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Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

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286 Simple Modelsbe an <strong>in</strong>tegrator or a resonator, as we illustrate <strong>in</strong> Fig. 8.5. The parameters c and ddo not affect steady-state subthreshold behavior. Instead, they take <strong>in</strong>to account theaction of high-threshold voltage-gated currents activated dur<strong>in</strong>g the spike and affectonly the after-spike transient behavior. If there are many currents with diverse timescales, then u, a, b, and d are vectors, and the equation (8.3) conta<strong>in</strong>s ∑ u <strong>in</strong>stead ofu.The simple model may be treated as quadratic <strong>in</strong>tegrate-and-fire neuron with adaptation<strong>in</strong> the simplest case b = 0. When b < 0, the model can be treated as quadratic<strong>in</strong>tegrate-and-fire neuron with a passive dendritic compartment (see Ex. 10). Whenb > 0, the connection to the quadratic <strong>in</strong>tegrate-and-fire neuron is lost, and the simplemodel represents a novel class of spik<strong>in</strong>g models.In the rest of this chapter we tune the simple model to reproduce spik<strong>in</strong>g andburst<strong>in</strong>g behavior of many known types of neurons. It is convenient to use it <strong>in</strong> theformC ˙v = k(v − v r )(v − v t ) − u + I if v ≥ v peak , then (8.5)˙u = a{b(v − v r ) − u} v ← c, u ← u + d (8.6)where v is the membrane potential, u is the recovery current, C is the membranecapacitance, v r is the rest<strong>in</strong>g membrane potential, and v t is the <strong>in</strong>stantaneous thresholdpotential. Though it looks like the model has ten parameters, but it is equivalentto (8.3,8.4) and hence it has only four <strong>in</strong>dependent parameters. As we described <strong>in</strong>Sect. 5.2.4, the parameters k and b can be found know<strong>in</strong>g the neuron’s rheobase and<strong>in</strong>put resistance. The sum of all slow currents that modulate the spike-generationmechanism are comb<strong>in</strong>ed <strong>in</strong> the phenomenological variable u with outward currentstaken with the plus sign.The sign of b determ<strong>in</strong>es whether u is an amplify<strong>in</strong>g (b < 0) or a resonant (b > 0)variable. In the latter case, the neuron sags <strong>in</strong> response to hyperpolarized pulses ofcurrent, peaks <strong>in</strong> response to depolarized subthreshold pulses, and produces rebound(post-<strong>in</strong>hibitory) responses. The recovery time constant is a. The spike cut-off value isv peak , and the voltage reset value is c. The parameter d describes the total amount ofoutward m<strong>in</strong>us <strong>in</strong>ward currents activated dur<strong>in</strong>g the spike and affect<strong>in</strong>g the after-spikebehavior. All these parameters can be easily fit to any particular neuron type, as weshow <strong>in</strong> subsequent sections.Implementation and phase portraitThe follow<strong>in</strong>g MATLAB code simulates the model and produces Fig. 8.6a.C=100; vr=-60; vt=-40; k=0.7;a=0.03; b=-2; c=-50; d=100;vpeak=35;T=1000; tau=1;n=round(T/tau);% parameters used for RS% neocortical pyramidal neurons% spike cutoff% time span and step (ms)% number of simulation steps

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