2019
DOI: 10.1088/1367-2630/ab4f59
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Universal phase transitions to synchronization in Kuramoto-like models with heterogeneous coupling

Abstract: We reveal a class of universal phase transitions to synchronization in Kuramoto-like models with both in-and out-coupling heterogeneity. By analogy with metastable states, an oscillatory state occurs as a high-order coherent phase accompanying explosive synchronization in the system. The critical points of synchronization transition and the stationary solutions are obtained analytically, by the use of mean-field theory. In particular, the stable conditions for the emergence of phase-locked states are determine… Show more

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Cited by 28 publications
(5 citation statements)
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“…To highlight the heterogeneity of coupling, we restrict ourselves to a special setting, namely, K i j = K|ω i | (in-coupling) with K > 0 [37][38][39][40][41][42][43][44]. The effect is to endow the oscillators with heterogeneous coupling establishing the frequency-coupling correlations in the coupled system.…”
Section: Dynamical Model and Numerical Resultsmentioning
confidence: 99%
“…To highlight the heterogeneity of coupling, we restrict ourselves to a special setting, namely, K i j = K|ω i | (in-coupling) with K > 0 [37][38][39][40][41][42][43][44]. The effect is to endow the oscillators with heterogeneous coupling establishing the frequency-coupling correlations in the coupled system.…”
Section: Dynamical Model and Numerical Resultsmentioning
confidence: 99%
“…In this setting, the randomness is intrinsic to the oscillators themselves rather than to the coupling between them [41][42][43][44][45][46][47][48][49]. Moreover, β ≥ 1 (β < 1) sets up a positive (negative) feedback between the coupling and the coherence of the system [50][51][52][53][54][55].…”
Section: Mathematical Model and Its Stationary Solutionsmentioning
confidence: 99%
“…In this setup, the bifurcation mechanism for phase transition in oscillator system becomes clear. On the one hand, ĝ(0) = 0 implies that the incoherent state loses its stability via Hopf bifurcation at the critical coupling K a = 2 πĝ(Ωc) [30,31], where Ω c is the imaginary part of the eigenvalue of the linear stability analysis about R = W = 0. On the other hand, the characteristic function F (s) indicates that a saddle node bifurcation takes place at K c = F (s c ) −1 , at which a number of oscillators lock their phases forming a macroscopic order characterized by a non-zero W c = s c F (s c ).…”
Section: A Tiered Phase Transitionmentioning
confidence: 99%