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Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

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58 One-Dimensional <strong>Systems</strong><strong>in</strong>wardcurrentsoutwardgat<strong>in</strong>gactivation, mdepolarization+ +<strong>in</strong>crease+ <strong>in</strong> m<strong>in</strong>wardcurrent+depolarization- +<strong>in</strong>crease- <strong>in</strong> moutwardcurrent+<strong>in</strong>activation, h-hyperpolarization- +<strong>in</strong>crease<strong>in</strong> h<strong>in</strong>wardcurrent+-negative feedback,resonant current +hyperpolarization+ +<strong>in</strong>crease+ <strong>in</strong> houtwardcurrent+positive feedback,amplify<strong>in</strong>g currentFigure 3.4: Feedback loopsbetween voltage and gat<strong>in</strong>gvariables <strong>in</strong> the four modelspresented above; see also Fig. 5.2.throughout the rest of this chapter. (Some biologists refer to transient Na + currentswith very slow <strong>in</strong>activation as be<strong>in</strong>g persistent, s<strong>in</strong>ce the current does not change muchon the time scale of 1 sec.) We obta<strong>in</strong> the experimental parameter valuesC = 10 µF , I = 0 pA , g L = 19 mS , E L = −67 mV ,g Na = 74 mS , V 1/2 = 1.5 mV , k = 16 mV , E Na = 60 mVus<strong>in</strong>g whole-cell patch clamp record<strong>in</strong>gs of a layer 5 pyramidal neuron <strong>in</strong> the visualcortex of a rat at room temperature. We prove <strong>in</strong> Ex. 3.3.8 and illustrate <strong>in</strong> Fig. 3.15that the model approximates the action potential upstroke dynamics of this neuron.The model’s I-V relation, I(V ), is depicted <strong>in</strong> Fig. 3.5a. Due to the negativeconductance region <strong>in</strong> the I-V curve, this one-dimensional model can exhibit a numberof <strong>in</strong>terest<strong>in</strong>g non-l<strong>in</strong>ear phenomena, such as bistability, i.e. co-existence of rest<strong>in</strong>gand excited states. From a mathematical po<strong>in</strong>t of view, bistability occurs becausethe right-hand side function <strong>in</strong> the differential equation (3.5), depicted <strong>in</strong> Fig. 3.5b,is not monotonic. In Fig. 3.6 we depict typical voltage time courses of the model(3.5) with two values of <strong>in</strong>jected dc-current I and 16 different <strong>in</strong>itial conditions. Thequalitative behavior <strong>in</strong> Fig. 3.6a is clearly bistable: depend<strong>in</strong>g on the <strong>in</strong>itial condition,the trajectory of the membrane potential goes either up to the excited state or downto the rest<strong>in</strong>g state. In contrast, the behavior <strong>in</strong> Fig. 3.6b is monostable, s<strong>in</strong>ce therest<strong>in</strong>g state does not exist. The goal of the dynamical system theory reviewed <strong>in</strong> thischapter is to understand why and how the behavior depends on the <strong>in</strong>itial conditionsand the parameters of the system.3.2 <strong>Dynamical</strong> <strong>Systems</strong>In general, dynamical systems can be cont<strong>in</strong>uous or discrete, depend<strong>in</strong>g on whetherthey are described by differential or difference equations. Cont<strong>in</strong>uous one-dimensional

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