
Contents
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7.1 The FitzHugh–Nagumo Model 7.1 The FitzHugh–Nagumo Model
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7.1.1 Nullclines 7.1.1 Nullclines
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7.1.2 Stability of the Equilibrium Points 7.1.2 Stability of the Equilibrium Points
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7.1.3 Instantaneous Current Pulses: Action Potentials 7.1.3 Instantaneous Current Pulses: Action Potentials
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7.1.4 Sustained Current Injection: A Limit Cycle Appears 7.1.4 Sustained Current Injection: A Limit Cycle Appears
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7.1.5 Onset of Nonzero Frequency Oscillations: The Hopf Bifurcation 7.1.5 Onset of Nonzero Frequency Oscillations: The Hopf Bifurcation
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7.2 The Morris–Lecar Model 7.2 The Morris–Lecar Model
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7.2.1 Abrupt Onset of Oscillations 7.2.1 Abrupt Onset of Oscillations
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7.2.2 Oscillations with Arbitrarily Small Frequencies 7.2.2 Oscillations with Arbitrarily Small Frequencies
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7.3 More Elaborate Phase Space Models 7.3 More Elaborate Phase Space Models
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7.4 Recapitulation 7.4 Recapitulation
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1727 Phase Space Analysis Of Neuronal Excitability
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Published:November 1998
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Abstract
The previous chapter provided a detailed description of the currents underlying the generation and propagation of action potentials in the squid giant axon. The Hodgkin-Huxley (1952d) model captures these events in terms of the dynamical behavior of four variables: the membrane potential and three state variables determining the state of the fast sodium and the delayed potassium conductances. This quantitative, conductance-based formalism reproduces the physiological data remarkably well and has been extremely fertile in terms of providing a mathematical framework for modeling neuronal excitability throughout the animal kingdom (for the current state of the art, see McKenna, Davis, and Zornetzer, 1992; Bower and Beeman, 1998; Koch and Segev, 1998). Collectively, these models express the complex dynamical behaviors observed experimentally, including pulse generation and threshold behavior, adaptation, bursting, bistability, plateau potentials, hysteresis, and many more. However, these models are difficult to construct and require detailed knowledge of the kinetics of the individual ionic currents. The large number of associated activation and inactivation functions and other parameters usually obscures the contributions of particular features (e.g., the activation range of the sodium activation particle) toward the observed dynamic phenomena. Even after many years of experience in recording from neurons or modeling them, it is a dicey business predicting the effect that varying one parameter, say, the amplitude of the calcium-dependent slow potassium current (Chap. 9), has on the overall behavior of the model. This precludes the development of insight and intuition, since the numerical complexity of these models prevents one from understanding which important features in the model are responsible for a particular phenomenon and which are irrelevant. Qualitative models of neuronal excitability, capturing some of the topological aspects of neuronal dynamics but at a much reduced complexity, can be very helpful in this regard, since they highlight the crucial features responsible for a particular behavior. By topological aspects we mean those properties that remain unchanged in spite of quantitative changes in the underlying system. These typically include the existence of stable solutions and their basins of attraction, limit cycles, bistability, and the existence of strange attractors.
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