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

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<strong>EEG</strong> segment D e (min) D 2 1<br />

0 ; 8 sec 0:0195 8 4:30 4:6<br />

21 ; 29 sec 0:0156 13 2:60 4:0<br />

29 ; 37 sec 0:0156 10 2:50 4:0<br />

37 ; 44 sec 0:0156 11 2:05 3:5<br />

44 ; 52 sec 0:0156 13 2:15 3:0<br />

Table 5: Optimal value <strong>of</strong> time lag (insec ), minimum embedding dimension D (min)<br />

e ,<br />

Correlation Dimension (D 2 ), <strong>and</strong> maximum Lyapunov exponent ( 1 ) for the stationary<br />

<strong>EEG</strong> segments (Data-set size: N = 2048 see text).<br />

showed in table 5, it can be concluded that the dynamical behavior was more regular<br />

during the seizure.<br />

Summarizing, we found a good evidence that during the epileptic seizure there is<br />

a transition from a complex to a simple dynamical behavior. Furthermore, this result<br />

yields insights with respect to the theory <strong>of</strong> how epileptic seizures occur (i.e.<br />

synchronization <strong>of</strong> the disordered background <strong>EEG</strong> activity).<br />

as a<br />

5.7 Conclusion<br />

Deterministic chaos theory gives an alternative new type <strong>of</strong> <strong>analysis</strong> compared with<br />

the ones given by the traditional <strong>methods</strong>. However, the application <strong>of</strong> chaos <strong>methods</strong>,<br />

should be done with care in order to avoid misleading results. In this way a right election<br />

<strong>of</strong> parameters required for the calculations is critical.<br />

Chaos <strong>analysis</strong> has several prerequisites, some <strong>of</strong> them making impossible its application<br />

to the study <strong>of</strong> <strong>EEG</strong> <strong>signals</strong>. One <strong>of</strong> these prerequisites is the availability <strong>of</strong><br />

long data recordings but on the other h<strong>and</strong>, data must be stationary. Consequently,<br />

chaos <strong>analysis</strong> cannot be applied in nonstationary short data recordings as in the case <strong>of</strong><br />

event-related potentials. In these types <strong>of</strong> series, the dynamics <strong>of</strong> the system is changing<br />

completely in fractions <strong>of</strong> a second due to the eect <strong>of</strong> the stimulus <strong>and</strong> therefore, it has<br />

no sense to dene an attractor <strong>and</strong> to calculate any metric invariant from it.<br />

Since <strong>methods</strong> for calculation <strong>of</strong> D 2 <strong>and</strong> 1 were developed for ideal <strong>signals</strong> (i.e.<br />

innite, noise-free <strong>and</strong> stationary), then, due to the complex structure <strong>of</strong> the <strong>EEG</strong>s,<br />

results should be considered <strong>of</strong> relative relevance <strong>and</strong>, as suggested by Pritchard <strong>and</strong><br />

Duke (1992), is more realistic to talk about Dimensionality instead <strong>of</strong> Correlation Dimension.<br />

By using this view, several groups reported changes in D 2 <strong>and</strong> 1 values in<br />

dierent brain states <strong>and</strong> pathologies. Nevertheless, these measures seem not to be suit-<br />

84

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