A Multiplier Theorem for Herz-Type Hardy Spaces Associated with the Dunkl Transform
Abstract
The main purpose of this paper is to establish a Hörmander multiplier theorem for Herz-type Hardy spaces associated with the Dunkl transform.
1. Introduction
Theorem 1. Let ℓ be the least integer greater than α + 1 and let m be a bounded Cℓ-function on ℝ∖{0} which satisfies the Hörmander condition Mα(2, ℓ) as follows:
The Hardy spaces associated with Herz spaces can be regarded as the local version at the origin of the classical Hardy spaces Hp and they are good substitutes for Hp when we study the boundedness of nontranslation invariant operators. To establish the boundedness of operators in hardy-type spaces on ℝn, one usually appeals to the atomic decomposition characterization of these spaces. In [4, 5], the authors studied the Herz-type Hardy spaces for the Dunkl operator in one-dimension and gave an atomic decomposition characterization of these spaces. The aim of this work is to prove the following Hörmander multiplier theorem on the spaces .
Theorem 2. Let 0 < p ≤ 1, β = (1/p) − (1/2), and ℓ be an integer greater than 2(α + 1)β. If m satisfies the Hörmander condition Mα(2, ℓ), then the operator is bounded on .
The paper is organized as follows. In Section 2, we recall some results about harmonic analysis and Herz-type Hardy spaces associated with the Dunkl operator on ℝ. In Section 3, we give the proof of the main result of this work. Then, as an application, we obtain the boundedness of the generalized Hilbert transform on .
Throughout this paper, let S(ℝ) be the usual Schwartz space and let ℰ(ℝ) be the space of C∞-functions on ℝ. We always use C to denote a positive constant that is independent of the main parameters involved but whose value may differ from line to line. We use the shorter notation ∥f∥p,α instead of .
2. Preliminaries
In this section, we recapitulate some results about harmonic analysis on Dunkl hypergroups and the Herz-type Hardy space and its atomic decomposition which will be used later. For details, the reader is referred to [6–8].
- (i)
For all f ∈ L1(μα), we have
() - (ii)
For all f ∈ L1(μα) such that ℱα(f) ∈ L1(μα), we have the following inversion formula:
() - (iii)
For all f ∈ 𝒮(ℝ),
() - (iv)
ℱα is a topological isomorphism from 𝒮(ℝ) into itself.
- (v)
ℱα is an isometric isomorphism of L2(μα), and we have the following Parseval formula:
()
The following lemma can be proved, similar to Lemma 7.25, page 343, in [12].
Lemma 3. Let ℓ be the least integer greater than α + 1. If m satisfies the Hörmander condition Mα(2, ℓ), then there is a constant C independent of m, such that if q = 1 or s − ℓ + α + 1 < (α + 1)/q ≤ α + 1, the following inequality holds:
Notation. For all x, y, z ∈ ℝ, we put
- (i)
For x, y ∈ ℝ and a continuous function f on ℝ, we have
() - (ii)
For all x ∈ ℝ, the operator τx can be extended to Lp(μα) (p ≥ 1), and for f ∈ Lp(μα), we have
() - (iii)
For all x, λ ∈ ℝ and f ∈ L1(μα), we have
()
Let p, q, r ∈ [1, ∞] such that 1/p + 1/q = 1/r + 1. The convolution product of f ∈ Lp(μα) and g ∈ Lq(μα) is defined by
Definition 4. Let β ∈ ℝ, p ∈ ]0, ∞[, and q ∈ [1, ∞].
- (i)
The homogeneous weighted Herz space is the space constituted by all functions , such that
()where χk is the characteristic function of Ak = {x ∈ ℝ/2k−1 ≤ |x| ≤ 2k}. - (ii)
The nonhomogeneous weighted Herz space is defined, as usual, by . Moreover, .
Note that .
