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njit-etd2003-081 - New Jersey Institute of Technology

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67<br />

3.7.1 Continuous Wavelet Transform<br />

The continuous wavelet transform maps a function f (t) onto time-scale space as<br />

This operation can be expressed in a simpler inner product notation as<br />

ψab (t) represents a family <strong>of</strong> functions obtained from a single wavelet function ψ (t) and<br />

the dilation and translation parameters a and b as<br />

where a and b are continuous.<br />

The wavelet function ψ(t) is a band-pass function. It is desired that this function<br />

have a good time and frequency localization so that f (t) is decomposed into elementary<br />

building blocks which are jointly well localized in time and frequency. The wavelet<br />

function has to satisfy the "admissibility" condition that makes it an isometry (up to a<br />

constant) <strong>of</strong> I! (R) onto 1,2 (R x R) . This requirement limits the wavelet functions which<br />

must satisfy [45][46]<br />

where ψ(Ω) is the Fourier transform <strong>of</strong> the wavelet function ψ(t). The admissibility<br />

condition is directly related to the decay <strong>of</strong> the wavelet function ψ(t) which is required<br />

to have good localization. The admissibility condition for a continuous ψ(Ω) is<br />

equivalent to a zero-mean wavelet function in time:

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