Fig 4. The role of N₂, P and D on the desynchronisation for the PDF-control.

The average Kuramoto order parameter 〈R(t)〈 is reported as a function of number of controlled oscillators, N₂, and the control strength, P, for D = 10. For each couple (N₂, P) ∈ [5, 50] × [2, 40], we numerically simulate the PDF-controlled system on the KM involving N = 100 oscillators coupled using an all-to-all scheme; each point being the average of 25 independent realisations. The coupling parameter is K = 0.5 and the natural frequencies are drawn from a normal distribution $\mathcal{N}(1,\sigma )$, σ = 0.01 and the initial angles uniformly randomly drawn in [0, 2π].