12.07.2015 Views

Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

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Bifurcations 1831K+ activation variable, n0.5stablelimit cycleunstable limitcyclen-nullcl<strong>in</strong>eV-nullcl<strong>in</strong>estable equilibrium (rest)0-80 -70 -60 -50 -40 -30 -20 -10 0 10membrane voltage, V (mV)Figure 6.14: Phase portrait of the I Na,p +I K -model: Unstable limit cycle (dashed circle)is often surrounded by a stable one (solid circle) <strong>in</strong> two-dimensional neuronal models.F<strong>in</strong>ally, notice that there is always a bistability, i.e., co-existence, of the rest<strong>in</strong>gattractor and some other attractor near a subcritical Andronov-Hopf bifurcation <strong>in</strong>2-dimensional conductance-based models, as <strong>in</strong> Fig. 6.14 (<strong>in</strong> non-neural models, thetrajectories could go to <strong>in</strong>f<strong>in</strong>ity and there need not be bistability). The bistabilitymust also be present at the saddle-node bifurcation of an equilibrium, but may or maynot be present at the saddle-node on <strong>in</strong>variant circle or at a supercritical Andronov-Hopf bifurcation.Delayed loss of stabilityIn Fig. 6.17a we <strong>in</strong>ject a ramp of current <strong>in</strong>to the I Na,p +I K -model to drive it slowlythrough the subcritical Andronov-Hopf bifurcation po<strong>in</strong>t I ≈ 48.75 (see Fig. 6.16). Wechoose the ramp so that the bifurcation occurs exactly at t = 100. Even though thefocus equilibrium is unstable for t > 100, the membrane potential rema<strong>in</strong>s near -50mV as if the equilibrium were still stable. This phenomenon, discovered by Shishkova(1973), is called delayed loss of stability. It is ubiquitous <strong>in</strong> simulations of smoothdynamical systems near subcritical or supercritical Andronov-Hopf bifurcations.The mechanism of delayed loss of stability is quite simple. The state of the systemis attracted to the stable focus while t < 100. Even though the focus loses stabilityat t = 100, the state of the system is <strong>in</strong>f<strong>in</strong>itesimally close to the equilibrium, so ittakes a long time to diverge from it. The longer the convergence to the equilibrium,the longer the divergence from it, hence the noticeable delay. The delay has an upperbound that depends on the smoothness of the dynamical system (Nejshtadt 1985).It can be shortened or even reversed (advanced loss of stability) by weak noise thatis always present <strong>in</strong> neurons. This may expla<strong>in</strong> why the delay has never been seen

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