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Dynamical Systems in Neuroscience:

Dynamical Systems in Neuroscience:

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8 Introductionconcepts of dynamical systems theory. The reader does not have to follow all the detailsof this section because the concepts are expla<strong>in</strong>ed <strong>in</strong> a greater detail <strong>in</strong> subsequentchapters.A dynamical system consists of a set of variables that describe its state and alaw that describes the evolution of the state variables with time, i.e., how the stateof the system <strong>in</strong> the next moment of time depends on the <strong>in</strong>put and its state <strong>in</strong> theprevious moment of time. The Hodgk<strong>in</strong>-Huxley model is a four-dimensional dynamicalsystem because its state is determ<strong>in</strong>ed uniquely by the membrane potential, V , and socalled gat<strong>in</strong>g variables n, m and h for persistent K + and transient Na + currents. Theevolution law is given by a four-dimensional system of ord<strong>in</strong>ary differential equations.Typically, all variables describ<strong>in</strong>g neuronal dynamics can be classified <strong>in</strong>to fourclasses, accord<strong>in</strong>g to their function and the time scale:1. Membrane potential.2. Excitation variables, such as activation of Na + current. This variables are responsiblefor the upstroke of the spike.3. Recovery variables, such as <strong>in</strong>activation of Na + current and activation of fast K +current. This variables are responsible for the repolarization (downstroke) of thespike.4. Adaptation variables, such as activation of slow voltage- or Ca 2+ -dependent currents.This variables build up dur<strong>in</strong>g prolonged spik<strong>in</strong>g and can affect excitabilityon the long run.The Hodgk<strong>in</strong>-Huxley model does not have variables of the fourth type, but manyneuronal models do, especially those exhibit<strong>in</strong>g burst<strong>in</strong>g dynamics.1.2.1 Phase portraitsThe power of the dynamical systems approach to neuroscience, as well as to manyother sciences, is that we can tell someth<strong>in</strong>g, or many th<strong>in</strong>gs, about a system withouteven know<strong>in</strong>g all the details that govern the system evolution. We do not even useequations to do that! Some may even wonder why we call it a mathematical theory.As a start, let us consider a quiescent neuron whose membrane potential is rest<strong>in</strong>g.From the dynamical systems po<strong>in</strong>t of view, there are no changes of the statevariables of such a neuron, hence it is at an equilibrium po<strong>in</strong>t. All the <strong>in</strong>ward currentsthat depolarize the neuron are balanced, or equilibrated, by the outward currents thathyperpolarize it. If the neuron rema<strong>in</strong>s quiescent despite small disturbances and membranenoise, as <strong>in</strong> Fig. 1.9a, top, then we conclude that the equilibrium is stable. Isn’tit amaz<strong>in</strong>g that we can make such a conclusion without know<strong>in</strong>g the equations thatdescribe the neuron’s dynamics? We do not even know the number of variables neededto describe the neuron; it could be <strong>in</strong>f<strong>in</strong>ite, for all we care.

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