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Dynamical Systems in Neuroscience:

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Conductance-Based Models 163v peak , and the voltage reset value is c. The parameter d describes the total amount ofoutward m<strong>in</strong>us <strong>in</strong>ward currents activated dur<strong>in</strong>g the spike and affect<strong>in</strong>g the after-spikebehavior. All these parameters can be easily fit to any particular neuron type, as weshow <strong>in</strong> Chap. 8.Review of Important Concepts• Amplify<strong>in</strong>g gat<strong>in</strong>g variables describe activation of an <strong>in</strong>ward currentor <strong>in</strong>activation of an outward current. They amplify voltage changes.• Resonant gat<strong>in</strong>g variables describe <strong>in</strong>activation of an <strong>in</strong>ward currentor activation of an outward current. They resist voltage changes.• To exhibit excitability, it is enough to have one amplify<strong>in</strong>g and oneresonant gat<strong>in</strong>g variable <strong>in</strong> a neuronal model.• Many models can be reduced to two-dimensional systems with oneequation for voltage and <strong>in</strong>stantaneous amplify<strong>in</strong>g currents, and oneequation for resonant gat<strong>in</strong>g variable.• The behavior of a two-dimensional model depends on the positionof its nullcl<strong>in</strong>es. Many models have an N-shaped V -nullcl<strong>in</strong>e and asigmoid shaped nullcl<strong>in</strong>e for the gat<strong>in</strong>g variable.• There is a relationship between nullcl<strong>in</strong>es and I-V curves.• Quite different electrophysiological models can have similar nullcl<strong>in</strong>es,and hence essentially the same dynamics.• The spike-generation mechanism of detailed electrophysiologicalmodels depends on the dynamics near the left knee of the fast V -nullcl<strong>in</strong>e, and it can be captured by a simple model (5.5, 5.6).Bibliographical NotesRichard FitzHugh pioneered the usage of phase planes and nullcl<strong>in</strong>es to study theHodgk<strong>in</strong>-Huxley model (FitzHugh 1955). Later, he suggested a simple model withN-shaped cubic V -nullcl<strong>in</strong>e and a straight-l<strong>in</strong>e slow nullcl<strong>in</strong>e, known as the FitzHugh-Nagumo model, to illustrate the mechanism of excitability of the Hodgk<strong>in</strong>-Huxleysystem. However, it was Kr<strong>in</strong>skii and Kokoz (1973) who first discovered the relationshipn(t) + h(t) ≈ const and were thus able to reduce the four-dimensional Hodgk<strong>in</strong>-Huxleymodel to a two-dimensional system. S<strong>in</strong>ce then, the phase plane analysis of neuronalmodels became standard, at least <strong>in</strong> Russian language literature.Current awareness of the geometrical methods of phase plane analysis of neuronal

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