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Dynamical Systems in Neuroscience:

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Excitability 239co-existence of rest<strong>in</strong>g and spik<strong>in</strong>g statesYES(bistable)NO(monostable)subthreshold oscillationsNO(<strong>in</strong>tegrator)YES(resonator)saddle-nodesubcriticalAndronov-Hopfsaddle-node on<strong>in</strong>variant circlesupercriticalAndronov-HopfFigure 7.14: Classification of neurons <strong>in</strong>tomonostable/bistable <strong>in</strong>tegrators/resonatorsaccord<strong>in</strong>g to the bifurcation of the rest<strong>in</strong>gstate.orbit bifurcation <strong>in</strong> Fig. 7.13b, and <strong>in</strong> the oscillations with zero frequency at I = 3.08.Thus, the F-I behavior of the model <strong>in</strong> this figure (and <strong>in</strong> Fig. 7.10) exhibits Class 2excitability but Class 1 spik<strong>in</strong>g. Because of the logarithmic scal<strong>in</strong>g of the F-I curve atthe saddle homocl<strong>in</strong>ic bifurcation (see Sect. 6.2.4), estimat<strong>in</strong>g experimentally the zerovalue of the F-I curves is challeng<strong>in</strong>g.Interest<strong>in</strong>gly, steps of <strong>in</strong>jected dc-current, as <strong>in</strong> Fig. 7.10c, <strong>in</strong>duce the transition“rest<strong>in</strong>g → spik<strong>in</strong>g”. But because the model <strong>in</strong> the figure is near codimension-2Bogdanov-Takens bifurcation, the steps test the frequency of the limit cycle attractorat the bifurcation “spik<strong>in</strong>g → rest<strong>in</strong>g”, as <strong>in</strong> Fig. 7.10e; that is, they test the classof spik<strong>in</strong>g! The F-I curve <strong>in</strong> response to steps <strong>in</strong> the figure is the same as the F-I curve<strong>in</strong> response to a slowly decreas<strong>in</strong>g current ramp. As an exercise, expla<strong>in</strong> why this istrue for Fig. 7.10 but not for Fig. 7.13.To summarize, we def<strong>in</strong>e the class of excitability accord<strong>in</strong>g to the frequency ofemerg<strong>in</strong>g spik<strong>in</strong>g of a neuron <strong>in</strong> response to a slowly <strong>in</strong>creas<strong>in</strong>g current ramp. The classof excitability corresponds to a bifurcation of the rest<strong>in</strong>g state (equilibrium) result<strong>in</strong>g<strong>in</strong> the transition “rest<strong>in</strong>g → spik<strong>in</strong>g”. We def<strong>in</strong>e the class of spik<strong>in</strong>g accord<strong>in</strong>g to thefrequency of disappear<strong>in</strong>g spik<strong>in</strong>g of a neuron <strong>in</strong> response to a slowly decreas<strong>in</strong>g currentramp. The class of spik<strong>in</strong>g corresponds to the bifurcation of the limit cycle result<strong>in</strong>g <strong>in</strong>the transition “spik<strong>in</strong>g → rest<strong>in</strong>g”. Stimulat<strong>in</strong>g a neuron with the ramps (and pulses)is the first step <strong>in</strong> explor<strong>in</strong>g the bifurcations <strong>in</strong> the neuron dynamics. Comb<strong>in</strong>ed withthe test for the existence of subthreshold oscillations of the membrane potential, it tellswhether the neuron is an <strong>in</strong>tegrator or a resonator, and whether it is monostable orbistable, as we discuss next.7.2 Integrators vs. ResonatorsIn this book we classify excitable systems based on two features: the co-existence ofrest<strong>in</strong>g and spik<strong>in</strong>g states and the existence of subthreshold oscillations. The formerfeature divides all systems <strong>in</strong>to monostable and bistable. The latter feature dividesall systems <strong>in</strong>to <strong>in</strong>tegrators (no oscillations) and resonators. These features determ<strong>in</strong>e

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