For μ≥−12, and under appropriate conditions on the sequence {Mp}∞p=0 of weights, the elements, the (weakly, weakly*, strongly) bounded subsets, and the (weakly, weakly*, strongly) convergent sequences in the dual of a space Kμ of type Hankel-K{Mp} can be represented by distributional derivatives of functions and measures in terms of iterated adjoints of the differential operator x−1Dx and the Bessel operator Sμ=x−μ−12Dxx2μ+1Dxx−μ−12. In this paper, such representations are compiled, and new ones involving adjoints of suitable iterations of the Zemanian differential operator Nμ= xμ+12Dxx−μ−12 are proved. Prior to this, new descriptions of the topology of the space Kμ are given in terms of the latter iterations.
Citation: Samuel García-Baquerín, Isabel Marrero. Duals of Gelfand-Shilov spaces of type K{Mp} for the Hankel transformation[J]. AIMS Mathematics, 2024, 9(7): 18247-18277. doi: 10.3934/math.2024891
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For μ≥−12, and under appropriate conditions on the sequence {Mp}∞p=0 of weights, the elements, the (weakly, weakly*, strongly) bounded subsets, and the (weakly, weakly*, strongly) convergent sequences in the dual of a space Kμ of type Hankel-K{Mp} can be represented by distributional derivatives of functions and measures in terms of iterated adjoints of the differential operator x−1Dx and the Bessel operator Sμ=x−μ−12Dxx2μ+1Dxx−μ−12. In this paper, such representations are compiled, and new ones involving adjoints of suitable iterations of the Zemanian differential operator Nμ= xμ+12Dxx−μ−12 are proved. Prior to this, new descriptions of the topology of the space Kμ are given in terms of the latter iterations.
As it is well known, Schwartz developed the theory of distributions in the late 1940's; a detailed exposition appears in his monograph [29]. Generalized functions of any kind, as well as their use to solve the Cauchy problem, were introduced by Gelfand and Shilov around 1953. In the period of 1956–58, these two authors published three volumes (in Russian) on the subject, which were translated into English during the 1960's [11,12,13]. Meanwhile, Friedman disseminated the ideas of Gelfand and Shilov in his book [10], enhancing them with more recent applications to differential equations, as well as a more complete treatment of the Cauchy problem.
Several test function spaces that were derived in the framework of the generalized Fourier transformation belong to the family of Gelfand-Shilov K{Mp} spaces, whose theory was developed in [10,12,13] in connection with the Cauchy problem for various partial differential equations, boundary value problems for elliptic equations, and the problem of eigenfunction expansions for several differential operators. Among them are the spaces DK and S, introduced by Schwartz [29]; the space H (also denoted by K1), as developed by Sebastião e Silva [30] and later studied by Hasumi [16], Zieleźny [41], Sznajder and Zieleźny [34], and, somewhat more recently, by de Sousa Pinto [31]; the spaces denoted by Kp (p>1), as developed by Sznajder and Zieleźny [35]; and the spaces Sα,A and WM,a, developed by Gelfand and Shilov themselves [12,13].
Most of the examples listed above have analogues in the Hankel transformation setting, such as those considered by Zemanian [38,39], Betancor and Marrero [5], Betancor and Rodríguez-Mesa [6,7], Durán [8], van Eijndhoven and Kerkhof [9], Lee [21], Pathak and Sahoo [26], and Pathak and Upadhyay [27]. In order to unify the underlying theory, Marrero introduced [24] and studied [22,23,25] the so-called Hankel-K{Mp} spaces, which were intended to play the same role in the Hankel transformation setting as do the Gelfand-Shilov K{Mp} spaces in the Fourier transformation setting. The study of Hankel-K{Mp} spaces was continued by Arteaga and Marrero [1,2].
In [10, p. 37], Friedman asserts the following:
One of the most interesting and important problems in the theory of generalized functions is the problem of finding the structure of generalized functions by expressing them in terms of differential operators acting on functions or on measures.
Our aim in this paper is threefold: first, we want to briefly review the existing literature on the structure of distributions in spaces of type Hankel-K{Mp}; second, we want to obtain new structural results for these distributions in terms of the Zemanian differential operator Nμ [40, Section 5.3, Equation (3)]; and, third, we want to apply them in the characterization of the bounded subsets and the convergent sequences in the duals of spaces of type Hankel-K{Mp}.
The paper is organized as follows. In Section 2, the definition and topological properties, along with some examples of Hankel-K{Mp} spaces, are recalled. Section 3 is devoted to reviewing the literature on the structural properties of the dual of a space of type Hankel-K{Mp}. The main results are established in Section 4, where a new description of the topology of a Hankel-K{Mp} space is obtained; then, in Section 5, where such a description is applied to provide new results on the structure, boundedness, and convergence of distributions of type Hankel-K{Mp}.
Throughout the paper, the standard notation in distribution theory will be used. The letter I will stand for the interval ]0,∞[ and, unless otherwise stated, μ will be a fixed real parameter not less than −12, while C will represent a suitable positive constant which may vary from line to line.
Definition 2.1. ([24, Definition 2.1]) Let {Mp}∞p=0 be a sequence of continuous functions defined on I=]0,∞[ such that
1=M0(x)≤M1(x)≤M2(x)≤…(x∈I). |
We say that Kμ is a space of type Hankel-K{Mp}, or just a Hankel-K{Mp} space, provided that Kμ consists of all of the complex-valued functions φ∈C∞(I) such that
‖φ‖μ,∞,p=max0≤k≤psupx∈I|Mp(x)(x−1D)kx−μ−12φ(x)|<∞(p∈N0). |
Kμ is endowed with the locally convex topology generated by the sequence of norms {‖⋅‖μ,∞,p}∞p=0. The dual space of Kμ will be denoted by K′μ.
What follows are examples of test function spaces of type Hankel-K{Mp} arising in connection with the generalized Hankel transformation.
Example 2.2. Let
Mp(x)=(1+x2)p(x∈I, p∈N0). |
The corresponding Hankel-K{Mp} space is the Zemanian space Hμ [38], [40, Chapter 5].
Example 2.3. Fix a>0. If the functions {Mp}∞p=0 are allowed to take on the value ∞, then, with the convention that 0⋅∞=0, the Zemanian space Bμ,a [39] can be regarded as a Hankel-K{Mp} space upon setting
Mp(x)={1,0<x<a∞,x≥a(p∈N0). |
Example 2.4. Given α,A>0, define
Mp(x)=(1+x2)pexp{αeA1α(1−1p)x1α}(x∈I, p∈N0). |
The resulting Hankel-K{Mp} space is the space Hμ,α,A, as introduced by Betancor and Marrero [5].
Example 2.5. The space χμ, as defined by Betancor and Rodríguez-Mesa [6], is the Hankel-K{Mp} space corresponding to the choice
Mp(x)=exp(px)(x∈I, p∈N0). |
Example 2.6. The space U∞μ,M,a developed by Pathak and Upadhyay [27] is also of type Hankel-K{Mp}, as can be seen upon setting
Mp(x)=exp{M[a(1−1p)x]}(x∈I, p∈N0), |
where a>0,
M(x)=∫x0v(ξ)dξ(x∈I), |
and the function v=v(ξ) is continuous and increasing on [0,∞[, with v(0)=0 and v(∞)=∞.
