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. 2015 Sep 9;112(38):E5361–E5370. doi: 10.1073/pnas.1516400112

Fig. 7.

Fig. 7.

Phase plane analysis of Type II–Type I–Type II* transitions in a 2D reduction of the Connor–Stevens model. (A) FI curves in a 2D reduced Connor–Stevens model (see Methods) for three different values of g¯A corresponding to (Left) Type II, (Middle) Type I, and (Right) Type II*. Bifurcation types are indicated at the respective values of the applied current (Hopf, Andronov–Hopf; SN, Saddle Node; FLC, Fold Limit Cycle). Stars indicate the value of the applied current at which each phase plane is plotted. (B) Phase planes computed at spiking threshold for each of the three g¯A cases. The specific bifurcation induced by applied current, Iapp, is indicated on each plot (IHopf, Andronov–Hopf bifurcation; ISNIC, Saddle Node on Invariant Circle; ISN, Saddle Node). Open circles correspond to unstable fixed points, black filled circles correspond to stable fixed points, and half-filled circles correspond to saddle node points. V nullclines are shown in blue, and w nullclines are shown in green. (Insets) Phase plane detail during repetitive spiking; red dotted arrows indicate membrane potential trajectories.