local units remain dynamically independent of each other, or whether they will change their states simultaneously, following identical rhythms. This is the notion of synchronization, which we will study throughout this chapter. Starting with the paradigmatic Kuramoto model we will learn that synchronization processes may be driven either by averaging dynamical variables, or through causal mutual influences. On the way, we will visit piecewise linear dynamical systems and the reference model for infectious diseases, the SIRS model.
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Notes
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Note, that \(\int dx \cos ^2(x) = [\cos {}(x)\sin {}(x)+x]/2\), modulo a constant.
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One has \(\int dx \cos ^2(x)\sin ^2(x) = x/8 - \sin {}(4x)/32\), plus an integration constant.
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In the complex plane, \(\psi _j(t)=\mathrm {e}^{i\theta _j(t)}= \mathrm {e}^{i(\omega t-kj)}\) corresponds to a plane wave on a periodic ring. Eq. (9.28) is then equivalent to the phase evolution of the wavefunction \(\psi _j(t)\). The system is invariant under translations \(j\to j+1\), which implies that the discrete momentum k is a good quantum number, in the jargon of quantum mechanics. The periodic boundary condition \(\psi _{j+N}=\psi _j\) is satisfied for \(k = 2\pi n_k/N\).
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Chimera states are shortly discussed on page 336.
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Maximal Lyapunov exponents are discussed together with the theory of discrete maps in Chap. 2.
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Gros, C. (2024). Synchronization Phenomena. In: Complex and Adaptive Dynamical Systems. Springer, Cham. https://doi.org/10.1007/978-3-031-55076-8_9
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