In the previous examples, the sequence of weights {Mp}∞p=0 satisfies at least one of the conditions in the following definition.
Definition 2.7. The sequence {Mp}∞p=0 is said to satisfy condition (⋅) for ⋅=O, A, M, N, P, provided that the following hold:
(O) The limit limx→0+Mp(x) (p∈N0) exists.
(A) Given r,p∈N0, there exist s∈N0 and brp>0 such that
Mr(x)Mp(x)≤brpMs(x)(x∈I). |
(M) Each Mp (p∈N0) is quasi-monotonic, that is, there exists Cp>0 such that
Mp(x)≤CpMp(y)(x,y∈I, x≤y). |
(N) For every p∈N0, there exists r∈N0, r>p such that the function
mpr(x)=Mp(x)Mr(x)(x∈I) |
lies in L1(I) and satisfies
limx→∞mpr(x)=0. |
(P) Given p∈N0, there exists r∈N0, r>p for which
limx→∞Mp(x)Mr(x)=0. |
By imposing appropriate combinations of the above conditions on the weights {Mp}∞p=0, Hankel-K{Mp} spaces can be endowed with interesting properties as topological vector spaces. It should be remarked that conditions similar to those in Definition 2.7 have been considered by several authors [12,14,15,19,20,32,33,37] in order to develop a suitable theory of the Gelfand-Shilov spaces of type K{Mp}.
In fact, under adequate assumptions on the weights {Mp}∞p=0, a space Kμ of type Hankel-K{Mp} can be nuclear [36, Definition Ⅲ.50.1], Schwartz [17, Definition 3.15.1], Montel [17, Definition 3.9.1], and reflexive. We excerpt from [24] some of the results available along these lines, as well as those that reveal the relationship between Kμ and the Zemanian spaces Hμ and Bμ (see Examples 2.2 and 2.3).
Proposition 2.8. ([24, Proposition 4.1]) The space Kμ is Fréchet. If the sequence {Mp}∞p=0 satisfies (O) and (P), then Kμ is Schwartz, Montel, and reflexive.
Proposition 2.9. ([24, Proposition 4.3]) Assume that {Mp}∞p=0 satisfies conditions (O) or (M). Then, the injection Bμ↪Kμ is continuous. If, additionally, {Mp}∞p=0 satisfies (P), then Bμ is dense in Kμ.
Proposition 2.10. ([24, Proposition 4.4]) Assume that {Mp}∞p=0 satisfies (M) and (N).
(i) For every p∈N0, there exist r∈N0, r>p, and Cpr>0 such that x≤CprMr(x) (x∈I).
(ii) If {Mp}∞p=0 satisfies (A) as well, then Kμ⊂Hμ with a continuous embedding.
Corollary 2.11. ([24, Corollary 4.5]) If {Mp}∞p=0 satisfies conditions (A), (M), and (N), then Bμ⊂Kμ⊂Hμ with a continuous embedding. Moreover, Bμ is dense in Kμ and Kμ is dense in Hμ.
Proposition 2.12. ([24, Proposition 4.6]) Under (A), (M), and (N), the topology of Kμ is compatible with any one of the families of norms {‖⋅‖μ,q,p}∞p=0 (q∈R, 1≤q<∞), where
‖φ‖μ,q,p={p∑k=0∫∞0|Mp(x)(x−1D)kx−μ−12φ(x)|qdx}1q(φ∈Kμ). |
In this case, Kμ is nuclear, Schwartz, Montel, and reflexive.
Again, by imposing appropiate conditions on the weights {Mp}∞p=0, the strong dual K′μ,b of a Hankel-K{Mp} space Kμ can be made nuclear, Schwartz, bornological [17, Definition 3.7.1], complete, Montel, and reflexive. Additionally, a wide range of structural results and characterizations of the bounded subsets and convergent sequences in K′μ are made available.
Proposition 3.1. ([24, Proposition 5.1]) Let Kμ be a Hankel-K{Mp} space with a strong dual K′μ,b.
(i) If the sequence {Mp}∞p=0 satisfies (O) and (P), then K′μ,b is complete, bornological, Schwartz, Montel, and reflexive.
(ii) If {Mp}∞p=0 satisfies (A),(M), and (N), then K′μ,b is complete, bornological, Schwartz, Montel, reflexive, and nuclear.
Next, we show that the functionals in the dual K′μ of a space Kμ of type Hankel-K{Mp} can be expressed as distributional derivatives of integrable functions and measures. The highest order of the differential operators that provide such representations is uniform over bounded subsets of K′μ,b. Furthermore, the convergence to zero of a sequence in this space is determined by the convergence to zero, in their respective spaces, of the functions or measures representing the terms of the sequence.
In Propositions 3.2 and 3.3 below, the results on boundedness and convergence will be stated for the strong topology of K′μ, but, it must be kept in mind that, under the same conditions, they are equally valid if the weak or weak* topologies are instead considered on that space. Indeed, by making appropriate assumptions on the weights, Kμ becomes Montel, and, hence, reflexive (Propositions 2.8 and 2.12). Thus, the weak and weak* topologies of K′μ coincide, whereas the weak* and strong sequential convergence are equivalent on this space [36, Proposition Ⅱ.34.6, Corollary 1]. Furthermore, given that Kμ is Fréchet (Proposition 2.8), it is also barrelled [36, Definition Ⅱ.33.1 and Proposition Ⅱ.33.2, Corollary 1], and, in this class of spaces, the weak* and strong topologies share the same bounded sets [36, Theorem Ⅱ.33.2].
At this point, we are in a position to state the first result on representation, boundedness, and convergence in the dual of Kμ. To this end, let C(I) denote the space of all of the functions f∈C[0,∞[ such that
limx→∞f(x)=0, |
normed with
‖f‖∞=supx∈I|f(x)|. |
Its dual C′(I) consists of all of the regular, complex Borel measures σ on [0,∞[, with the total variation norm |σ|.
Proposition 3.2. Assume that {Mp}∞p=0 satisfies (O) and (P).
(i) [24, Proposition 5.2] A linear functional f belongs to K′μ if, and only if, there exist p∈N0 and σk∈C′(I) (k∈N0, 0≤k≤p) satisfying
f=p∑k=0x−μ−12(−Dx−1)k[Mp(x)σk]. |
(ii) [24, Proposition 5.4] A set B⊂K′μ,b is bounded if, and only if, each f∈B admits the representation
f=p∑k=0x−μ−12(−Dx−1)k[Mp(x)σk,f], |
with σk,f∈C′(I) (k∈N0, 0≤k≤p) such that
p∑k=0∫∞0d|σk,f|≤C, |
where p∈N0 and C>0 do not depend on f∈B.
(iii) [24, Proposition 5.4] A sequence {fj}∞j=0 converges to zero in K′μ,b if, and only if, each fj admits the representation
fj=p∑k=0x−μ−12(−Dx−1)k[Mp(x)σk,j](j∈N0), |
with σk,j∈C′(I) (k∈N0, 0≤k≤p) such that p∈N0 does not depend on j and
limj→∞p∑k=0∫∞0d|σk,j|=0. |
Proposition 3.3. Assume that {Mp}∞p=0 satisfies (A), (M), and (N).
