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.
At Q = 1 the NUIS collapses into a two-cluster state with equally populated groups
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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.