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4.2 Theoretical Background<br />

4.2.1 Continuous Wavelet Transform<br />

A wavelet family ab is a set <strong>of</strong> elemental functions generated by dilations <strong>and</strong> translations<br />

<strong>of</strong> a unique admissible mother wavelet (t):<br />

ab(t) = jaj ;1=2<br />

t ; b<br />

where a b 2 R, a 6= 0 are the scale <strong>and</strong> translation parameters respectively.<br />

a<br />

<br />

(27)<br />

As a<br />

increases the wavelet becomes more narrow <strong>and</strong> by varying b, the mother wavelet is<br />

displaced in time. Thus, the wavelet family gives a unique pattern <strong>and</strong> its replicas at<br />

dierent scales <strong>and</strong> with variable localization in time.<br />

The continuous wavelet transform <strong>of</strong> a signal X(t) 2 L 2 (R) (nite energy <strong>signals</strong>) is<br />

dened as the correlation between the signal <strong>and</strong> the wavelet functions ab , i.e.<br />

(W X)(a b) = jaj ;1=2 Z 1<br />

;1<br />

X(t) ( t ; b<br />

a ) dt = < X(t) ab > (28)<br />

where denotes complex conjugation. Then, the dierent correlations<br />

< X(t) ab > indicates how precisely the wavelet function locally ts the signal at<br />

every scale a. Since the correlation is made with dierent scales <strong>of</strong> a single function,<br />

instead <strong>of</strong> with complex sinusoids characterized by their frequencies, wavelets give a<br />

time-scale representation.<br />

4.2.2 Dyadic Wavelet Transform<br />

The continuous Wavelet Transform maps a signal <strong>of</strong> one independent variable t onto<br />

a function <strong>of</strong> two independent variables a b. This procedure is redundant <strong>and</strong> not<br />

ecient for algorithm implementations. In consequence, it is more practical to dene<br />

the Wavelet Transform only at discrete scales a <strong>and</strong> discrete times b. One way toachieve<br />

this, is by choosing the discrete set <strong>of</strong> parameters fa j = 2 j b jk = 2 j kg, with j k 2 Z.<br />

Replacing in eq. 27 we obtain the discrete wavelet family<br />

jk(t) = 2 ;j=2 ( 2 ;j t ; k ) j k 2 Z (29)<br />

that forms a basis <strong>of</strong> the Hilbert space L 2 (R), <strong>and</strong> whose correlation with the signal is<br />

called Dyadic Wavelet Transform.<br />

38

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