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. 2020 Sep 4;16(9):e1008144. doi: 10.1371/journal.pcbi.1008144

Fig 8. Dependence of global phase-locking changes on the baseline state of the brain network model.

Fig 8

(A) The left axis (gray) shows the network-averaged baseline PLV ρglobal as a function of background drive PEbase-PE* for a coupling C = 2.5. The right axis (purple) shows the grand average 〈|Δρbase|〉 of the perturbation-induced absolute changes in baseline band PLVs as a function of PEbase-PE*. (B) The left axis (gray) shows the network-averaged baseline PLV ρglobal as a function of background drive PEbase-PE* for a coupling C = 2.5. The right axis (purple) shows the coefficient of variation of the perturbation-induced average absolute changes in baseline band PLVs, CoV[|Δρδibase|], as a function of PEbase-PE*. (C) The left axis (gray) shows the network-averaged baseline PLV ρglobal as a function of background drive PEbase-PE* for a coupling C = 2.5. The right axis (green) shows the grand average 〈|Δρexc|〉 of the perturbation-induced absolute changes in excited band PLVs as a function of PEbase-PE*. (D) The left axis (gray) shows the network-averaged baseline PLV ρglobal as a function of background drive PEbase-PE* for a coupling C = 2.5. The right axis (green) shows the standard deviation of the perturbation-induced average absolute changes in excited band PLVs, std[|Δρδiexc|], as a function of PEbase-PE*. (Note that here we consider the standard deviation rather than the coefficient of variation since the mean response in the excited band eventually drops to zero.).