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performed. On one h<strong>and</strong>, must be large enough in order to give a reliable statistic<br />

<strong>and</strong> on the other h<strong>and</strong> if it is too large, it will not be possible to observe fast<br />

changes.<br />

2. The mean <strong>and</strong> variance for each bin were calculated, <strong>and</strong> zones in which their<br />

values do not have signicant changes (e.g. less than 20%) were selected.<br />

3. Finally, the corresponding histogram for this zone was constructed, <strong>and</strong> the normality<br />

<strong>of</strong> the obtained distribution was veried.<br />

I would like to remark that although the above criterion is arbitrary <strong>and</strong> does not<br />

prove stationarity 7 , it was very useful as a rst approximation in order to select <strong>EEG</strong><br />

data segments to work with, or to reject others with clear non stationary behavior.<br />

However, I would like to stress that in general elaborated statistical criteria can be<br />

hardly fullled by <strong>EEG</strong> <strong>signals</strong>. For a more complete discussion about stationarity<br />

related with the application <strong>of</strong> Chaos <strong>methods</strong>, see for example Schreiber (1997).<br />

Eckman et al. (1987) presented another approach to the problem <strong>of</strong> stationarity by<br />

using the so called recurrence plots. Recurrence plots are based on distance calculations<br />

in the phase space. After a phase space reconstruction, the Euclidean distance between<br />

the embedding vectors (lets say N in total) is calculated. Then, an NxN plot is performed<br />

in the following way: for each pair <strong>of</strong> embedding vectors (i j) (i represented in<br />

the horizontal axis <strong>and</strong> j in the vertical axis) a point is plotted if its distance is less<br />

than a certain value r. Stationary <strong>signals</strong> will be characterized by homogeneous plots<br />

<strong>and</strong> non-stationary <strong>signals</strong> will show inhomogeneities due to varying features <strong>of</strong> the embedding<br />

vectors in the phase space. As an example, Fig. 25 shows the recurrence plot<br />

<strong>of</strong> an stationary one minute <strong>EEG</strong> signal (see Blanco et al., 1995a).<br />

Recurrence plots give an elegant representation <strong>of</strong> the stationarity <strong>of</strong> the signal, but<br />

in many occasions their interpretation is subjective <strong>and</strong> further <strong>analysis</strong> is required.<br />

5.4 Short review <strong>of</strong> Chaos <strong>analysis</strong> <strong>of</strong> <strong>EEG</strong> <strong>signals</strong><br />

5.4.1 Correlation Dimension<br />

Since the pioneering work <strong>of</strong> Babloyantz <strong>and</strong> coworkers (Babloyantz, 1985), several<br />

groups started to study the dynamics <strong>of</strong> the brain activity by reconstructing the trajectory<br />

<strong>of</strong> the system in the phase space <strong>and</strong> by calculating parameters as the Correlation<br />

Dimension (D 2 ). Low D 2 values correspond to simple systems <strong>and</strong> high D 2 values to<br />

7 Autocorrelation function is not checked, <strong>and</strong> the choice <strong>of</strong> what is considered as stable mean <strong>and</strong><br />

variances is in fact arbitrary.<br />

75

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