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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A<br />
<strong>Time</strong>-<strong>frequency</strong> resolution <strong>and</strong> the Uncertainty<br />
Principle<br />
In this section after the introduction <strong>of</strong> some basic concepts from signal <strong>analysis</strong>, I will<br />
show the pro<strong>of</strong> <strong>of</strong> the Uncertainty Principle. Then, I will describe its application to the<br />
Fourier, Gabor <strong>and</strong> Wavelet Transform, stressing the advantages <strong>of</strong> each method related<br />
with time-<strong>frequency</strong> localization properties.<br />
A.1 Preliminary concepts<br />
Lets consider a normalized signal x(t) (i.e. x2 (t)dt = 1) with a corresponding<br />
Fourier Transform X(!) 9 . The energy density can be written as jx(t)j 2 in the time<br />
domain or as jX(!)j 2 in the <strong>frequency</strong> domain. Since the total energy or intensity should<br />
be the same in both domains, we have the following relation (Parceval's theorem)<br />
I =<br />
Z 1<br />
;1<br />
jx(t)j 2 dt = 1<br />
2<br />
R 1<br />
;1<br />
Z 1<br />
;1<br />
jX(!)j 2 d! (56)<br />
Considering the energy densities per time <strong>and</strong> <strong>frequency</strong>, the average time can be<br />
dened as:<br />
<strong>and</strong> the average <strong>frequency</strong> as:<br />
=<br />
Z 1<br />
;1<br />
t jx(t)j 2 dt (57)<br />
=<br />
Z 1<br />
;1<br />
! jX(!)j 2 d! (58)<br />
Furthermore, the mean <strong>frequency</strong> can be calculated without the previous computation<br />
<strong>of</strong> the Fourier spectrum, just by using the following relation (see demonstration<br />
in Cohen, 1995 pp:11)<br />
=<br />
Z 1<br />
;1<br />
! jX(!)j 2 d! =<br />
Z 1<br />
;1<br />
x (t) 1 i<br />
d<br />
x(t) dt (59)<br />
dt<br />
were denotes complex conjugation. From the energy densities we can also dene the<br />
second order moments as:<br />
=<br />
Z 1<br />
;1<br />
t 2 jx(t)j 2 dt (60)<br />
9 for simplicity I will use in this section the angular <strong>frequency</strong> ! =2f<br />
111