Volume 2013, Issue 1 694714
Research Article
Open Access

A Multiplier Theorem for Herz-Type Hardy Spaces Associated with the Dunkl Transform

A. Gasmi

Corresponding Author

A. Gasmi

Department of Mathematics, Faculty of Sciences, Taibah University, Universities Road, P.O. Box 344, Al Madinah Al Monawarah 30001, Saudi Arabia taibahu.edu.sa

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First published: 20 November 2013
Academic Editor: Julian López-Gómez

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

Let Tm(f) be a multiplier operator defined in terms of Fourier transforms by Tm(f) = −1(m(f)) for suitable functions f. The multiplier theorem of Hörmander [1] gives a sufficient condition on m for the operator Tm to be bounded on Lp(n) whenever 1 < p < , namely, that m is a bounded C-function on n∖{0} satisfying the Hörmander condition M(2, ) as follows:
()
where is the least integer greater than n/2 and s = 0, 1, …, . In [2], the authors proved that if m satisfies the Hörmander condition with > n (1/p − 1/2), then Tm is bounded on the Hardy spaces Hp(n) with 0 < p ≤ 1.
In [3], the authors considered the following multiplier operator which is associated with the Dunkl transform:
()
where α designs the Dunkl transform and using Hörmander’s technique proved the following theorem.

Theorem 1. Let be the least integer greater than α + 1 and let m be a bounded C-function on ∖{0} which satisfies the Hörmander condition Mα(2, ) as follows:

()
where C is a constant independent of R and s = 0, 1, …, . Then, the multiplier operator associated with the Dunkl transform can be extended to a bounded operator from Lp(μα) into itself for 1 < p < , where Lp(μα) is the Lebesgue space on with respect to the following measure:
()

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 n, 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 be an integer greater than 2(α + 1)β. If m satisfies the Hörmander condition Mα(2, ), 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 . 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() be the usual Schwartz space and let () be the space of C-functions on . 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 ∥fp,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 [68].

Let α > −1/2. We consider the differential-difference operator introduced in [9] as follows:
()
and call it the Dunkl operator.
For λ, the following initial value problem:
()
has a unique solution Eα(λ  ·) (called the Dunkl kernel) given by
()
where jα is the normalized Bessel function of the first kind (with order α) defined on by
()
The integral representation of Eα is given by
()
From which, we get
()
The Dunkl transform α, which was introduced by [10] and studied in [11], is defined for fL1(μα) by
()
This transform satisfies the following properties.
  • (i)

    For all fL1(μα), we have

    ()

  • (ii)

    For all fL1(μα) such that α(f) ∈ L1(μα), we have the following inversion formula:

    ()

  • (iii)

    For all f𝒮(),

    ()

  • (iv)

    α is a topological isomorphism from 𝒮() into itself.

  • (v)

    α 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 be the least integer greater than α + 1. If m satisfies the Hörmander condition Mα(2, ), then there is a constant C independent of m, such that if q = 1 or s + α + 1 < (α + 1)/qα + 1, the following inequality holds:

()
Furthermore, in case s + α + 1 < 0, then |x|s|m(s)(x)| ≤ C and m(s) is continuous on ∖{0}.

Notation. For all x, y, z, we put

()
where
()
The Dunkl translation operator τx, x is defined for a continuous function f on by
()
where γx,y   is the signed measures given by
()
The operator τx has the following properties.
  • (i)

    For x, y and a continuous function f on , we have

    ()

  • (ii)

    For all x, the operator τx can be extended to Lp(μα)  (p ≥ 1), and for fLp(μα), we have

    ()

  • (iii)

    For all x, λ and fL1(μα), we have

    ()

Let p, q, r ∈ [1, ] such that 1/p + 1/q = 1/r + 1. The convolution product of fLp(μα) and gLq(μα) is defined by

()
and we have
()
If f, gL1(μα), then
()

Now, let us recall the definition of the Herz-type Hardy space and its atomic decomposition. For N being sufficiently large, we denote by FN the subset of S() constituted by all those ϕS() such that   supp (ϕ)⊂[−1,1] and for all m, n such that m, nN, we have
()
Moreover, the system of seminorms {ρm,n} m,n generates the topology of S().
Let fS(). We define the α-grand maximal function Gα(f) of f by
()
where ϕt is the dilation of ϕ given by
()

Definition 4. Let β, 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/2k−1 ≤ |x| ≤ 2k}.

