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Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

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Excitability 23720 mV50 msaverage fir<strong>in</strong>g frequency, Hz25020015010050F-I curveClass 2 excitabilitynoisewithwithout noise00 500 1000 1500<strong>in</strong>jected dc-current, I (pA)Figure 7.12: Examples of noise-<strong>in</strong>duced low-frequency fir<strong>in</strong>gs of Class 2 excitable system.The F-I curve may look like the one for Class 1 excitability. Shown are record<strong>in</strong>gsof bra<strong>in</strong>stem mesV neuron.neuro-computational property: Bistable systems can be switched from one state tothe other by an appropriately timed brief stimulus. R<strong>in</strong>zel (1978) predicted such abehavior <strong>in</strong> the Hodgk<strong>in</strong>-Huxley model, and then bistability and hysteresis were foundexperimentally <strong>in</strong> the squid axon (Guttman et al. 1980). What was really surpris<strong>in</strong>gfor many neuroscientists is that neurons can be switched from repetitive spik<strong>in</strong>g torest<strong>in</strong>g by brief depolariz<strong>in</strong>g shock-stimuli.This phenomenon is illustrated <strong>in</strong> Fig. 7.11. Each shaded area <strong>in</strong> the figure denotesthe attraction doma<strong>in</strong> of a spik<strong>in</strong>g limit cycle attractor. Obviously, the state of therest<strong>in</strong>g neuron must be pushed <strong>in</strong>to the shaded area to <strong>in</strong>itiate periodic spik<strong>in</strong>g. Similarly,the state of the periodically spik<strong>in</strong>g neuron must be pushed out of the shadedarea to stop the spik<strong>in</strong>g. As the arrows <strong>in</strong> the figure <strong>in</strong>dicate, both excitatory and <strong>in</strong>hibitorystimuli can do that, depend<strong>in</strong>g on their tim<strong>in</strong>g relative to the phase of spik<strong>in</strong>goscillation. This protocol can be used to test bistability experimentally.Bistable behavior reveals itself <strong>in</strong>directly when a neuron is kept close to the bifurcation,e.g., when the <strong>in</strong>jected dc-current is just below the rheobase. Noisy perturbationscan switch the neuron from rest<strong>in</strong>g to spik<strong>in</strong>g states thereby creat<strong>in</strong>g an irregular spiketra<strong>in</strong> consist<strong>in</strong>g of short bursts of spikes. Such stutter<strong>in</strong>g spik<strong>in</strong>g have been observed<strong>in</strong> many neurons, <strong>in</strong>clud<strong>in</strong>g some regular spik<strong>in</strong>g (RS) and fast spik<strong>in</strong>g (FS) neocorticalneurons, as we discuss <strong>in</strong> Chap. 8. The mean fir<strong>in</strong>g frequency dur<strong>in</strong>g stutter<strong>in</strong>gis proportional to the amplitude of the <strong>in</strong>jected current and it can be quite low evenfor Class 2 excitable system, as we illustrate <strong>in</strong> Fig. 7.12. Thus, caution should be

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