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Quantitative analysis of EEG signals: Time-frequency methods and ...

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5 Deterministic Chaos<br />

5.1 Introduction<br />

In the previous chapters I described the application <strong>of</strong> several time-<strong>frequency</strong> <strong>methods</strong><br />

to the <strong>analysis</strong> <strong>of</strong> brain <strong>signals</strong>. Since these <strong>methods</strong> are linear, a completely dierent<br />

approach canbeachieved by applying the concepts <strong>of</strong> non-linear dynamics, also known<br />

as Deterministic Chaos theory.<br />

Chaotic systems have an apparently noisy behavior but are in fact ruled by deterministic<br />

laws. They are characterized by their sensibility on initial conditions. That<br />

means, similar initial conditions give completely dierent outcomes after some time.<br />

Since chaotic <strong>signals</strong> look like noise <strong>and</strong> furthermore, since they also have a broadb<strong>and</strong><br />

<strong>frequency</strong> spectrum, linear approaches as the ones described in the previous sections<br />

are sometimes not suitable for their study. Several <strong>methods</strong> were developed in order<br />

to calculate the degree <strong>of</strong> determinism (or r<strong>and</strong>om nature), complexity, chaoticity, etc.<br />

<strong>of</strong> these <strong>signals</strong>. Among these, the Correlation Dimension, Lyapunov Exponents <strong>and</strong><br />

Kolmogorov Entropy have been the most popular. In this chapter I will give a mathematical<br />

background <strong>of</strong> these <strong>methods</strong> <strong>and</strong> then I will describe their application to the<br />

study <strong>of</strong> <strong>EEG</strong> <strong>signals</strong>.<br />

The chapter is organized as follows. After a brief denition <strong>of</strong> the basic concepts<br />

related with chaos, the mathematical background for the calculation <strong>of</strong> the Correlation<br />

Dimension <strong>and</strong> Lyapunov Exponents will be described. In section x5.2.4, I will remark<br />

some problems in the selection <strong>of</strong> computational parameters. One <strong>of</strong> these problems is<br />

the stationarity <strong>of</strong> the signal to be studied. In Section x5.3, I will describe a criterion<br />

based on weak stationarity (Blanco et al., 1995a). In section x5.4, I will give a brief<br />

review <strong>of</strong> previous results <strong>of</strong> chaos <strong>analysis</strong> <strong>of</strong> <strong>EEG</strong> <strong>signals</strong>. In sections x5.5 <strong>and</strong> x5.6,<br />

I will show the application <strong>of</strong> Chaos <strong>methods</strong> to scalp normal <strong>EEG</strong> recordings <strong>and</strong> to<br />

intracranially recorded Gr<strong>and</strong> Mal seizures (Blanco et al., 1995a,b, 1996a). Finally in<br />

section x5.7, I will discuss about the applicability <strong>and</strong>results <strong>of</strong> chaos <strong>analysis</strong> to <strong>EEG</strong><br />

<strong>signals</strong>.<br />

5.2 Theoretical Background<br />

5.2.1 Basic concepts<br />

Phase space: It is a common practice in physics to represent the evolution <strong>of</strong> a system<br />

in phase spaces. For example, in mechanics,itisvery useful to represent the movement<br />

<strong>of</strong> a system as a pendulum by plotting the position vs. the velocity or more generally,<br />

68

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