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Dynamical Systems in Neuroscience:

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Excitability 2592) Neuronal responses become less sensitive to noise, s<strong>in</strong>ce only prolong <strong>in</strong>puts cancause spikes.Interest<strong>in</strong>gly, but resonators do not exhibit long latencies even though there is aneighborhood where the vector field is small and even zero, as we show <strong>in</strong> Fig. 7.35,right. When the current pulse is applied, the V -nullcl<strong>in</strong>e moves up and the voltagevariable accelerates. However, it misses the shaded neighborhood, and the neuronfires an action potential practically without any latency. In Ex. 5 we discuss whysome models near Andronov-Hopf bifurcation, <strong>in</strong>clud<strong>in</strong>g the Hodgk<strong>in</strong>-Huxley model<strong>in</strong> Fig. 7.26, seem to exhibit small but noticeable latencies. In Sect. 8.2.7 we showthat latencies could result from slow charg<strong>in</strong>g of the dendritic compartment. In thiscase, <strong>in</strong>tegrators neurons exhibit latency to the first spike, while resonator neurons mayexhibit latency to the second spike (after they fire the first, transient spike).7.2.10 Flipp<strong>in</strong>g from an <strong>in</strong>tegrator to a resonatorOne of the reasons we provided so many examples of neuronal systems <strong>in</strong> Chap. 5is to conv<strong>in</strong>ce the reader that all neuronal models can exhibit both saddle-node andAndronov-Hopf bifurcations, depend<strong>in</strong>g on the parameters describ<strong>in</strong>g the ionic currents.S<strong>in</strong>ce the k<strong>in</strong>etics of ionic currents <strong>in</strong> neurons could change dur<strong>in</strong>g developmentor due to the action of neuromodulators, neurons could switch from be<strong>in</strong>g <strong>in</strong>tegratorsto be<strong>in</strong>g resonators.In Fig. 7.36 we illustrate an <strong>in</strong>terest<strong>in</strong>g case: Mitral cells <strong>in</strong> rat ma<strong>in</strong> olfactory bulbcan exhibit bistability of membrane potential. That is, the potential can be <strong>in</strong> twostates: down-state around −60 mV, and up-state around −50 mV (Heyward et al.2001). A sufficiently strong synaptic <strong>in</strong>put can shift the cell between these states <strong>in</strong>a matter of milliseconds. An amaz<strong>in</strong>g observation is that the down-state is a stablenode and the up-state is a stable focus, as we illustrate at the bottom of the figure andstudy <strong>in</strong> detail <strong>in</strong> Sect. 8.4.5. As a result, mitral cells can be quickly switched frombe<strong>in</strong>g <strong>in</strong>tegrators to be<strong>in</strong>g resonators by synaptic <strong>in</strong>put.Similar phenomenon was observed <strong>in</strong> a cerebella Purk<strong>in</strong>je neuron <strong>in</strong> Fig. 7.37. It actsas an <strong>in</strong>tegrator <strong>in</strong> the down-state, but has fast (> 100 Hz) subthreshold oscillations<strong>in</strong> the up-state, and hence can act as a resonator.Cortical pyramidal neurons can also exhibit up- and down-states, though the statesare not <strong>in</strong>tr<strong>in</strong>sic, but <strong>in</strong>duced by the synaptic activity. S<strong>in</strong>ce the neurons are depolarized<strong>in</strong> the up-state, there is an <strong>in</strong>terest<strong>in</strong>g possibility that fast K + conductancesare partially activated and the fast Na + <strong>in</strong>activation gate is partially <strong>in</strong>activated sothat the neuron exhibits fast subthreshold oscillations and acts as a resonator. Thatis, <strong>in</strong>tegrator neurons could switch to the resonator mode when <strong>in</strong> the up-state. Thispossibility needs to be tested experimentally.

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