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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4.2.5 Wavelet Packets<br />
In the approach described before, only the successive <strong>signals</strong> x j (n) are decomposed, but<br />
in many cases, it is also interesting to decompose the details r j (n). If we decompose<br />
both x j (n) <strong>and</strong> r j (n), then the original signal can be represented in dierent ways as<br />
combinations <strong>of</strong> x j (n) <strong>and</strong> r j (n) <strong>of</strong>dierent levels j.<br />
In this work, a decomposition called trigonometric wavelet packets was used (Serrano,<br />
1996). The main idea is to decompose the components r j (n) in portions.<br />
We dene any portion or local signal as<br />
r (ml)<br />
j ( n ) =<br />
l+2 m ;1<br />
X<br />
k=l<br />
C j (k) jk ( n ) (36)<br />
where the parameters m <strong>and</strong> l are chosen for r (ml)<br />
j (n) to cover the full time interval<br />
2 ;j l n 2 ;j (l +2 m ), which is a relative long interval <strong>of</strong> length 2 m;j . Note that we<br />
dened the local wavelet packet with 2 m basic functions jk (n) fork = l l+2 m ; 1.<br />
Now, we dene the set <strong>of</strong> fundamental frequencies<br />
! mh = +2h=2 m (37)<br />
with 0 h 2 m;1 <strong>and</strong> associated Fourier matrix M (m) given by<br />
M (m)<br />
dk<br />
= 2 ;m=2 8><<br />
>:<br />
sin[ (k +1=2) ]<br />
if d = 1<br />
2 1=2 cos[ ! mh (k +1=2) ] if d is even<br />
2 1=2 sin[ ! mh (k +1=2) ] if d is odd<br />
cos[ 2(k +1=2) ] if d = 2 m <br />
with 1 d 2 m , 0 k < 2 m <strong>and</strong> h = [d=2], where [ ] denotes the integer part. It<br />
can be demonstrated that M (m) is a 2 m 2 m dimensional orthogonal matrix (Serrano,<br />
1996).<br />
Then, we can dene the new set <strong>of</strong> elemental functions in order to exp<strong>and</strong> r (ml)<br />
j (n)<br />
as a 2 m dimensional vector obtained from<br />
for 1 d 2 m .<br />
(ml)<br />
jd<br />
( n ) =<br />
l+2 m ;1<br />
X<br />
k=l<br />
(38)<br />
M (m)<br />
dk jk ( n ) (39)<br />
Clearly, these functions constitute a new local orthonormal basis covering the interval<br />
under <strong>analysis</strong> 2 ;j l n 2 ;j (l +2 m ). Therefore we can give a second description <strong>of</strong><br />
the local signal as<br />
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