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

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ENTROPY<br />

Thermodynamics<br />

Signal <strong>analysis</strong><br />

Situation A<br />

Order<br />

=<br />

low entropy<br />

Fourier<br />

Situation B<br />

Disorder<br />

=<br />

high entropy<br />

Fourier<br />

Figure 30: Entropy in thermodynamics <strong>and</strong> in signal <strong>analysis</strong>.<br />

These disadvantages <strong>of</strong> the Fourier Transform are partially resolved by using the<br />

Gabor Transform (Powell <strong>and</strong> Percival already dened a time evolving entropy from<br />

the Gabor Transform by using a Hanning window). Nevertheless, as already discused in<br />

previous chapters, the selection <strong>of</strong> the window size is critical due to the UncertaintyPrinciple<br />

<strong>and</strong> this limitation becomes important when the signal has transient components<br />

localized in time as in ERPs.<br />

Wavelets haveavarying window size, thus allowing a better time-<strong>frequency</strong> resolution<br />

for all the scales. Consequently, a further improvement to the spectral entropy is to<br />

dene the entropy from the Wavelet transform. In the latter case, the time evolution <strong>of</strong><br />

the <strong>frequency</strong> patterns can be followed with an optimal time-<strong>frequency</strong> resolution.<br />

In this chapter, I will rst introduce the denition <strong>of</strong> the Wavelet-entropy <strong>and</strong> then I<br />

will describe its application to the study <strong>of</strong> ERPs (Quian Quiroga et al., 1999a,b Rosso<br />

et al., 1998).<br />

87

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