12.07.2015 Views

Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

SHOW MORE
SHOW LESS
  • No tags were found...

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Introduction 21Review of Important Concepts• Neurons are dynamical systems.• Rest<strong>in</strong>g state of neurons corresponds to a stable equilibrium, tonicspik<strong>in</strong>g state corresponds to a limit cycle attractor.• Neurons are excitable because the equilibrium is near a bifurcation.• There are many ionic mechanisms of spike-generation, but only fourgeneric bifurcations of equilibria.• These bifurcations divide neurons <strong>in</strong>to four categories: <strong>in</strong>tegratorsor resonators, monostable or bistable.• Analyses of phase portraits at bifurcations expla<strong>in</strong> why some neuronshave well-def<strong>in</strong>ed thresholds, all-or-none spikes, post-<strong>in</strong>hibitoryspikes, frequency preference, hysteresis, etc., while others do not.• These features, and not ionic currents per se, determ<strong>in</strong>e the neuronalresponses, i.e., the k<strong>in</strong>d of computations neurons do.• A good neuronal model must reproduce not only electrophysiologybut also the bifurcation dynamics of neurons.Bibliographical NotesRichard FitzHugh at the National Institutes of Health (NIH) pioneered the phase planeanalysis of neuronal models with the view to understand their neuro-computationalproperties. He was the first to analyze the Hodgk<strong>in</strong>-Huxley model (FitzHugh 1955;years before they received the Nobel prize) and to prove that it has neither thresholdnor all-or-none spikes. FitzHugh (1961) <strong>in</strong>troduced a simplified model of excitabilityand showed that one can get the right k<strong>in</strong>d of neuronal dynamics <strong>in</strong> models lack<strong>in</strong>gconductances and currents. Nagumo et al. (1962) designed a correspond<strong>in</strong>g tunneldiode circuit, so the model is called the FitzHugh-Nagumo oscillator. Chapter 8 dealswith such simplified models.FitzHugh research program was further developed by John R<strong>in</strong>zel and G. BardErmentrout. In their 1989 sem<strong>in</strong>al paper, R<strong>in</strong>zel and Ermentrout revived Hodgk<strong>in</strong>’sclassification of excitability and po<strong>in</strong>ted out to the connection between the behavior ofneuronal models and the bifurcations they exhibit. (They also refer to the excitabilityas “type I” and “type II”). Unfortunately, many people treat the connection <strong>in</strong> asimplem<strong>in</strong>ded fashion and <strong>in</strong>correctly identify “type I = saddle-node, type II = Hopf”.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!