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Dynamical Systems in Neuroscience:

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Burst<strong>in</strong>g 389spike synchronizationburst synchronizationFigure 9.51: Various regimes of synchronization of bursters.neurons but not for others. In contrast, other topological types of bursters have widelyvary<strong>in</strong>g <strong>in</strong>stantaneous <strong>in</strong>terspike frequencies, as <strong>in</strong> Fig. 9.49a, that scan or sweep abroad frequency range go<strong>in</strong>g all the way to zero.When the bifurcation from rest<strong>in</strong>g to spik<strong>in</strong>g state is of the saddle-node on <strong>in</strong>variantcircle type, i.e., the system is Class 1 excitable, the frequency of emerg<strong>in</strong>g spik<strong>in</strong>g isfirst small, and then <strong>in</strong>creases. Therefore, all “circle/*” bursters generate chirps with<strong>in</strong>stantaneous <strong>in</strong>terspike frequencies <strong>in</strong>creas<strong>in</strong>g from zero to a relatively large value,at least at the beg<strong>in</strong>n<strong>in</strong>g of the burst. Similarly, when the bifurcation of the spik<strong>in</strong>gstate is of the saddle-node on <strong>in</strong>variant circle or saddle homocl<strong>in</strong>ic orbit type, thefrequency of spik<strong>in</strong>g at the end of the burst decreases to zero, so all “*/circle” and“*/homocl<strong>in</strong>ic” bursters also generate chirps, as <strong>in</strong> Fig. 9.49a. In summary, all shadedbursters <strong>in</strong> Fig. 9.50 have sweep<strong>in</strong>g <strong>in</strong>terspike frequencies, so that one part of the burstis resonant for one neuron and another part of the same burst is resonant for anotherneuron.9.4.5 SynchronizationConsider two coupled burst<strong>in</strong>g neurons of the fast-slow type. S<strong>in</strong>ce each burster hastwo times scales, one for rhythmic spik<strong>in</strong>g and one for repetitive burst<strong>in</strong>g, there aretwo synchronization regimes:• Spike synchronization, as <strong>in</strong> Fig. 9.51, left.• Burst synchronization, as <strong>in</strong> Fig. 9.51, right.One of them does not imply the other. Of course, there is an additional regime whenspikes and bursts are synchronized. We will study synchronization phenomena <strong>in</strong> detail<strong>in</strong> Chap. 10; here we just mention how they depend on the topological type of burst<strong>in</strong>g.Let us consider spike synchronization first. S<strong>in</strong>ce we are <strong>in</strong>terested <strong>in</strong> the fast timescale, we neglect the slow variable dynamics for a while and treat two bursters ascoupled oscillators. A necessary condition for synchronization of two weakly coupledoscillators is that they have nearly equal frequencies. How near is “near” dependson the strength of the coupl<strong>in</strong>g. Thus, spike synchronization depends crucially on

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