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

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6.2 Theoretical Background<br />

Although the denition <strong>of</strong> this time evolving entropy can be done from any time<strong>frequency</strong><br />

representation, as Gabor Transform or dierent type <strong>of</strong> wavelets, I will describe<br />

the method from the wavelet coecients C ij (where i denotes time <strong>and</strong> j are the<br />

dierent scales) obtained after applying the multiresolution decomposition method (see<br />

sec. x4.2.3).<br />

Once the coecients C ij are known, the energy for each time i <strong>and</strong> level j can be<br />

calculated as<br />

E ij = C 2 ij (51)<br />

Since the number <strong>of</strong> components for each resolution level is dierent, I will redene<br />

the energy by calculating, for each level, its mean value in successive time windows<br />

(t = 128ms) denoted by the index k which will now give the time evolution. Then,<br />

the energy will be:<br />

E kj = 1 N<br />

i 0<br />

X+t<br />

i=i 0<br />

E ij (52)<br />

where i 0 is the starting value <strong>of</strong> the time window (i 0 =1 1+t 1+2t : : :) <strong>and</strong> N is<br />

the number <strong>of</strong> components in the time window for each resolution level. For every time<br />

window k, the total energy can be calculated as:<br />

E k = X j<br />

E kj (53)<br />

<strong>and</strong> we can dene the quantity<br />

p kj = E kj<br />

E k<br />

(54)<br />

as a probability distribution associated with the scale level j. Clearly, for each time<br />

window k, P j p kj = 1 <strong>and</strong> then, following the denition <strong>of</strong> entropy given by Shannon<br />

(1948), the time varying Wavelet-entropy can be dened as (for further details see Blanco<br />

et al., 1998a):<br />

WS k = ; X j<br />

p kj log 2<br />

p kj (55)<br />

88

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