2014
DOI: 10.1103/physreve.89.012810
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Nature of synchronization transitions in random networks of coupled oscillators

Abstract: We consider a system of phase oscillators with random intrinsic frequencies coupled through sparse random networks and investigate how the connectivity disorder affects the nature of collective synchronization transitions. Various distribution types of intrinsic frequencies are considered: uniform, unimodal, and bimodal distribution. We employ a heterogeneous mean-field approximation based on the annealed networks and also perform numerical simulations on the quenched Erdös-Rényi networks. We find that the con… Show more

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Cited by 21 publications
(31 citation statements)
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“…2(c) confirm by the annealed MF th case with the bimoda transition with β = 1/ as seen in Fig. 2(d Adapted with permission from [70]. Copyrighted by the American Physical Society.…”
Section: Conclusion and Dsupporting
confidence: 59%
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“…2(c) confirm by the annealed MF th case with the bimoda transition with β = 1/ as seen in Fig. 2(d Adapted with permission from [70]. Copyrighted by the American Physical Society.…”
Section: Conclusion and Dsupporting
confidence: 59%
“…63 [69] The next is step is then verifying how the synchronization phase transition changes if the link-disorder is removed, while keeping the fluctuations in the frequency. More specifically, in this case, the connections between oscillators are kept constant over different realizations of the network dynamics (networks whose adjacency matrices are fixed over time or over different realizations are also referred as quenched networks [70,71]). At first, one could expect that the phase transition remains unchanged except from a shift in the coupling strength.…”
Section: Conclusion and Dmentioning
confidence: 99%
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“…In analogy with equilibrium critical phenomena, we expect the order parameter in the critical region to satisfy the FSS [14],…”
Section: Random Frequency Distributionmentioning
confidence: 99%
“…(3.7), we examine the local slopes of χ against | | in double logarithmic plots for very large N . The effective exponent γ eff is defined as 14) and the critical exponents are obtained from their asymptotic values as γ = lim →0 + γ eff ( ) and γ = lim →0 − γ eff ( ). Figure 4 shows the inverse of the effective exponent γ −1 eff as a function of .…”
Section: B Dynamic Fluctuationsmentioning
confidence: 99%