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.
( 29) are somewhat unex- pected, (nonetheless see [17]) , since they depend on the mean fields Z1 and Z2, but not on θj itself
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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.