12.07.2015 Views

Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

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Two-Dimensional <strong>Systems</strong> 99108642y0-2-4-6-8-10-10 -8 -6 -4 -2 0 2 4 6 8 10xFigure 4.6: Representative trajectories of the two-dimensional system (4.3,4.4).go<strong>in</strong>g. Thus, to understand the geometry of a vector field, it is always useful to plot afew representative trajectories start<strong>in</strong>g from various <strong>in</strong>itial po<strong>in</strong>ts, as we do <strong>in</strong> Fig. 4.6.Due to the uniqueness of the solutions, the trajectories cannot cross, so they partitionthe phase space <strong>in</strong>to various regions. This is an important step toward determ<strong>in</strong><strong>in</strong>gthe phase portrait of a two-dimensional system.Let us return to the I Na,p +I K -model (4.1, 4.2) with low-threshold K + current andexpla<strong>in</strong> two odd phenomena discussed <strong>in</strong> the first chapter: Failure to generate all-ornoneaction potentials (Fig. 1.5b) and <strong>in</strong>ability to have a fixed value of the thresholdvoltage. Brief and strong current pulses <strong>in</strong> Fig. 4.7 reset the value of the voltage variableV but do not change the value of the K + activation variable n. Thus, each voltagetrace after the pulse corresponds to a trajectory start<strong>in</strong>g with different values of V 0 butthe same value n 0 . We see that each trajectory makes a counter-clockwise excursionand returns to the rest state. However, the size of the excursion depends on the <strong>in</strong>itialvalue of the voltage variable and can be small (subthreshold response), <strong>in</strong>termediate, orlarge (action potential). This phenomenon was considered theoretically by FitzHugh <strong>in</strong>early sixties (see bibliography) and demonstrated experimentally by Cole et al. (1970)us<strong>in</strong>g squid giant axon at higher than normal temperatures.In Fig. 4.8 we apply a long pre-pulse current of various amplitudes to reset theK + activation variable n to various values, and then a brief strong pulse to reset Vto exactly −48 mV. Each voltage trace after the pulse corresponds to a trajectorystart<strong>in</strong>g with the same V 0 = −48 mV, but different values of n 0 . We see that sometrajectories return immediately to the rest state while others do so after generat<strong>in</strong>g anaction potential. Therefore, V = −48 mV is a subthreshold value when n 0 is large,and a superthreshold one otherwise.

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