Definition 5. Let β ∈ ℝ, p ∈ ]0, ∞], and q ∈ ]1, ∞]. The Herz-type Hardy space is the space of distributions f ∈ S′(ℝ) such that . Moreover, we define
Definition 6. Let q ∈ ]1, ∞] and β ≥ 1 − 1/q. A measurable function a on ℝ is called a (central) (β, q, s)-atom if it satisfies the following:
- (i)
supp (a)⊂[−r, r], for some r > 0,
- (ii)
∥a∥q,α ≤ r−2(α+1)β,
- (iii)
∫ℝ a(x)xkdμα(x) = 0, k = 0,1, …, s, where s = [2(α + 1)(β − 1 + 1/q)] and [·] denotes the integer part function.
The following theorem is shown in [4].
Theorem 7. Let 0 < p ≤ 1 < q ≤ ∞ and β ≥ 1 − 1/q . Then, if and only if, for all j ∈ ℕ∖{0}, there exist a (β, q, s)-atom aj and λj ∈ ℂ, such that and . Moreover,
In the sequel, fix q = 2 and β = 1/p − 1/2.
Definition 8. For 0 < p ≤ 1. Set s ≥ [2(α + 1)(1/p − 1)], ε > s/2(α + 1), , and b = 1/2 + ε. A central (p, s, ε)-molecule is a function M ∈ L2(μα) satisfying the following:
- (i)
M(x)|x|2(α+1)b ∈ L2(μα),
- (ii)
,
- (iii)
∫ℝ M(x)xkdμα(x) = 0, k = 0,1, …, s.
Proposition 9. Let (p, s, ε) be the triple cited in the previous definition. Every central (p, s, ε)-molecule M belongs to and , where the constant C is independent of M.
Proof. Let M be a central (p, s, ε)-molecule and suppose that . In the general case, letting , we have .
Let E0 = {|x| ≤ 1}, Ek = {2k−1 < |x| ≤ 2k}, and Mk = Mχk, k = 1, 2, 3, …, where χk is the characteristic function of Ek. For each k, there exists a unique polynomial Qk, of degree at most s, such that if Pk = Qkχk; then
Using some ideas in [2], we can show that each (Mk − Pk) is a multiple of a central (β, 2, s)-atom with a sequence of coefficients in lp. We also show that the sum can be written as an infinite linear combination of central (β, ∞, s)-atom with a sequence of coefficients in lp. Since a (β, ∞, s)-atom is also (β, 2, s)-atom, hence,
The following Lemma plays an important role in the proof of the main result of this work.
Lemma 10. Let a be a (β, 2, s)-atom. For all integer 0 ≤ k ≤ s and every 1 ≤ u ≤ ∞, there exists a constant C independent of a, such that
Proof. (i) Let a be a (β, 2, s)-atom. Consider that r > 0 such that supp (a)⊂[−r, r] and that ∥a∥2,α ≤ r−2(α+1)β. From (9), (iii) of Definition (19), and the estimate for the remainder in Taylors’ formula, it follows that
3. Proof of Theorem 2
Let 0 < p ≤ 1 and ℓ be an integer greater than 2(α + 1)β. Set s = [2(α + 1)(1/p − 1)], ϵ = ℓ/2(α + 1) − (1/2), a = 1 − (1/p) + ϵ, and b = ϵ + (1/2).
- (a)
if l − k > α + 1, we choose u = 1;
- (b)
if 0 < l − k ≤ α + 1 and k > α + 1, we choose u = ∞;
- (c)
if 0 < l − k ≤ α + 1 and k ≤ α + 1, we choose 0 < u < ∞
Finally, combining (56) and (59), we obtain (47). (i) and (ii) are hence proved.
To prove (iii), it suffices to prove that for all integer 0 ≤ j ≤ s and : indeed if according to (14), which we have is continuous, and hence .
Corollary 11. Let 0 < p ≤ 1. Then, the generalized Hilbert transform Hα defined by
Acknowledgment
This paper was supported by a generous grant from Taibah University Research Project.