(i) [24, Proposition 5.3] A linear functional f belongs to K′μ if, and only if, for every q, 1<q≤∞, there exists p∈N0 such that f can be written as
f=p∑k=0x−μ−12(−Dx−1)k[Mp(x)gk(x)], |
with gk∈Lq(I) (k∈N0, 0≤k≤p).
(ii) [24, Proposition 5.5] A set B⊂K′μ,b is bounded if, and only if, given q, 1<q≤∞, there exist p∈N0, C>0, and, for each f∈B, functions gk,f∈Lq(I) (k∈N0, 0≤k≤p) such that
f=p∑k=0x−μ−12(−Dx−1)k[Mp(x)gk,f(x)], |
with
p∑k=0‖gk,f‖q≤C. |
(iii) [24, Proposition 5.5] A sequence {fj}∞j=0 converges to zero in K′μ,b if, and only if, for every q, 1<q≤∞, there exist p∈N0 and gk,j∈Lq(I) (k∈N0, 0≤k≤p) such that
fj=p∑k=0x−μ−12(−Dx−1)k[Mp(x)gk,j(x)](j∈N0), |
with
limj→∞p∑k=0‖gk,j‖q=0. |
Starting from Proposition 3.3, and adapting a technique of Kamiński [18], Marrero [25] obtained the results on structure, boundedness, and convergence in K′μ, labeled below as Theorems 3.4, 3.5, and 3.6, respectively. Unlike Proposition 3.3, the aforementioned theorems have the advantage of allowing the elements of the dual to be expressed as the distributional derivative of a single continuous function under the same differential operator.
Theorem 3.4. ([25, Theorem 2.4]) Assume that {Mp}∞p=0 satisfies conditions (A), (M), and (N). Then, the following statements are equivalent:
(i) The functional f lies in K′μ.
(ii) There exist k,p∈N0 and a function F, continuous on I, such that
f=x−μ−12(Dx−1)kF(x) | (3.1) |
and
M−1pF∈Lq(I) | (3.2) |
for any q, 1≤q≤∞.
(iii) There exist k,p∈N0 and a function F, continuous on I and satisfying (3.1), such that (3.2) holds for some q, 1≤q≤∞.
(iv) There exist k,p∈N0 and a function F, continuous on I and satisfying (3.1), such that (3.2) holds for q=∞.
Now, we shall state a characterization of boundedness in K′μ.
Theorem 3.5. ([25, Theorem 2.5]) Assume that {Mp}∞p=0 satisfies conditions (A), (M), and (N). Then, the following four statements are equivalent:
(i) The set B⊂K′μ is (weakly, weakly*, strongly) bounded.
(ii) There exist k,p∈N0, C>0, and, for each f∈B, a function gf, continuous on I, such that
f=x−μ−12(Dx−1)kgf(x) | (3.3) |
and
‖M−1pgf‖q≤C | (3.4) |
for any q, 1≤q≤∞.
(iii) There exist k,p∈N0, C>0, and, for each f∈B, a function gf, continuous on I and satisfying (3.3), such that (3.4) holds for some q, 1≤q≤∞.
(iv) There exist k,p∈N0, C>0, and, for each f∈B, a function gf, continuous on I and satisfying (3.3), such that (3.4) holds for q=∞.
Finally, convergence in K′μ is described.
Theorem 3.6. ([25, Theorem 2.6]) Assume that {Mp}∞p=0 satisfies conditions (A), (M), and (N). Then, the following statements are equivalent:
(i) The sequence {fj}∞j=0 converges (weakly, weakly*, strongly) to zero in K′μ.
(ii) There exist k,p∈N0 and Fj, continuous on I, such that
fj=x−μ−12(Dx−1)kFj(x)(j∈N0) | (3.5) |
and
limj→∞‖M−1pFj‖q=0 | (3.6) |
for any q, 1≤q≤∞.
(iii) There exist k,p∈N0 and Fj, continuous on I and satisfying (3.5), such that (3.6) holds for some q, 1≤q≤∞.
(iv) There exist k,p∈N0 and Fj, continuous on I and satisfying (3.5), such that (3.6) holds for q=∞.
(v) There exist k,p∈N0, C>0, and functions Fj, continuous on I and satisfying (3.5), such that
‖M−1pFj‖∞≤C(j∈N0) |
and limj→∞Fj(x)=0 for almost all x∈I.
Arteaga and Marrero [1] have shown that the topology of a Hankel-K{Mp} space can be generated by families of norms of type Lq (1≤q≤∞) that involve the Bessel operator.
Definition 3.7. For 1≤q<∞, consider the following families of norms on Kμ:
|φ|μ,q,r=r∑k=0{∫∞0|Mr(x)x−μ−12Skμφ(x)|qdx}1q|φ|μ,∞,r=max0≤k≤rsupx∈I|Mr(x)x−μ−12Skμφ(x)|(φ∈Kμ, r∈N0), |
where
Sμ=x−μ−12Dx2μ+1Dx−μ−12=D2−4μ2−14x2 |
is the Bessel operator.
Theorem 3.8. ([1, Proposiciones 2.5 and 2.6]) Under conditions (A), (M), and (N) on the weights {Mp}∞p=0, any one of the families of norms {|⋅|μ,q,r}∞r=0 (1≤q≤∞) generates the usual topology of Kμ.
Remark 3.9. Theorem 3.8 widens the class of spaces of type Hankel-K{Mp} and shows how some of them, treated independently in the literature, actually coincide. In fact, for a>0, let
Mp(x)=exp{M(a[1−1p]x)}(x∈I, p∈N0), |
where M∈C2[0,∞[ satisfies that M(0)=M′(0)=0, M′(∞)=∞, and M′′(x)>0 (x∈I); also, let Kμ be the corresponding Hankel-K{Mp} space. Then, we get that Kμ=xμ+12WeM,a, where WeM,a is the space introduced by van Eijndhoven and Kerkhof [9]. For the space Uqμ,M,a (1≤q≤∞) developed by Pathak and Upadhyay [27], the algebraic and topological identification
Kμ=Uqμ,M,a=U∞μ,M,a=xμ+12WeM,a(1≤q<∞) |
follows; see [7] as well.
More recently, on the basis of Theorem 3.8, and by combining techniques from [24,25], Arteaga and Marrero [2] found new representations for the elements, the bounded subsets, and the convergent sequences in K′μ, this time with the operator Sμ instead of the operator x−1D (see Sections 3.2 and 3.3). Their results are summarized below, beginning with the structure of the distributions in K′μ.
Theorem 3.10. ([2, Theorem 4.1]) Assume that the sequence of weights {Mp}∞p=0 satisfies conditions (A), (M), and (N). The following statements are equivalent:
(i) The functional f lies in K′μ.
(ii) For each q, 1<q≤∞, there exist r∈N0 and fk∈Lq(I) (k∈N0, 0≤k≤r) such that
f=∑rk=0Skμ[Mr(x)x−μ−12fk(x)]. |
(iii) There exist k,p∈N0 and F∈C(I) such that f=Skμx−μ−12F(x), with M−1pF∈Lq(I) for all q, 1≤q≤∞.
(iv) There exist k,p∈N0 and F∈C(I) such that f=Skμx−μ−12F(x), with M−1pF∈Lq(I) for some q, 1≤q≤∞.
(v) There exist k,p∈N0 and F∈C(I) such that f=Skμx−μ−12F(x), with M−1pF∈L∞(I).
Next, boundedness in K′μ is characterized.
