Biorthogonal decomposition in Multilevel decompositions

Wavelets on the interval 129 or kvk α, q ≍ kP j v k +     X j ∈ b α q j    X k∈ ˆ j | ˆv j k | p    q p     1q , ∀v ∈ Z α q , if ✁ = { j ∈ ✂ : j ≥ j ∈ ✂ }. It is possible to prove a similar result for dual topological spaces see e.g. [5]. Indeed, let V be reflexive and h f, vi denote the dual pairing between the topological dual space V ′ and V . For each j ∈ ✁ , let e P j : V ′ → V ′ be the adjoint operator of P j and e V j = Im e P j ⊂ V ′ . It is possible to show that the family {e V j , e P j } satisfies the same abstract assumptions of {V j , P j }. Moreover, let 1 q ∞ and let q ′ be the conjugate index of q 1 q + 1 q ′ = 1 . Set Z −α q = Z α q ′ ′ , for 0 α 1, then one has: T HEOREM 2. Under the same assumptions of Theorem 1 and with the notations of this Section, we have Z −α q =    f ∈ Z ′ : X j ≥ j b −αq j k e Q j f k q V ′ +∞    , with k f k Z − α q ≍ e P j f V ′ +   X j ≥ j b −αq j k e Q j v k q V ′   1q , ∀ f ∈ Z −α q .

2.3. Biorthogonal decomposition in

The abstract setting can be applied to construct a biorthogonal system of compactly supported wavelets on the real line and a biorthogonal decomposition of L p 1 p ∞. We will be very brief and we refer to [5, 6, 11, 17] for proofs and more details. We suppose to have a couple of dual compactly supported scaling functions ϕ ∈ L p and e ϕ ∈ L p ′ 1 p + 1 p ′ = 1 satisfying the following conditions. There exists a couple of finite real filters h = {h n } n 1 n=n , ˜ h = ˜h n ˜ n 1 n= ˜ n with n , ˜n ≤ 0 and n 1 , ˜n 1 ≥ 0, so that ϕ and e ϕ satisfy the refinement equations: ϕ x = √ 2 n 1 X n=n h n ϕ 2x − n , e ϕ x = √ 2 ˜ n 1 X n= ˜ n ˜h n e ϕ 2x − n , 25 and supp ϕ = [n , n 1 ] , supp e ϕ = ˜n , ˜n 1 . From now on, we will only describe the primal setting, the parallel ˜ construction following by analogy; it will be understood that there p has to be replaced by the conjugate index p ′ . Setting, as usual, for j, k ∈ ✂ , ϕ j k x = 2 j p ϕ 2 j x − k, we have the biorthogonality relations hϕ j k , e ϕ j k ′ i = Z ϕ j k x e ϕ j k ′ x d x = δ kk ′ , ∀ j, k, k ′ ∈ ✂ . 130 L. Levaggi – A. Tabacco Thus 8 j = {ϕ j k : k ∈ ✂ } are uniformly p-stable bases for the spaces V j = V j = span L p {ϕ j k : k ∈ ✂ } =    X k∈ α k ϕ j k : {α k } k∈ ∈ ℓ p    , and, for any v ∈ V j , we can write v = X k∈ α k ϕ j k = X k∈ ˘v j k ϕ j k with ˘v j k = hv, e ϕ j k i and kvk L p ≍   X k∈ | ˘v j k | p   1 p . 26 We have V j ⊂ V j +1 , \ j ∈ V j = {0} , [ j ∈ V j = L p . We suppose there exists an integer L ≥ 1 so that, locally, the polynomials of degree up to L − 1 we will indicate this set ✁ L−1 are contained in V j . It is not difficult to show that L must satisfy the relation L ≤ n 1 − n 27 see [6], equation 3.2. We set ψ x = √ 2 1− e n X n=1− e n 1 g n ϕ 2x − n , with g n = −1 n e h 1−n , and ψ j k x = 2 j p ψ 2 j x − k, ∀ j, k ∈ ✂ . Then hψ j k , e ψ j ′ k ′ i = δ j j ′ δ kk ′ , ∀ j, j ′ , k, k ′ ∈ ✂ . The wavelet spaces W j =    X k∈ α k ψ j k : {α k } k∈ ∈ ℓ p    , ∀ j ∈ ✂ , satisfy L p = ⊕ j ∈ W j . For any v ∈ L p , this implies the expansion v = X j,k∈ ˆv j k ψ j k , with ˆv j k = hv, ˜ ψ j k i ; 28 in addition, if p = 2, kvk L 2 ≍   X j,k∈ | ˆv j k | 2   12 , ∀v ∈ L 2 . 29 Next, let us recall that if ϕ ∈ B s pq s 0, 1 p, q +∞ then the Bernstein and Jackson inequalities hold for every space Z = B s pq with 0 ≤ s mins , L. Indeed, we have |v| B s pq 2 j s kvk L p , ∀v ∈ V j , ∀ j ∈ ✂ 30 Wavelets on the interval 131 and kv − P j v k L p 2 − j s |v| B s pq , ∀v ∈ B s pq , ∀ j ∈ ✂ . 31 Thus, taking into account 1, we can apply the characterization Theorems 1 and 2 to the Besov space Z .

3. Scaling function spaces for the half-line