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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2 Fourier Transform<br />
2.1 Introduction<br />
<strong>Time</strong> <strong>signals</strong> can be represented in many dierent ways depending on the interest in<br />
visualizing certain given characteristics. Among these, the <strong>frequency</strong> representation is<br />
the most powerful <strong>and</strong> st<strong>and</strong>ard one. The main advantage over the time representation<br />
is that it allows a clear visualization <strong>of</strong> the periodicities <strong>of</strong> the signal, in many cases<br />
helping to underst<strong>and</strong> underlying physical phenomena. Frequency <strong>analysis</strong>, developed<br />
by Jean Baptiste Fourier (1768-1830), reached innumerable applications in mathematics,<br />
physics <strong>and</strong> natural sciences. Furthermore, the Fourier Transform is computationally<br />
very attractive since it can be calculated by using an extremely ecient algorithm called<br />
the Fast Fourier Transform (FFT Cooley <strong>and</strong> Tukey, 1965).<br />
This chapter starts with a brief mathematical background <strong>of</strong> Fourier Transform <strong>and</strong><br />
then, applications <strong>of</strong> Fourier <strong>analysis</strong> to <strong>EEG</strong> <strong>signals</strong> will be reviewed. Four main<br />
applications will be described: <strong>analysis</strong> <strong>of</strong> <strong>frequency</strong> b<strong>and</strong>s, topographical mapping,<br />
<strong>analysis</strong> <strong>of</strong> evoked responses <strong>and</strong> coherence.<br />
2.2 Theoretical background<br />
Under mild conditions, the Fourier Transform describes a signal x(t) (I will consider<br />
only real <strong>signals</strong>) as a linear superposition <strong>of</strong> sines <strong>and</strong> cosines characterized by their<br />
<strong>frequency</strong> f.<br />
where<br />
x(t) =<br />
X(f) =<br />
Z +1<br />
;1<br />
Z +1<br />
;1<br />
X(f) e i2ft df (1)<br />
x(t) e ;i2ft dt (2)<br />
are complex valued coecients that give the relative contribution <strong>of</strong> each <strong>frequency</strong> f.<br />
Equation 2 is the continuous Fourier Transform <strong>of</strong> the signal x(t). It can be seen as an<br />
inner product <strong>of</strong> the signal x(t) with the complex sinusoidal mother functions e ;i2ft ,<br />
i.e.<br />
X(f) = (3)<br />
Its inverse transform is given by eq. 1 <strong>and</strong> since the mother functions e ;i2ft are<br />
orthogonal, the Fourier Transform is nonredundant <strong>and</strong> unique.<br />
Let us consider in the following that the signal consists <strong>of</strong> N discrete values, sampled<br />
every time .<br />
13