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. 2009 Feb 4;101(4):2146–2165. doi: 10.1152/jn.90958.2008

FIG. 9.

FIG. 9.

Generation of one-phase oscillations in the pre-BötC model. A: traces of output activities of pre-I and early-I neurons. B: bifurcation diagram for the full system given by Eqs. 1, 2, and 5, generated with dimensionless bifurcation parameter D1. For each fixed D1, the full system has a unique equilibrium point, at which the time derivatives of all variables are zero. The curve formed of these points is plotted, with a dashed component where these points are unstable and a solid component where they are stable. Also, for each D1 value that is not too large, the system has a periodic solution, which is a one-phase oscillation. For each such D1 value, the maximal and minimal values of V1 along the one-phase oscillation are marked with circles. As D1 grows, oscillations are terminated in an Andronov–Hopf (AH) bifurcation near D1 = 0.03 and, for larger D1, the only stable state is an equilibrium point of the full system. C: one-phase oscillations (solid) superimposed on V1 nullclines (dashed) in the (V1, hNaP) plane, for various D1 values as indicated. Recall that each V1 nullcline is the collection of points on which dV1/dt = 0 for the corresponding D1. The hNaP-nullcline, which consists of points where dhNaP/dt = 0 and which is independent of D1 (see Eq. 5), is also shown (dash-dotted). The oscillations evolve clockwise and the amplitude shrinks as D1 increases such that the bifurcation is approached. D: changes of the oscillation period (T) and the durations of inspiration (TI) and expiration (TE) produced by changes in total (dimensionless) drive to pre-I neuron (D1).