Theorem 3.11. ([2, Theorem 5.1]) Assume that the sequence of weights {Mp}∞p=0 satisfies conditions (A), (M), and (N). The following five statements are equivalent:
(i) The set B⊂K′μ is (weakly, weakly*, strongly) bounded.
(ii) Given q, 1<q≤∞, there exist r∈N0, C>0, and, for each f∈B, functions gf,i∈Lq(I) (i∈N0, 0≤i≤r) such that
f=r∑i=0Siμ[Mr(x)x−μ−12gf,i(x)], |
with ∑ri=0‖gf,i‖q≤C.
(iii) There exist k,p∈N0, C>0, and, for each f∈B, a function gf∈C(I) such that f=Skμx−μ−12gf(x), with ‖M−1pgf‖q≤C for every q, 1≤q≤∞.
(iv) There exist k,p∈N0, C>0, and, for each f∈B, a function gf∈C(I) such that f=Skμx−μ−12gf(x), with ‖M−1pgf‖q≤C for some q, 1≤q≤∞.
(v) There exist k,p∈N0, C>0, and, for each f∈B, a function gf∈C(I) such that f=Skμx−μ−12gf(x), with ‖M−1pgf‖∞≤C.
We close this section with the corresponding characterization of sequential convergence in K′μ.
Theorem 3.12. ([2, Theorem 6.1]) Under conditions (A), (M), and (N) on the sequence of weights {Mp}∞p=0, the following statements are equivalent:
(i) The sequence {fn}∞n=0 converges (weakly, weakly*, strongly) to zero in K′μ.
(ii) For each q, 1<q≤∞, there exist r∈N0 and fn,i∈Lq(I) (n,i∈N0, 0≤i≤r) such that
fn=r∑i=0Siμ[Mr(x)x−μ−12fn,i(x)](n∈N0), |
with limn→∞∑ri=0‖fn,i‖q=0.
(iii) There exist k,p∈N0 and Fn∈C(I) such that
fn=Skμx−μ−12Fn(x)(n∈N0), |
with limn→∞‖M−1pFn‖q=0 for all q, 1≤q≤∞.
(iv) There exist k,p∈N0 and Fn∈C(I) such that
fn=Skμx−μ−12Fn(x)(n∈N0), |
with limn→∞‖M−1pFn‖q=0 for some q, 1≤q≤∞.
(v) There exist k,p∈N0 and Fn∈C(I) such that
fn=Skμx−μ−12Fn(x)(n∈N0), |
with limn→∞‖M−1pFn‖∞=0.
(vi) There exist k,p∈N0, C>0, and Fn∈C(I) such that
fn=Skμx−μ−12Fn(x), |
with ‖M−1pFn‖∞≤C (n∈N0) and limn→∞Fn(x)=0 for almost all x∈I.
First, we shall show that, for μ≥−12 and every p, 1≤p≤∞, the families of norms {ρμp,r}∞r=0 generate the usual topology of a space Kμ of type Hankel-K{Mp}, where, for r∈N0 and φ∈Kμ,
ρμ∞,r(φ)=max0≤k≤rsupx∈I|Mr(x)Tμ,kφ(x)|,ρμp,r(φ)=max0≤k≤r{∫∞0|Mr(x)Tμ,kφ(x)|pdx}1p(1≤p<∞). | (4.1) |
Here,
Tμ,k=Nμ+k−1⋯Nμ(k∈N), | (4.2) |
where Nμ=xμ+12Dx−μ−12 denotes the Zemanian operator [40, pp. 135ff] and Tμ,0 is the identity operator. The differential operators in (4.2) are interesting because of their symmetric behavior in the presence of the Hankel transformation; in fact, for an appropriate order of this transformation, it exchanges the order of the powers of the variable and the order of the differential operator defined in (4.2), an extremely useful operational rule that is very similar to its Fourier counterpart [40, Proof of Theorem 5.4-1].
This new description for the topology of Kμ was motivated by [4, Theorem 3.3], where a similar result was established for the Zemanian space Hμ (Example 2.2). The validity of this result requires assuming conditions (O), (A), (M), and (N) apply to the sequence of weights {Mp}∞p=0 (Definition 2.7), which is a hypothesis that will be maintained throughout the entire section, although, for the sake of simplicity, it will not be made explicit on all occasions.
The proof of this first result imitates that of [4, Theorem 3.3]. Roughly speaking, it consists of introducing a new space of test functions, which we will denote by Sμ, and whose definition is formally analogous to that of Kμ, but with the operator Tμ,k in place of the operator (x−1D)kx−μ−12 (k∈N0); this is followed by proving, with the aid of the open mapping theorem [28, Corollary 2.12], that, actually, Sμ=Kμ (Theorem 4.4). Once this is done, it is not difficult to infer that the families of norms defined in (4.1) are equivalent over Sμ (Proposition 4.6). At this point, we will apply techniques that are analogous to those used in the proof of the results in Section 3 in order to find representations of the elements, the (weakly, weakly*, strongly) bounded subsets, and the (weakly, weakly*, strongly) convergent sequences in the dual space S′μ=K′μ, this time as distributional derivatives induced by the adjoint of the operator Tμ,k (k∈N0). Thus, Theorems 5.4–5.7 below generalize and improve, in a sense that will be specified in due course, their analogues for the space H′μ in [4].
We must emphasize that, although the ideas presented in this section are not entirely new, the results obtained in the general context of Hankel-K{Mp} spaces have not appeared previously in the literature.
Given μ∈R, denote by Sμ the vector space of all smooth, complex-valued functions φ=φ(x) defined on I=]0,∞[ such that ωμp,k(φ)<∞, where
ωμp,k(φ)=supx∈I|Mp(x)Tμ,kφ(x)|(p,k∈N0) |
and Tμ,k (k∈N0) is as defined above.
A direct computation shows that, for k∈N0,
Tμ,k=xk+μ+12(x−1D)kx−μ−12=bμk,0x−k+bμk,1x−k+1D+…+bμk,kDk, | (4.3) |
where the coefficients bμk,j (0≤j≤k) are appropriate constants, with bμk,k=1.
The family Ω={ωμp,k}∞p,k=0 is a countable family of seminorms. This family is separating, because {ωμp,0}∞p=0 are norms. Consequently, Ω makes Sμ into a countably multinormed space.
A family of norms P={ρμ∞,r}∞r=0 that is equivalent to Ω, with the property that ρμ∞,r≤ρμ∞,s (r,s∈N0), is obtained by setting
ρμ∞,r=max0≤k≤rωμr,k(r∈N0). |
Proposition 4.1. The space Sμ (μ∈R) is Fréchet.
Proof. Let {φn}∞n=0 be a Cauchy sequence in Sμ; we want to prove that it converges in Sμ.
