12.07.2015 Views

Dynamical Systems in Neuroscience:

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Chapter 10Synchronization (seewww.izhikevich.com)In this chapter we consider networks of tonically spik<strong>in</strong>g neurons. As any other k<strong>in</strong>d ofphysical, chemical, or biological oscillators, such neurons could synchronize and exhibitcollective behavior that is not <strong>in</strong>tr<strong>in</strong>sic to any <strong>in</strong>dividual neuron. For example, partialsynchrony <strong>in</strong> cortical networks is believed to generate various bra<strong>in</strong> oscillations, such asthe alpha and gamma EEG rhythms. Increased synchrony may result <strong>in</strong> pathologicaltypes of activity, such as epilepsy. Coord<strong>in</strong>ated synchrony is needed for locomotion andswim pattern generation <strong>in</strong> fish. There is an ongo<strong>in</strong>g debate on the role of synchrony<strong>in</strong> neural computation, see e.g., the special issue of Neuron (September 1999) devotedto the b<strong>in</strong>d<strong>in</strong>g problem.Depend<strong>in</strong>g on the circumstances, synchrony could be good or bad, and it is importantto know what factors contribute to synchrony and how to control it. This is thesubject of the present chapter – the most advanced chapter of the book. It provides anice application of the theory developed earlier and hopefully gives some <strong>in</strong>sight <strong>in</strong>towhy the previous chapters might be worth master<strong>in</strong>g.Our goal is to understand how the behavior of two coupled neurons depends on their<strong>in</strong>tr<strong>in</strong>sic dynamics. First, we <strong>in</strong>troduce the method of description of an oscillation byits phase. Then, we describe various methods of reduction of coupled oscillators tosimple phase models. The reduction method and the exact form of the phase modeldepends on the type of coupl<strong>in</strong>g, i.e., whether it is pulsed, weak, or slow, and on thetype of bifurcations of the limit cycle attractor generat<strong>in</strong>g tonic spik<strong>in</strong>g. F<strong>in</strong>ally, weshow how to use phase models to understand the collective dynamics of many coupledoscillators.10.1 Pulsed Coupl<strong>in</strong>gIn this section we consider oscillators of the formẋ = f(x) + Aδ(t − t s ) , x ∈ R m , (10.1)457

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