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The explicit four-tap Daubechies pair satisfies the orthogonal filter and two-moment conditions

Statement

The pair (h,g) in Explicit four-tap Daubechies filter and its high-pass partner is admissible in Periodic finite orthogonal compact-filter wavelet transform. In addition, ∑j=03jrgj=0 for r=0,1, so the high-pass filter annihilates constant and affine data.

Facts & Assumptions

Given: The exact four entries of h and the definition gj=(−1)jh3−j.

[F1]

Explicit four-tap Daubechies filter and its high-pass partner: h=(1+3,3+3,3−3,1−3)/(42) and g=(h3,−h2,h1,−h0).

[F2]

Periodic finite orthogonal compact-filter wavelet transform: admissibility requires unit even-shift autocorrelation for each filter, zero cross-correlation at every even shift, ∑jhj=2, and ∑jgj=0.

Proof

1.1givenF1algebra

Write r=3. Direct addition gives ∑hj=8/(42)=2. The numerator of ∑gj is (1−r)−(3−r)+(3+r)−(1+r)=0, and the numerator of ∑jgj is −(3−r)+2(3+r)−3(1+r)=0. Thus g has the required zero sum and two vanishing moments.

1.2givenF1algebra

With denominator 32, the numerator of ∑hj2 is (4+2r)+(12+6r)+(12−6r)+(4−2r)=32, so the zero-shift autocorrelation is 1. The only possible nonzero even-shift autocorrelation of a four-tap filter is at shift 2 or −2; at shift 2 its numerator is (3−r)(1+r)+(1−r)(3+r)=2r−2r=0, and the shift −2 sum is the same by reindexing. Reversal with alternating signs gives ∑gj2=1 and ∑gjgj−2=h3h1+h2h0=0.

2.1step 1.1step 1.2givenF1F2algebra∎

For the cross-correlation ∑jhjgj−2s, only s=−1,0,1 can have overlapping taps. These sums are respectively h0g2+h1g3=h0h1−h1h0=0, h0g0+h1g1+h2g2+h3g3=0 by pairwise cancellation, and h2g0+h3g1=h2h3−h3h2=0. For all other integers s the supports do not overlap, so the sum is zero. Together with steps 1.1 and 1.2 this verifies every condition in [F2].

Depends on

Used by

Cited to discharge well-definedness by Explicit four-tap Daubechies filter and its high-pass partner.

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