By (4.3), we have
Dk=Tμ,k−(bμk,0x−k+…+bμk,k−1x−1Dk−1). | (4.4) |
Proceeding by induction on k, we find that, for each compact K⊂I, there exist constants cμk,j (0≤j≤k) such that
supx∈K|Dkφ(x)|≤cμk,0ωμ0,0(φ)+cμk,1ωμ0,1(φ)+…+cμk,kωμ0,k(φ)(φ∈Sμ). |
Since ωμ0,k(φn−φm)→n,m→∞0, the sequence {Dkφn}∞n=0 is uniformly Cauchy on compact subsets of I for all k∈N0. Thus, there exists φ∈C∞(I) such that
Dkφn(x)→n→∞Dkφ(x)(k∈N0) |
uniformly over compact subsets of I. This φ is the limit of {φn}∞n=0 in Sμ. Indeed, for any p,k∈N0 and every ε>0, there exists Nμp,k=Nμp,k(ε)∈N0 such that
|Mp(x)Tμ,k(φn−φm)(x)|<ε(x∈I, n,m≥Nμp,k). |
Taking the limit as n→∞, it follows that
ωμp,k(φ−φm)≤ε(m≥Nμp,k). |
On the other hand, there exists Bμp,k>0, independent of m, such that
ωμp,k(φm)≤Bμp,k(m,p,k∈N0). |
Thus,
ωμp,k(φ)≤Bμp,k+ε(p,k∈N0). |
This shows that φ∈Sμ and {φn}∞n=0 converges to φ in Sμ, as asserted.
Proposition 4.2. For μ≥−12, the inclusion Kμ⊂Sμ holds. Moreover, the embedding Kμ↪Sμ is continuous.
Proof. Let p∈N0. Proposition 2.10(i), along with condition (A) on the weights, yields r,s∈N0, s>r>p+μ+12, and C>0 such that
|Mp(x)Tμ,kφ(x)|=|Mp(x)xk+μ+12(x−1D)kx−μ−12φ(x)|≤C|Mp(x)Mr(x)(x−1D)kx−μ−12φ(x)|≤C|Ms(x)(x−1D)kx−μ−12φ(x)|(x∈I, k∈N0, 0≤k≤p) |
whenever φ∈Kμ. According to Definition 2.1, this means that
ρμ∞,p(φ)≤C‖φ‖μ,∞,s<∞(φ∈Kμ), |
which completes the proof.
Proposition 4.3. Suppose that φ∈Sμ. Then, φ∈Kμ if, and only if, the following limits exist:
limx→0+(x−1D)kx−μ−12φ(x)(k∈N0). | (4.5) |
In other words,
Kμ={φ∈Sμ:there existlimx→0+(x−1D)kx−μ−12φ(x) (k∈N0)}={φ∈Sμ:(x−1D)kx−μ−12φ(x)=O(1)asx→0+ (k∈N0)}. | (4.6) |
Proof. Note that the existence of a limit is a stronger condition than boundedness near the origin; thus, the first set on the right-hand side of (4.6) is contained in the second set.
Under (A), (M), and (N), we have that Kμ⊂Hμ (Proposition 2.10(ii)). Hence, if φ∈Kμ, then φ∈Sμ (by Proposition 4.2) and the limits given by (4.5) exist [40, Lemma 5.2-1].
Finally, suppose that φ∈Sμ and (x−1D)kx−μ−12φ(x) is bounded near zero for all k∈N0. Since (O) holds, Mp(x)(x−1D)kx−μ−12φ(x) is also bounded near zero for any p,k∈N0. On the other hand,
|Mp(x)(x−1D)kx−μ−12φ(x)|=|Mp(x)x−k−μ−12Tμ,kφ(x)|≤|Mp(x)Tμ,kφ(x)|≤ωμp,k(φ)<∞(1≤x<∞, p,k∈N0). |
This proves that φ∈Kμ.
Theorem 4.4. For μ≥−12, the inclusion Sμ⊂Hμ holds with a continuous embedding. Consequently, Sμ=Kμ both algebraically and topologically.
Proof. To show that Sμ⊂Hμ and the inclusion map Sμ↪Hμ is continuous, note that, given p∈N0, Proposition 2.10(i) and condition (A) on the weights yield r∈N0, r>p, and C>0, for which xp≤CMr(x) (x∈I). Therefore,
supx∈I|xpTμ,kφ(x)|≤Csupx∈I|Mr(x)Tμ,kφ(x)|≤Cρμ∞,r(φ)<∞(φ∈Sμ, k∈N0, 0≤k≤p), |
and it suffices to invoke [4, Theorem 3.3]. In particular, the limits given by (4.5) exist whenever φ∈Sμ [40, Lemma 5.2-1], and, from Proposition 4.3, it follows that Sμ=Kμ.
This equality is also topological, as it can be deduced from Propositions 2.8, 4.1, and 4.2 by applying the open mapping theorem [28, Corollary 2.12].
Once it is proved that Sμ⊂Hμ, Proposition 4.5 is an immediate consequence of [4, Theorem 3.3 and Proposition 2.3]. Just for the sake of completeness, a direct proof is included.
Proposition 4.5. Let μ≥−12. Every φ∈Sμ is bounded. For any k∈N0, Dkφ is rapidly decreasing at infinity; in particular, Sμ is a dense proper subspace of L1(I).
Proof. Every φ∈Sμ is bounded because ωk0,0(φ)<∞.
To prove that Dkφ (k∈N0) is rapidly decreasing at infinity, we proceed by induction on k, bearing in mind (4.4) and the fact that, given m∈N0, Proposition 2.10(i), along with condition (A), yields r∈N0, r>m, and C>0 such that xm≤CMr(x) (x∈I). The inductive scheme is as follows.
k=0: xmφ(x) (m∈N0) is bounded for x∈I because
|xmφ(x)|≤C|Mr(x)φ(x)|=Cωμr,0(φ)<∞. |
Therefore, φ(x) is rapidly decreasing at infinity.
k=1: xmDφ(x) (m∈N0) is bounded for x≥1 because, by (4.4), we have
xmDφ(x)=xm Tμ,1φ(x)⏟ωμr,1(φ)<∞−bμ1,0xm−1φ(x)⏟m≥1: step 0m=0: φ bounded. |
Therefore, Dφ(x) is rapidly decreasing at infinity.
k=2: xmD2φ(x) (m∈N0) is bounded for x≥1 because, by (4.4), we have
xmD2φ(x)=xm Tμ,2φ(x)⏟ωμr,2(φ)<∞−bμ2.0xm−2φ(x)⏟m≥2: step 0m=0,1: φ bounded−b2,1xm−1Dφ(x)⏟m≥1: step 1m=0: Dφ bounded. |
Therefore, D2φ(x) is rapidly decreasing at infinity.
Assuming that the statement
xmDnφ(x) (m∈N0) is bounded for x≥1 |
holds true for all n∈N0 with 0≤n≤k, we prove it for k+1.
k+1: xmDk+1φ(x) (m∈N0) is bounded for x≥1 because, by (4.4), we have
xmDk+1φ(x)=xm Tμ,k+1φ(x)⏟ωμr,k+1(φ)<∞−bμk+1,0xm−k−1φ(x)⏟m≥k+1: ind. hyp.0≤m≤k: φ bounded−bμk+1,1xm−kDφ(x)⏟m≥k: ind. hyp.0≤m≤k−1: Dφ bounded−…−bμk+1,kxm−1Dkφ(x)⏟m≥1: ind. hyp.m=0: Dkφ bounded. |
Therefore, Dk+1φ(x) is rapidly decreasing at infinity and the induction is complete.
Finally, it is clear that
D(I)⊂Sμ⊂L1(I), |
which implies that Sμ is dense in L1(I).
