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Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

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Simple Models 311membrane potential, v (mV)40200-20-40rest<strong>in</strong>g-60-80I=0I=0I=-1 nA<strong>in</strong>jected currentAsagB0 100 200 300time (ms)CDhyperpolarized staterest<strong>in</strong>grecovery variable, u2001000-100-200v-nullcl<strong>in</strong>e, I=-1 nAsagBv-nullcl<strong>in</strong>e, I=0ADresetrest<strong>in</strong>g-80 -60 -40 -20membrane potential, v (mV)Chyperpolarized statesaddlereboundspikeFigure 8.26: The mechanism of sag and rebound spike of the model <strong>in</strong> Fig. 8.25.equilibrium (black square), which is outside the attraction doma<strong>in</strong>. Upon release fromthe hyperpolarization, the trajectory fires a phasic spike and then returns to the rest<strong>in</strong>gstate. Some LTS <strong>in</strong>terneurons fire bursts of spikes, and for that reason are calledburst-spik<strong>in</strong>g non-pyramidal (BSNP) neurons.8.2.6 Fast spik<strong>in</strong>g (FS) <strong>in</strong>terneuronsFast spik<strong>in</strong>g neurons fire “fast” tonic spike tra<strong>in</strong>s of relatively constant amplitudeand frequency <strong>in</strong> response to depolarized pulses of current. In a systematic study,Tateno et al. (2004) have shown that FS neurons have Class 2 excitability <strong>in</strong> the sensethat their frequency-current (F-I) relation has a discont<strong>in</strong>uity around 20 Hz. Whenstimulated with barely superthreshold current, such neurons exhibit irregular fir<strong>in</strong>grandomly switch<strong>in</strong>g between spik<strong>in</strong>g and fast subthreshold oscillatory mode (Kubotaand Kawaguchi 1999, Tateno et al. 2004).The absence of spike frequency adaptation <strong>in</strong> FS neurons is mostly due to the fastK + current that activates dur<strong>in</strong>g the spike, produces deep AHP, completely de<strong>in</strong>activatesNa + current, and thereby facilitates the generation of the next spike. Block<strong>in</strong>gthe K + current by TEA (Erisir et al. 1999) removes AHP, leaves residual <strong>in</strong>activationof the Na + current and slows down the spik<strong>in</strong>g, essentially transform<strong>in</strong>g the FS fir<strong>in</strong>gpattern <strong>in</strong>to LTS.The existence of fast subthreshold oscillations of membrane potential suggest thatthe rest<strong>in</strong>g state of the FS neurons is near Andronov-Hopf bifurcation. Stutter<strong>in</strong>gbehavior at the threshold currents po<strong>in</strong>ts to the co-existence of rest<strong>in</strong>g and spik<strong>in</strong>gstates, as <strong>in</strong> Fig. 8.16, and suggests that the bifurcation is of the subcritical type.However, FS neurons do not fire post-<strong>in</strong>hibitory (rebound) spikes — the feature usedto dist<strong>in</strong>guish them experimentally from LTS types. Thus, we cannot use the simplemodel (8.5, 8.6) <strong>in</strong> its present form to simulate FS neurons because the model withl<strong>in</strong>ear slow nullcl<strong>in</strong>e would fire rebound spikes accord<strong>in</strong>g to the mechanism depicted <strong>in</strong>Fig. 8.26. In addition, the simple model has a non-monotone I-V relation, whereas FS

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