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