Proposition 4.6. For μ≥−12 and any p, 1≤p≤∞, the families of norms {ρμp,r}∞r=0 generate the topology of Sμ, where, for r∈N0 and φ∈Sμ,
ρμ∞,r(φ)=max0≤k≤rsupx∈I|Mr(x)Tμ,kφ(x)|,ρμp,r(φ)=max0≤k≤r{∫∞0|Mr(x)Tμ,kφ(x)|pdx}1p(1≤p<∞). |
Proof. Fix 1<p<∞ and φ∈Sμ. Given r∈N0, condition (N) yields s∈N0, s>r such that
∫∞0Mr(x)Ms(x)dx<∞. | (4.7) |
Since
0≤Mr(x)Ms(x)≤1(x∈I), | (4.8) |
we may write the following:
ρμp,r(φ)=max0≤k≤r{∫∞0|Mr(x)Tμ,kφ(x)|pdx}1p=max0≤k≤r{∫∞0|Ms(x)Tμ,kφ(x)|p(Mr(x)Ms(x))pdx}1p≤max0≤k≤ssupx∈I|Ms(x)Tμ,kφ(x)|{∫∞0Mr(x)Ms(x)dx}1p={∫∞0Mr(x)Ms(x)dx}1pρμ∞,s(φ). |
A new application of (4.7) and (4.8), in combination with Hölder's inequality, leads to
ρμ1,r(φ)=max0≤k≤r∫∞0|Mr(x)Tμ,kφ(x)|dx=max0≤k≤r∫∞0|Ms(x)Tμ,kφ(x)|Mr(x)Ms(x)dx≤max0≤k≤s{∫∞0|Ms(x)Tμ,kφ(x)|pdx}1p{∫∞0(Mr(x)Ms(x))qdx}1q={∫∞0Mr(x)Ms(x)dx}1qρμp,s(φ). |
Here, q=p(p−1)−1 denotes the conjugate exponent of p.
Finally, given k0∈N0 and φ∈Sμ, the function (x−1D)kx−μ−12φ(x) is rapidly decreasing at infinity because Sμ⊂Hμ (Theorem 4.4). Hence, for φ∈Sμ and r,k∈N0 with 0≤k≤r, by using (M), we find that
|Mr(x)Tμ,kφ(x)|=|Mr(x) xk+μ+12(x−1D)kx−μ−12φ(x)|=|Mr(x) xk+μ+12∫∞xt(t−1D)k+1t−μ−12φ(t)dt|≤C∫∞x|Mr(t) t(k+1)+μ+12(t−1D)k+1t−μ−12φ(t)|dt≤C∫∞0|Mr(t)Tμ,k+1φ(t)|dt(x∈I). |
Consequently,
ρμ∞,r(φ)≤Cρμ1,r+1(φ). |
The proof is thus complete.
Now that Proposition 4.6 has been proved, we intend to apply techniques similar to those employed in the proof of the results in Section 3 in order to characterize the elements, the (weakly, weakly*, strongly) bounded subsets, and the (weakly, weakly*, strongly) convergent sequences in the dual space K′μ=S′μ (μ≥−12), this time as distributional derivatives induced by the adjoint of the operator Tμ,k (k∈N0). The main results correspond to Theorems 5.4–5.5, 5.6, and 5.7, respectively. Prior to deriving these results, three auxiliary lemmas must be established.
Lemma 5.1. Let μ≥−12, and let F∈C(I) be such that there exists p∈N0 with M−1pF∈Lq(I) (1≤q≤∞). Then, for each k∈N0, there exist pk∈N0, pk≥p, and a function Fk∈C(I) satisfying
x−μ−12(Dx−1)kxk+μ+12Fk(x)=F(x)(x∈I) | (5.1) |
and
M−1pkFk∈Lq(I)(1≤q≤∞). | (5.2) |
Proof. We proceed by induction on k. The result is obvious if k=0. Suppose that, given k∈N0, k≥1, there exist pk∈N0, pk≥p, and a function Fk∈C(I) satisfying (5.1) and (5.2). Use (N) to find n,t∈N0, n>t>pk, such that
∫∞0Mpk(x)Mt(x)dx<∞, | (5.3) |
∫∞0Mt(x)Mn(x)dx<∞. | (5.4) |
The inductive hypotheses, along with (M) and (5.3), allow us to write the following:
1Mt(x)∫x0|Fk(ξ)|dξ≤C∫∞0|Fk(ξ)Mt(ξ)|dξ=C∫∞0|Fk(ξ)Mpk(ξ)|Mpk(ξ)Mt(ξ)dξ≤Csupξ∈I|Fk(ξ)Mpk(ξ)|∫∞0Mpk(ξ)Mt(ξ)dξ=Csupξ∈I|Fk(ξ)Mpk(ξ)|. | (5.5) |
The function
˜Fk(x)=x−k−μ−12∫x0Fk(ξ)ξk+μ+12dξ(x∈I) |
is continuous, and, by (5.1), we have
x−μ−12(Dx−1)k+1x(k+1)+μ+12˜Fk(x)=x−μ−12(Dx−1)kxk+μ+12Fk(x)=F(x)(x∈I). |
Furthermore, using (5.5), it follows that
|˜Fk(x)Mt(x)|=1Mt(x)|x−k−μ−12∫x0Fk(ξ)ξk+μ+12dξ|≤1Mt(x)∫x0|Fk(ξ)|dξ≤Csupξ∈I|Fk(ξ)Mpk(ξ)|(x∈I). |
Because n>t, given (5.2), it clearly follows that
supx∈I|˜Fk(x)Mn(x)|≤supx∈I|˜Fk(x)Mt(x)|≤Csupξ∈I|Fk(ξ)Mpk(ξ)|<∞. |
On the other hand, if 1≤q<∞, then, given (5.2), and with the aid of (5.4), we obtain
∫∞0|˜Fk(x)Mn(x)|qdx=∫∞0|˜Fk(x)Mt(x)|q(Mt(x)Mn(x))qdx≤Csupξ∈I|Fk(ξ)Mpk(ξ)|q∫∞0Mt(x)Mn(x)dx=Csupξ∈I|Fk(ξ)Mpk(ξ)|q<∞. |
To complete the induction, it suffices to take pk+1=n and Fk+1=˜Fk.
Lemma 5.2. Let μ≥−12, and let M be a family of functions in C(I) with the property that
supF∈M‖M−1pF‖q≤A(1≤q≤∞) |
for certain p∈N0 and A>0. Then, given k∈N0, there exist pk∈N0, pk≥p, Ck>0, and, for each F∈M, a function gk,F∈C(I) such that
x−μ−12(Dx−1)kxk+μ+12gk,F(x)=F(x)(x∈I) | (5.6) |
and
supF∈M‖M−1pkgk,F‖q≤Ck(1≤q≤∞). | (5.7) |
Proof. The result holds trivially for k=0. Proceeding by induction, fix k∈N0, k≥1. Let pk∈N0, pk≥p, and Ck>0, and, for each F∈M, let gk,F∈C(I) satisfy (5.6) and (5.7). As in the proof of Lemma 5.1, for every F∈M, we construct a function ˜gk,F∈C(I) such that
x−μ−12(Dx−1)k+1x(k+1)+μ+12˜gk,F(x)=F(x)(x∈I),supx∈I|˜gk,F(x)Mn(x)|≤Csupξ∈I|gk,F(ξ)Mpk(ξ)|, |
and
∫∞0|˜gk,F(x)Mn(x)|qdx≤Csupξ∈I|gk,F(ξ)Mpk(ξ)|q(1≤q<∞) |
for some n∈N0, n>pk, where the positive constant C does not depend on F. To complete the proof, it suffices to choose pk+1=n and gk+1,F=˜gk,F, as well as to take into account the inductive hypotheses.