  • (ii)

    The nonhomogeneous weighted Herz space is defined, as usual, by . Moreover, .

Note that .

Definition 5. Let β, p ∈ ]0, ], and q ∈ ]1, ]. The Herz-type Hardy space is the space of distributions fS() such that . Moreover, we define

()
In the same way, we define the space for the non-homogeneous case.

Definition 6. Let q ∈ ]1, ] and β ≥ 1 − 1/q. A measurable function a on is called a (central) (β, q, s)-atom if it satisfies the following:

  • (i)

    supp  (a)⊂[−r, r], for some r > 0,

  • (ii)

    aq,αr−2(α+1)β,

  • (iii)

    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∖{0}, there exist a (β, q, s)-atom aj and λj, such that and . Moreover,

()
where the infimum is taking over all atomic decompositions of f.

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 ML2(μα) satisfying the following:

  • (i)

    M(x)|x|2(α+1)bL2(μα),

  • (ii)

    ,

  • (iii)

    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 (MkPk) 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,

()
where ai is a central (β, 2, s)-atom and . It follows from Theorem 7 that and .

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 ≤ ks 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 ∥a2,αr−2(α+1)β. From (9), (iii) of Definition (19), and the estimate for the remainder in Taylors’ formula, it follows that

()
From (ii) of Definition (19), we obtain
()
(ii) For u = 1,
()
Using (10), we get the following for all y:
()
From (ii) of Definition (19), we obtain the following for all y:
()
For u = ,
()
For 1 < u < ,
()
Finally, we get the following for all y:
()

3. Proof of Theorem 2

Let 0 < p ≤ 1 and be an integer greater than 2(α + 1)β. Set s = [2(α + 1)(1/p − 1)], ϵ = /2(α + 1) − (1/2), a = 1 − (1/p) + ϵ, and b = ϵ + (1/2).

We have − 1 ≥ s; then, according to Proposition 9 to prove Theorem 2 it suffices to prove that, for any (β, 2, )-atom f, is a central (p, s, ϵ)-molecule with for some constant C independent of f. In other words, we need to check that
()
Firstly, we prove (i) and (ii).
m satisfies the Hörmander condition Mα(2, ); then, by Theorem 1, there exists a constant C independent of f, such that
()
From (14) and (13), we have
()
Then, by Plancherel theorem to estimate , it suffices to estimate , which turns out to prove that
()
By induction, we have
()
where ar and br are constants.
But, using Leibniz formula, we have the following for r ∈ {0, 1, …, }:
()
So, to establish (47), it suffices to claim that
()
For the case k = , we use Lemma 10 (ii) with u = and Lemma 3 to get the following:
()
For 0 ≤ k < , we have
()
where
()
and j0 is the integer, such that
()
Firstly, we estimate S1.
Using (i) of Lemma 10 and the fact that m satisfies the Hörmander condition Mα(2, ), we get
()
By (54), we obtain
()
Now, we estimate S2. By Holder’s inequality, we have
()
Using (ii) of Lemmas 10 and 3, we get
()
To guarantee the convergence of this summation, we choose the pair (k, u) as follows:
  • (a)

    if lk > α + 1, we choose u = 1;

  • (b)

    if 0 < lkα + 1 and k > α + 1, we choose u = ;

  • (c)

    if 0 < lkα + 1 and kα + 1, we choose 0 < u <

such that k > (α + 1)(1 − (1/u)).
Furthermore, by (54), we get
()

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 ≤ js and : indeed if according to (14), which we have is continuous, and hence .

Now, we check . We write , where
()
Using the fact that and Schwarz’s inequality, we get
()
For 0 ≤ js, we have
()
Using the fact that s < α + 1, we get I2C.
Finally, we check
()
We have
()
where ar and br are constants. Then, to prove (63), it suffices to prove that
()
By (i) of Lemma 10, we have
()
According to Lemma 3, we have |h|rk|m(rk)(h)| ≤ C; indeed 2(rk) + α + 1 < 0; then, we obtain
()
where (63) is hence proved. This finishes the proof of Theorem 2.

Corollary 11. Let 0 < p ≤ 1. Then, the generalized Hilbert transform Hα defined by

()
where τx is given by (19), is bounded on .

Proof. From Proposition 3.6 in [3], the generalized Hilbert transform Hα is a multiplier operator with m(ξ) = −sign (ξ); then the proof of the corollary follows from Theorem 2.

Acknowledgment

This paper was supported by a generous grant from Taibah University Research Project.

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