An isochron-based expansion produces second- and third-order phase equations for the MF-CGLE that include non-pairwise interactions responsible for its collective chaos at moderate coupling.
In the latter case, among infinitely many oscillator densities with R = 0 , there is a convergence to the UIS under an arbitrarily weak noise [22]
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Phase reduction beyond the first order: the case of the mean-field complex Ginzburg-Landau equation
An isochron-based expansion produces second- and third-order phase equations for the MF-CGLE that include non-pairwise interactions responsible for its collective chaos at moderate coupling.