The next result can be analogously established.
Lemma 5.3. Let μ≥−12, and let {Fj}∞j=0 be a sequence of functions in C(I) for which there exists p∈N0 with
limj→∞‖M−1pFj‖q=0(1≤q≤∞). |
Then, for each k∈N0, there exist pk∈N0, pk≥p, and Fk,j∈C(I) (j∈N0) such that
x−μ−12(Dx−1)kxk+μ+12Fk,j(x)=Fj(x)(x∈I, j∈N0) |
and
limj→∞‖M−1pkFk,j‖q=0(1≤q≤∞). |
At this point, we are in a position to give several representations of the elements in the dual space of Sμ in terms of the adjoint of the operator Tμ,k (k∈N0). This will be done in Theorems 5.4 and 5.5. The proof of Theorem 5.4 uses a fairly standard method, which can be traced back to [36] and was already used in [3,4,24], but we include it for the sake of completeness.
Theorem 5.4. Let μ≥−12. A linear functional f belongs to S′μ if, and only if, for every q, 1<q≤∞, there exist r∈N0 and measurable functions gk, with M−1rgk∈Lq(I) (k∈N0, 0≤k≤r), such that
f=x−μ−12r∑k=0(Dx−1)kxk+μ+12 gk(x). | (5.8) |
Proof. Fix q, 1<q≤∞, and let p, 1≤p<∞, be the conjugate exponent of q.
If f∈S′μ, then, by Proposition 4.6, there exist r∈N0 and C>0 such that
|⟨f,φ⟩|≤Cρμp,r(φ)(φ∈Sμ). | (5.9) |
Let us denote by Γp the direct sum of r+1 copies of Lp(I), normed by
‖(fk)0≤k≤r‖p=max0≤k≤r‖fk‖p, | (5.10) |
and by Ξq the direct sum of r+1 copies of Lq(I), normed by
‖(fk)0≤k≤r‖q=r∑k=0‖fk‖q. |
Consider the following injective map:
F:Sμ⟶Γpφ⟼F(φ)=(Mr(x)Tμ,kφ(x))0≤k≤r, |
and define on F(Sμ)⊂Γp the linear functional L by means of the formula
⟨L,F(φ)⟩=⟨f,φ⟩. |
In view of (5.9) and (5.10), L is continuous, and its norm is, at most, C. We continue to denote by L a norm-preserving Hahn-Banach extension of this functional up to Γp. The Riesz representation (fk)0≤k≤r∈Ξq of L over Γp satisfies
‖L‖=r∑k=0‖fk‖q≤C | (5.11) |
and
⟨f,φ⟩=⟨L,F(φ)⟩=r∑k=0∫∞0fk(x)Mr(x)xk+μ+12(x−1D)kx−μ−12φ(x)dx=r∑k=0⟨fk(x),Mr(x)xk+μ+12(x−1D)kx−μ−12φ(x)⟩=r∑k=0⟨x−μ−12(−Dx−1)kxk+μ+12Mr(x)fk(x),φ⟩=⟨x−μ−12r∑k=0(−Dx−1)kxk+μ+12Mr(x)fk(x),φ⟩(φ∈Sμ). |
Setting gk=(−1)kfkMr (k∈N0, 0≤k≤r), we obtain (5.8).
Conversely, if f is given by (5.8), then Hölder's inequality implies that
|⟨f,φ⟩|≤r∑k=0∫∞0|M−1r(x)gk(x)||Mr(x)xk+μ+12(x−1D)kx−μ−12φ(x)|dx≤ρμp,r(φ)r∑k=0‖M−1rgk‖q(φ∈Sμ), |
which yields that f∈S′μ.
Theorem 5.5. For μ≥−12, the following statements are equivalent:
(i) The functional f lies in S′μ.
(ii) There exist k,p∈N0 and a function F∈C(I) such that
f=x−μ−12(Dx−1)kxk+μ+12F(x), | (5.12) |
with
M−1pF∈Lq(I) | (5.13) |
for all q, 1≤q≤∞.
(iii) There exist k,p∈N0 and a function F∈C(I) satisfying (5.12) such that (5.13) holds for some q, 1≤q≤∞.
(iv) There exist k,p∈N0 and a function F∈C(I) satisfying (5.12) such that (5.13) holds for q=∞.
Proof. (i)⇒(ii) If f∈S′μ, Theorem 5.4 yields that p∈N0 and measurable functions Gi (i∈N0, 0≤i≤p) exist such that
f=x−μ−12p∑i=0(Dx−1)ixi+μ+12Gi(x) | (5.14) |
and
M−1pGi∈L∞(I)(i∈N0, 0≤i≤p). | (5.15) |
Apply (N) to get n,t∈N0, n>t>p, for which
∫∞0Mp(x)Mt(x)dx<∞, | (5.16) |
∫∞0Mt(x)Mn(x)dx<∞. | (5.17) |
Fix i∈N0, 0≤i≤p. By (M) and (5.16), we obtain
1Mt(x)∫x0|Gi(ξ)|dξ≤C∫∞0|Gi(ξ)Mp(ξ)|Mp(ξ)Mt(ξ)dξ≤Csupξ∈I|Gi(ξ)Mp(ξ)|∫∞0Mp(ξ)Mt(ξ)dξ=Csupξ∈I|Gi(ξ)Mp(ξ)|(x∈I). | (5.18) |
The function
˜Gi(x)=x−i−μ−12∫x0Gi(ξ)ξi+μ+12dξ(x∈I) |
is continuous and satisfies
x−μ−12(Dx−1)i+1x(i+1)+μ+12˜Gi(x)=x−μ−12(Dx−1)ixi+μ+12Gi(x)(x∈I). |
Using (5.18), we may write
|˜Gi(x)|Mt(x)=1Mt(x)|x−i−μ−12∫x0Gi(ξ)ξi+μ+12dξ|≤1Mt(x)∫x0|Gi(ξ)|dξ≤Csupξ∈I|Gi(ξ)Mp(ξ)|(x∈I). | (5.19) |
As n>t,
supx∈I|˜Gi(x)Mn(x)|≤supx∈I|˜Gi(x)Mt(x)|≤Csupξ∈I|Gi(ξ)Mp(ξ)|<∞. |
Furthermore, taking into account (5.19) and (5.17), we find that
∫∞0|˜Gi(x)Mn(x)|qdx=∫∞0|˜Gi(x)Mt(x)|q(Mt(x)Mn(x))qdx≤Csupξ∈I|Gi(ξ)Mp(ξ)|q∫∞0(Mt(x)Mn(x))qdx≤Csupξ∈I|Gi(ξ)Mp(ξ)|q∫∞0Mt(x)Mn(x)dx=Csupξ∈I|Gi(ξ)Mp(ξ)|q<∞ |
whenever 1≤q<∞. Now, applying Lemma 5.1 with μ+i+1≥−12 instead of μ≥−12, we obtain a function Fi∈C(I) and a non-negative integer si≥n such that
x−(μ+i+1)−12(Dx−1)p−ix(p−i)+(μ+i+1)+12Fi(x)=˜Gi(x)(x∈I), |
with
M−1siFi∈Lq(I)(1≤q≤∞). |
It follows that
x−μ−12(Dx−1)ixi+μ+12Gi(x)=x−μ−12(Dx−1)i+1x(i+1)+μ+12˜Gi(x)=x−μ−12(Dx−1)i+1x(μ+i+1)+12[x−(μ+i+1)−12(Dx−1)p−ix(p−i)+(μ+i+1)+12Fi(x)]=x−μ−12(Dx−1)i+1(Dx−1)p−ix(p+1)+μ+12Fi(x)=x−μ−12(Dx−1)p+1x(p+1)+μ+12Fi(x)(x∈I). |
Set
F=p∑i=0Fi,m=max0≤i≤psi. |
Then, F∈C(I). Using (5.14) and (5.15), we have
f=x−μ−12p∑i=0(Dx−1)ixi+μ+12Gi(x)=x−μ−12(Dx−1)p+1x(p+1)+μ+12p∑i=0Fi(x)=x−μ−12(Dx−1)p+1x(p+1)+μ+12F(x) |
and
M−1mF∈Lq(I)(1≤q≤∞). |
It is thus proved that (i) implies (ii).
