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Dynamical Systems in Neuroscience:

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276 ExcitabilityBibliographical NotesThere is no universally accepted def<strong>in</strong>ition of excitability. Our def<strong>in</strong>ition is consistentwith the one <strong>in</strong>volv<strong>in</strong>g ε-pseudo-orbits (Izhikevich 2000). R. FitzHugh (1955, 1960,1976) pioneered geometrical analyses of phase portraits of neuronal models with theview to understand their neuro-computational properties. It is amaz<strong>in</strong>g that such importantneuro-computational properties as all-or-none action potentials, fir<strong>in</strong>g thresholds,and <strong>in</strong>tegration of EPSPs are still <strong>in</strong>troduced and illustrated us<strong>in</strong>g the Hodgk<strong>in</strong>-Huxley model, which accord<strong>in</strong>g to FitzHugh, cannot have these properties. Throughoutthis chapter we follow Izhikevich (2000) to compare and contrast neuro-computationalproperties of <strong>in</strong>tegrators and resonators.The frozen noise experiment <strong>in</strong> Fig. 7.24 was pioneered by Bryant and Segundo <strong>in</strong>1976, but due to an <strong>in</strong>terest<strong>in</strong>g quirk of history, it is better known at present as theMa<strong>in</strong>en-Sejnowski (1995) experiment (despite the fact that the latter paper refers tothe former). Post-<strong>in</strong>hibitory facilitation was po<strong>in</strong>ted out by Luk and Aihara (2000),Izhikevich (2001). John R<strong>in</strong>zel suggested to call it “post-<strong>in</strong>hibitory exaltation” (<strong>in</strong>a similar va<strong>in</strong>, the phenomenon <strong>in</strong> Fig. 7.49b may be called “post-excitatory hesitation”).Richardson et al. (2003) po<strong>in</strong>ted out that frequency preference and resonanceoccurs without subthreshold oscillations when the system is near the transition froman <strong>in</strong>tegrator to a resonator.The Hodgk<strong>in</strong>’s classification of neuronal excitability can be applied to classify anyrhythmic system, e.g., contractions of uterus dur<strong>in</strong>g labor. Typically, the contractionsstart with low frequency that gradually <strong>in</strong>creases — Class 1 excitability. The author’swife had to be <strong>in</strong>duced pharmacologically to evoke labor contractions, which is a typicalmedical <strong>in</strong>tervention when the baby is overdue. The contraction monitor showed as<strong>in</strong>usoidal signal with constant period, around 2 m<strong>in</strong>utes, but slowly grow<strong>in</strong>g amplitude— Class 2 excitability via supercritical Andronov-Hopf bifurcation! S<strong>in</strong>ce the motherhad an advance degree <strong>in</strong> applied mathematics, the author waited for a 1-m<strong>in</strong>ute periodof quiescence between the contractions and managed to expla<strong>in</strong> to the deliver<strong>in</strong>g motherthe basic relationship between bifurcations and excitability. Five years later, <strong>in</strong>duceddelivery of the author’s second daughter resulted <strong>in</strong> the same supercritical Andronov-Hopf bifurcation. The author rem<strong>in</strong>ded this concept to the mother and expla<strong>in</strong>ed it tothe obstetrician m<strong>in</strong>utes after the delivery.Exercises1. When can the FitzHugh-Nagumo model (4.11, 4.12) exhibit <strong>in</strong>hibition-<strong>in</strong>ducedspik<strong>in</strong>g, such as the one <strong>in</strong> Fig. 7.32?2. (French ducks) Numerically <strong>in</strong>vestigate the quasi-threshold <strong>in</strong> the FitzHugh-Nagumo model (4.11, 4.12). How is it related to the French duck (canard; seeEckhaus 1983) limit cycles discussed <strong>in</strong> Sect. 6.3.4?

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