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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

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