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Foundations of Data Science

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Scale and wavelet coefficients equations<br />

φ(x) = ∑ d−1<br />

k=0 c kφ(2x − k)<br />

∞∫<br />

−∞<br />

d−1<br />

φ(x)φ(x − k)dx = δ(k)<br />

∑<br />

c j = 2<br />

j=0<br />

d−1 ∑<br />

c j c j−2k = 2δ(k)<br />

j=0<br />

c k = 0 unless 0 ≤ k ≤ d − 1<br />

d even<br />

d−1 ∑<br />

j=0<br />

c 2j = d−1 ∑<br />

c 2j+1<br />

j=0<br />

ψ(x) = d−1 ∑<br />

∞∫<br />

x=−∞<br />

∞∫<br />

x=−∞<br />

∞∫<br />

x=−∞<br />

d−1<br />

k=0<br />

b k φ(x − k)<br />

φ(x)ψ(x − k) = 0<br />

ψ(x)dx = 0<br />

ψ(x)ψ(x − k)dx = δ(k)<br />

∑<br />

(−1) k b i b i−2k = 2δ(k)<br />

i=0<br />

d−1 ∑<br />

c j b j−2k = 0<br />

j=0<br />

d−1 ∑<br />

b j = 0<br />

j=0<br />

b k = (−1) k c d−1−k<br />

One designs wavelet systems so the above conditions are satisfied.<br />

Lemma 11.2 provides a necessary but not sufficient condition on the coefficients <strong>of</strong><br />

the dilation equation for shifts <strong>of</strong> the scale function to be orthogonal. One should note<br />

that the conditions <strong>of</strong> Lemma 11.2 are not true for the triangular or piecewise quadratic<br />

solutions to<br />

φ(x) = 1 2 φ(2x) + φ(2x − 1) + 1 φ(2x − 2)<br />

2<br />

and<br />

φ(x) = 1 4 φ(2x) + 3 4 φ(2x − 1) + 3 4 φ(2x − 2) + 1 φ(2x − 3)<br />

4<br />

which overlap and are not orthogonal.<br />

For φ(x) to have finite support the dilation equation can have only a finite number <strong>of</strong><br />

terms. This is proved in the following lemma.<br />

Lemma 11.3 If 0 ≤ x < d is the support <strong>of</strong> φ(x), and the set <strong>of</strong> integer shifts, {φ(x −<br />

k)|k ≥ 0}, are linearly independent, then c k = 0 unless 0 ≤ k ≤ d − 1.<br />

Pro<strong>of</strong>: If the support <strong>of</strong> φ(x) is 0 ≤ x < d, then the support <strong>of</strong> φ(2x) is 0 ≤ x < d 2 . If<br />

φ(x) =<br />

∞∑<br />

k=−∞<br />

362<br />

c k φ(2x − k)

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