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Dynamical Systems in Neuroscience:

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Excitability 265modelI K(M)I Na,p +I K -modelC ˙V{ }} { { }} {= I −g L (V −E L )−g Na m ∞ (V )(V −E Na )−g K n(V −E K ) − g M n M (V −E K )ṅ = (n ∞ (V ) − n)/τ(V )ṅ M = (n ∞,M (V ) − n M )/τ M (V ) (slow K + M-current)(7.1)whose excitable and spik<strong>in</strong>g properties are similar to those of the I Na,p +I K -submodelon a short time scale. However, the long-term behavior of the two models may be quitedifferent. For example, the K + M-current may result <strong>in</strong> frequency adaptation dur<strong>in</strong>g along tra<strong>in</strong> of action potentials. It can change the shape of the I-V relation of the modeland result <strong>in</strong> slow oscillations, post-<strong>in</strong>hibitory spikes, and other resonator propertieseven when the I Na,p +I K -submodel is an <strong>in</strong>tegrator. All these <strong>in</strong>terest<strong>in</strong>g phenomenaare discussed <strong>in</strong> this section.In general, models hav<strong>in</strong>g fast and slow currents, such as (7.1), can be written <strong>in</strong>the fast-slow formẋ = f(x, u) (fast spik<strong>in</strong>g),˙u = µg(x, u) (slow modulation),(7.2)where the vector x ∈ R m describes fast variables responsible for spik<strong>in</strong>g. It <strong>in</strong>cludes themembrane potential V , activation and <strong>in</strong>activation gat<strong>in</strong>g variables for fast currents,etc. The vector u ∈ R k describes relatively slow variables that modulate fast spik<strong>in</strong>g,e.g., the gat<strong>in</strong>g variable of a slow K + current, the <strong>in</strong>tracellular concentration of Ca 2+ions, etc. The small parameter µ represents the ratio of time scales between spik<strong>in</strong>gand its modulation. Such systems often result <strong>in</strong> burst<strong>in</strong>g activity, and we study them<strong>in</strong> detail <strong>in</strong> Chap. 9.7.3.1 Spike-frequency modulationSlow currents can modulate the <strong>in</strong>stantaneous spik<strong>in</strong>g frequency of a long tra<strong>in</strong> ofaction potentials, as we illustrate <strong>in</strong> Fig. 7.43a us<strong>in</strong>g record<strong>in</strong>gs of a layer 5 pyramidalneuron. The neuron generates a tra<strong>in</strong> of spikes with <strong>in</strong>creas<strong>in</strong>g <strong>in</strong>terspike <strong>in</strong>terval (see<strong>in</strong>set <strong>in</strong> the figure) <strong>in</strong> response to a long pulse of <strong>in</strong>jected dc-current. In Fig. 7.43bwe plot the <strong>in</strong>stantaneous <strong>in</strong>terspike <strong>in</strong>tervals T i , i.e., the time <strong>in</strong>tervals between spikesnumber i and i + 1, as a function of the magnitude of <strong>in</strong>jected current I. Notice thatT i (I) < T i+1 (I), mean<strong>in</strong>g that the <strong>in</strong>tervals <strong>in</strong>crease with each spike. The functionT 0 (I) describes the latency of the first spike, and T ∞ (I) describes the steady-state(asymptotic) <strong>in</strong>terspike period. The <strong>in</strong>stantaneous frequencies are def<strong>in</strong>ed as F i (I) =1000/T i (I) (Hz), and they are depicted <strong>in</strong> Fig. 7.43c. S<strong>in</strong>ce the neuron is Class 1excitable, the F-I curves are square-root parabolas (see Sect. 6.1.2). Notice that F 0 (I)is nearly a straight l<strong>in</strong>e, probably reflect<strong>in</strong>g the passive charg<strong>in</strong>g of the dendritic tree.Decrease of the <strong>in</strong>stantaneous spik<strong>in</strong>g frequency, as <strong>in</strong> Fig. 7.43, is referred to asspike-frequency adaptation. This is a prom<strong>in</strong>ent feature of cortical pyramidal neuronsof the regular spik<strong>in</strong>g (RS) type (Connors and Gutnick 1990), as well as many

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