Scholarlink

<p>Frequency desynchronized attractors cannot appear in identically coupled symmetric phase oscillators because “overtaking" of phases cannot occur. This restriction no longer applies for more general identically coupled oscillators. Hence, it is interesting to understand precisely how frequency synchrony is lost and how invariant sets such as attracting weak chimeras are generated at torus breakup, where the phase description breaks down. Maistrenko et al (2016) found numerical evidence of an organizing center for weak chimeras in a system of <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="332_2025_10137_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\(N=3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>=</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation> coupled identical Kuramoto oscillators with inertia. This paper identifies this organizing center and shows that it corresponds to a particular type of non-transverse heteroclinic bifurcation that is generic in the context of symmetry. At this codimension two bifurcation there is a splitting of connecting orbits between the in-phase (fully synchronized) state. This generates a wide variety of associated bifurcations to weak chimeras. We further highlight a second organizing center associated with a codimension two symmetry-breaking heteroclinic connection.</p>

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Global Bifurcations Organizing Weak Chimeras in Three Symmetrically Coupled Kuramoto Oscillators with Inertia

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  • 发表日期：

    2025年2月18日

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  • Peter Ashwin,
  • Christian Bick

摘要

Frequency desynchronized attractors cannot appear in identically coupled symmetric phase oscillators because “overtaking" of phases cannot occur. This restriction no longer applies for more general identically coupled oscillators. Hence, it is interesting to understand precisely how frequency synchrony is lost and how invariant sets such as attracting weak chimeras are generated at torus breakup, where the phase description breaks down. Maistrenko et al (2016) found numerical evidence of an organizing center for weak chimeras in a system of \(N=3\) N = 3 coupled identical Kuramoto oscillators with inertia. This paper identifies this organizing center and shows that it corresponds to a particular type of non-transverse heteroclinic bifurcation that is generic in the context of symmetry. At this codimension two bifurcation there is a splitting of connecting orbits between the in-phase (fully synchronized) state. This generates a wide variety of associated bifurcations to weak chimeras. We further highlight a second organizing center associated with a codimension two symmetry-breaking heteroclinic connection.