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Dynamical Systems in Neuroscience:

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Simple Models 317figure are v r = −60 mV and v t = −50 mV. The value p = 1.6 results <strong>in</strong> 40 pA rheobasecurrent and 60 MΩ <strong>in</strong>put resistance, and the membrane capacitance C = 200 pF givesthe right current-frequency (F-I) relationship. Thus, <strong>in</strong> the tonic mode, our model isessentially the quadratic <strong>in</strong>tegrate-and-fire neuron 200 ˙v = 1.6(v + 60)(v + 50) + I withthe after-spike reset from +35 mV to −60 mV.To model slow Ca 2+ dynamics <strong>in</strong> the burst mode, we assume that hyperpolarizationsbelow the Ca 2+ <strong>in</strong>activation threshold of −65 mV decrease u, thereby creat<strong>in</strong>g <strong>in</strong>wardcurrent. In the l<strong>in</strong>ear case, we take ˙u = 0.01{b(v + 65) − u} with b = 0 when v ≥ −65and b = 15 when v < −65, result<strong>in</strong>g <strong>in</strong> the piecewise l<strong>in</strong>ear u-nullcl<strong>in</strong>e depicted <strong>in</strong>Fig. 8.31, bottom. Prolonged hyperpolarization below −65 mV decreases u and movesthe trajectory outside the attraction doma<strong>in</strong> of the rest<strong>in</strong>g state (shaded region <strong>in</strong> thefigure). Upon release from the hyperpolarization, the model fires a rebound burst ofspikes, variable u → 0 reflect<strong>in</strong>g <strong>in</strong>activation of Ca 2+ , and the trajectory reenters theattraction doma<strong>in</strong> of the rest<strong>in</strong>g state. Steps of depolarized current produce reboundbursts followed by tonic spik<strong>in</strong>g with adapt<strong>in</strong>g frequency. A better quantitative agreementwith TC record<strong>in</strong>gs can be achieved when two slow variables, u 1 and u 2 , areused.8.3.2 Reticular thalamic nucleus (RTN) neuronsReticular thalamic nucleus (RTN) neurons provide reciprocal <strong>in</strong>hibition to TC relayneurons. RTN and TC cells are similar <strong>in</strong> the sense that they have two fir<strong>in</strong>g modes,illustrated <strong>in</strong> Fig. 8.32: They fire tra<strong>in</strong>s of s<strong>in</strong>gle spikes follow<strong>in</strong>g stimulation fromrest<strong>in</strong>g or depolarized potentials <strong>in</strong> the tonic mode, and rebound bursts upon releasefrom hyperpolarized potentials <strong>in</strong> the burst mode.The parameters of the simple model <strong>in</strong> Fig. 8.32 are adjusted to match the <strong>in</strong> vitrorecord<strong>in</strong>g of the RTN cell <strong>in</strong> the figure, and they differ from the parameters of the TCmodel cell. Nevertheless, the mechanism of rebound burst<strong>in</strong>g of RTN neuron is thesame as that of the TC neuron <strong>in</strong> Fig. 8.31, bottom. In contrast, the tonic mode of fir<strong>in</strong>gis different. S<strong>in</strong>ce b > 0, the model neuron is near the transition from an <strong>in</strong>tegratorto a resonator; It can fire transient spikes followed by slow subthreshold oscillationsof membrane potential; It has co-existence of stable rest<strong>in</strong>g and spik<strong>in</strong>g states, withthe bifurcation diagram similar to the one <strong>in</strong> Fig. 8.15, and it can stutter and produceclustered spikes when stimulated with barely threshold current. Interest<strong>in</strong>gly, similarbehavior of TC neurons was reported by Pirchio et al. (1997), Pedroarena and Ll<strong>in</strong>as(1997) and Li et al. (2003). We will return to the issue of subthreshold oscillations andstutter<strong>in</strong>g spik<strong>in</strong>g when we consider stellate cells of entorh<strong>in</strong>al cortex <strong>in</strong> Sect. 8.4.4.8.3.3 Thalamic <strong>in</strong>terneuronsIn contrast to TC and RTN neurons, thalamic <strong>in</strong>terneurons do not have a prom<strong>in</strong>entburst mode, though they can fire rebound spikes upon release from hyperpolarization(Pape and McCormick 1995). They have action potentials with short duration, and

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