Critical-line conjecture for the disordered two-community noisy Kuramoto model

Let μ\mu be the common distribution of natural frequencies in the two communities, let ψ=ψ2ψ1{0,π}\psi=\psi_{2}-\psi_{1}\in\{0,\pi\}, and let r1,r2r_{1},r_{2} be the two synchronization order parameters. Define

χ=Rμ(dω)12(1+4ω2).\chi=\int_{\mathbb{R}}\mu(\mathrm{d}\omega)\,\frac{1}{2(1+4\omega^{2})}.

Assume that μ\mu is symmetric and unimodal. Critical-line conjecture. The parameter space (K,L)R2(K,L)\in\mathbb{R}^{2} has the following two regimes:

  • If K+Lcosψχ1K+L\cos\psi\leq\chi^{-1}, the only solution is the unsynchronized solution (r1,r2)=(0,0)(r_{1},r_{2})=(0,0).
  • If K+Lcosψ>χ1K+L\cos\psi>\chi^{-1}, there are at least two solutions: (r1,r2)=(0,0)(r_{1},r_{2})=(0,0) and a symmetric synchronized solution (r1,r2)=(r,r)(r_{1},r_{2})=(r,r) for some r(0,1)r\in(0,1).

This identifies the expected synchronization threshold when the two communities have identical symmetric unimodal disorder and the phase difference is 00 or π\pi. The surrounding discussion derives the critical line heuristically; excluding solutions with one order parameter zero is described as non-trivial.

Sources & referencesView supporting material

Primary source

J. M. Meylahn, “Two-community noisy Kuramoto model”, arXiv:1812.05896 (2019).

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