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Pit Pattern Classification in Colonoscopy using Wavelets - WaveLab

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2.3 Discrete wavelet transform<br />

Us<strong>in</strong>g equation (2.2), T (a, b) can be rewritten <strong>in</strong> a more compact way as<br />

T (a, b) =<br />

∫ ∞<br />

−∞<br />

x(t)ψ a,b (t)dt (2.4)<br />

This can than be expressed as an <strong>in</strong>ner product of the signal x(t) and the wavelet function<br />

ψ a,b (t)<br />

T (a, b) = 〈x, ψ a,b 〉 (2.5)<br />

S<strong>in</strong>ce a, b ∈ R this is called the cont<strong>in</strong>uous wavelet transform. Simply spoken equation<br />

(2.5) returns the correlation between a signal x(t) and a wavelet ψ a,b .<br />

2.3 Discrete wavelet transform<br />

The discrete wavelet transform is very similar to the cont<strong>in</strong>uous wavelet transform, but while<br />

<strong>in</strong> equation (2.2) the parameters a and b were cont<strong>in</strong>uous, <strong>in</strong> the discrete wavelet transform<br />

these parameters are restricted to discrete values. To achieve this, equation (2.2) is slightly<br />

modified<br />

ψ m,n (t) =<br />

=<br />

(<br />

1 t − nb0 a m 0<br />

√ ψ a<br />

m<br />

0<br />

a m 0<br />

)<br />

1<br />

√ a<br />

m<br />

0<br />

ψ ( a −m<br />

0 t − nb 0<br />

)<br />

(2.6)<br />

(2.7)<br />

where m controls the dilation and n the translation with m, n ∈ Z. a 0 is a fixed dilation<br />

step parameter greater than 1 and b 0 is the location parameter which must be greater than<br />

0.<br />

The wavelet transform of a cont<strong>in</strong>uous signal x(t) us<strong>in</strong>g discrete wavelets of the form of<br />

equation (2.7) is then<br />

T m,n = 1 √ a<br />

m<br />

0<br />

∫ ∞<br />

−∞<br />

x(t)ψ ( a −m<br />

0 t − nb 0<br />

)<br />

dt (2.8)<br />

which aga<strong>in</strong> can be written <strong>in</strong> a more compact way<br />

T m,n =<br />

∫ ∞<br />

−∞<br />

x(t)ψ m,n (t)dt (2.9)<br />

and therefore leads to<br />

T m,n = 〈x, ψ m,n 〉 (2.10)<br />

9

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