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Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

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226 Excitabilityspike?spikerestrestexcitableoscillatoryFigure 7.1: Left: An abstract def<strong>in</strong>ition of excitability. There is a spike trajectory thatstarts near a stable equilibrium and returns to it. Right: Excitable systems are nearbifurcations. A modification of the vector field <strong>in</strong> the small shaded region can result<strong>in</strong> a periodic trajectory.that push the state of the neuron to or near the beg<strong>in</strong>n<strong>in</strong>g of the large trajectory(small square <strong>in</strong> Fig. 7.1), thereby <strong>in</strong>itiat<strong>in</strong>g the spike. These <strong>in</strong>puts can be <strong>in</strong>jected byexperimenter via an attached electrode, or they can represent the total synaptic <strong>in</strong>putfrom the other neurons <strong>in</strong> the network, or both.7.1.1 BifurcationsThe def<strong>in</strong>ition <strong>in</strong> Fig. 7.1 is quite general, and it does not make any assumptions regard<strong>in</strong>gthe details of the vector field <strong>in</strong>side or outside of the small shaded neighborhood.Us<strong>in</strong>g the theory presented <strong>in</strong> the previous chapter, we can show that such an excitablesystem is near a bifurcation from rest<strong>in</strong>g to oscillatory dynamics.• Bifurcation of a limit cycle. The vector field <strong>in</strong> the small shaded neighborhoodof the equilibrium can be modified slightly so that the spike trajectory enters thesquare and becomes periodic, as <strong>in</strong> Fig. 7.1, right. That is, the dynamical systemgoes through a bifurcation result<strong>in</strong>g <strong>in</strong> the appearance of a limit cycle.What happens to the stable equilibrium, denoted as “?” <strong>in</strong> the figure? Depend<strong>in</strong>g onthe type of the bifurcation of the limit cycle, the equilibrium may disappear or may losestability. This happens when the limit cycle appears via saddle-node on <strong>in</strong>variant circleor supercritical Andronov-Hopf bifurcations, respectively. Both cases are depicted <strong>in</strong>Fig. 7.2.

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