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Dynamical Systems in Neuroscience:

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314 Simple Models(1) fast oscillations result<strong>in</strong>g from the <strong>in</strong>terplay of amplify<strong>in</strong>g and resonant currents,and (2) slow ramp result<strong>in</strong>g from the slow k<strong>in</strong>etic of an amplify<strong>in</strong>g variable, such asslow <strong>in</strong>activation of an outward current (e.g., K + A-current) or slow activation of an<strong>in</strong>ward current, or both. In addition, the ramp could result from the slow charg<strong>in</strong>g ofthe dendritic compartment of the neuron.The exact mechanism responsible for the slow ramp <strong>in</strong> LS neurons is not known atpresent. Fortunately, we do not need to know the mechanism to simulate LS neuronsus<strong>in</strong>g the simple model approach. Indeed, simple models with passive dendrites areequivalent to simple models with l<strong>in</strong>ear amplify<strong>in</strong>g currents. For example, the model <strong>in</strong>Fig. 8.28 consists of a 2-dimensional system (v, u) responsible for the spike-generationmechanism at the soma and a l<strong>in</strong>ear equation for the passive dendritic compartmentv d .When stimulated with the threshold current, i.e., just above the neuronal rheobase,LS neurons often exhibit stutter<strong>in</strong>g behavior seen <strong>in</strong> Fig. 8.28, middle. Subthresholdoscillations, voltage ramps, and stutter<strong>in</strong>g are consistent with the follow<strong>in</strong>g geometricalpicture: Abrupt onset of stimulation evokes a transient spike followed by brief hyperpolarizationand then susta<strong>in</strong>ed depolarization. While depolarized, the fast subsystemaffects the slow subsystem, e.g., slowly charges the dendritic tree or slowly <strong>in</strong>activatesthe K + current. In any case, there is a slow decrease of the outward current, or equivalently,slow <strong>in</strong>crease of the <strong>in</strong>ward current that drives the fast subsystem throughthe subcritical Andronov-Hopf bifurcation. Because of the co-existence of rest<strong>in</strong>g andspik<strong>in</strong>g states near the bifurcation, the neuron can be switched from one state to theother by the membrane noise. Once the bifurcation is passed, the neuron is <strong>in</strong> thetonic spik<strong>in</strong>g mode. Overall, LS neurons can be thought of as be<strong>in</strong>g FS neurons with aslow subsystem that damps any abrupt changes, delays the onset of spik<strong>in</strong>g, and slowsdown its frequency.8.2.8 Diversity of <strong>in</strong>hibitory <strong>in</strong>terneuronsIn contrast to excitatory neocortical pyramidal neurons, which have stereotypical morphologicaland electrophysiological classes (RS, IB, CH), <strong>in</strong>hibitory neocortical <strong>in</strong>terneuronshave wildly diverse classes with various fir<strong>in</strong>g patters that cannot be classifiedas FS, LTS, or LS. Markram et al. (2004) reviewed recent results on the relationshipbetween electrophysiology, pharmacology, immunohistochemistry and gene-expressionpatterns of <strong>in</strong>hibitory <strong>in</strong>terneurons. An extreme <strong>in</strong>terpretation of their f<strong>in</strong>d<strong>in</strong>gs is thatthere is a cont<strong>in</strong>uum of different classes of <strong>in</strong>terneurons rather than a set of 3 classes.Figure 8.29 summarizes five of the most ubiquitous groups <strong>in</strong> the cont<strong>in</strong>uum:• (NAC) non-accommodat<strong>in</strong>g <strong>in</strong>terneurons fire repetitively without frequency adaptation<strong>in</strong> response to a wide range of susta<strong>in</strong>ed somatic current <strong>in</strong>jections. ManyFS and LS neurons are of this type.• (AC) accommodat<strong>in</strong>g <strong>in</strong>terneurons fire repetitively with frequency adaptationand therefore do not reach high fir<strong>in</strong>g rates of NAC neurons. Some FS and LS

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