(ii)⇒(iii) This is obvious.
(iii)⇒(iv) Suppose that there exist k,p∈N0 and a function F∈C(I) satisfying (5.12) and (5.13) for some q, 1≤q≤∞, and apply (N) to find t∈N0, t>p, such that
∫∞0Mp(x)Mt(x)dx<∞. | (5.20) |
The function
˜F(x)=x−k−μ−12∫x0F(ξ)ξk+μ+12dξ(x∈I) |
is continuous, with
x−μ−12(Dx−1)k+1x(k+1)+μ+12˜F(x)=x−μ−12(Dx−1)kxk+μ+12F(x)=f. |
By choosing n>t and using (M), we obtain
supx∈I|˜F(x)Mn(x)|≤Csupx∈I|x−k−μ−12∫x0F(ξ)Mp(ξ)Mp(ξ)Mt(ξ)Mt(ξ)Mn(ξ)ξk+μ+12dξ|≤C∫∞0|F(ξ)Mp(ξ)|Mp(ξ)Mt(ξ)dξ. |
If q=1, (5.13) and the fact that t>p imply that
supx∈I|˜F(x)Mn(x)|≤C∫∞0|F(ξ)Mp(ξ)|dξ<∞. |
If q=∞, conditions (5.13) and (5.20) yield
supx∈I|˜F(x)Mn(x)|≤Csupξ∈I|F(ξ)Mp(ξ)|∫∞0Mp(ξ)Mt(ξ)dξ<∞. |
Finally, if 1<q<∞, then (5.13), Hölder's inequality, and (5.20) lead to
supx∈I|˜F(x)Mn(x)|≤C{∫∞0|F(ξ)Mp(ξ)|qdξ}1q{∫∞0(Mp(ξ)Mt(ξ))q′dξ}1q′≤C{∫∞0|F(ξ)Mp(ξ)|qdξ}1q{∫∞0Mp(ξ)Mt(ξ)dξ}1q′<∞. |
Here, q′ denotes the conjugate exponent of q. Therefore, (5.12) and (5.13) hold with k+1 instead of k, ˜F instead of F, and n instead of p, when q=∞. This establishes (iv).
(iv)⇒ (i) To complete the proof, assume that there exist k,p∈N0 and F∈C(I) such that
f=x−μ−12(Dx−1)kxk+μ+12F(x), |
with
M−1pF∈L∞(I). |
This representation of f guarantees that f∈S′μ, as it can be deduced from the following estimate:
|⟨f,φ⟩|=|(−1)k∫∞0F(x)xk+μ+12(x−1D)kx−μ−12φ(x)dx|≤supx∈I|F(x)Mp(x)| supx∈I|Mr(x)xk+μ+12(x−1D)kx−μ−12φ(x)| ∫∞0Mp(x)Mr(x)dx≤Cωμr,k(φ)(φ∈Sμ), | (5.21) |
where r>p is chosen according to (N). Thus, (iv) implies (i), and we are done.
Next, we shall characterize boundedness in S′μ. Recall that, under (A), (M), and (N), Sμ is reflexive (Theorem 4.4 and Proposition 2.12), which means that the weak and weak* topologies of S′μ coincide. Furthermore, because Sμ is a Fréchet space (Proposition 4.1), it is barrelled [36, Definition Ⅱ.33.1 and Proposition Ⅱ.33.2, Corollary 1], and, in this class of spaces, the weak* and strong topologies share the same bounded sets [36, Theorem Ⅱ.33.2].
Theorem 5.6. For μ≥−12, the following five statements are equivalent:
(i) The set B⊂S′μ is (weakly, weakly*, strongly) bounded.
(ii) Given q, 1<q≤∞, there exist r∈N0, C>0, and, for each f∈B, measurable functions gk,f (k∈N0, 0≤k≤r) such that
f=x−μ−12r∑k=0(Dx−1)kxk+μ+12gk,f(x), |
with
r∑k=0‖M−1rgk,f‖q≤C. |
(iii) There exist k,p∈N0, C>0, and, for each f∈B, a function gf∈C(I) such that
f=x−μ−12(Dx−1)kxk+μ+12gf(x), | (5.22) |
with
‖M−1pgf‖q≤C | (5.23) |
for any q, 1≤q≤∞.
(iv) There exist k,p∈N0, C>0, and, for each f∈B, a function gf∈C(I) satisfying (5.22) such that (5.23) holds for some q, 1≤q≤∞.
(v) There exist k,p∈N0, C>0, and, for each f∈B, a function gf∈C(I) satisfying (5.22) such that (5.23) holds for q=∞.
Proof. Since Sμ is barrelled, a subset B of S′μ is (weakly, weakly*, strongly) bounded if, and only if, it is equicontinuous [36, Proposition Ⅱ.33.1], which means that (5.9) holds for r∈N0 and C>0 independent of f∈B. Now, (ii) can be obtained by using the same argument as in the proof of Theorem 5.4, taking into account condition (5.11) on the norms of the representing functions.
If (ii) holds, then, in particular, there exist p∈N0, A>0, and, for each f∈B, measurable functions Gi,f (i∈N0, 0≤i≤p) such that
f=x−μ−12p∑i=0(Dx−1)ixi+μ+12Gi,f(x), |
with
p∑i=0‖M−1pGi,f‖∞≤A. |
Fix i∈N0, 0≤i≤p. The argument in the proof that (i) implies (ii) in Theorem 5.5 yields that n∈N0, n>p, ˜A>0, and ˜Gi,f∈C(I) exist such that
x−μ−12(Dx−1)i+1x(i+1)+μ+12˜Gi,f(x)=x−μ−12(Dx−1)ixi+μ+12Gi,f(x)(x∈I), |
supx∈I|˜Gi,f(x)Mn(x)|≤Csupξ∈I|Gi,f(ξ)Mp(ξ)|≤˜A, |
and
∫∞0|˜Gi,f(x)Mn(x)|qdx≤Csupξ∈I|Gi,f(ξ)Mp(ξ)|q≤˜Aq(1≤q<∞), |
where ˜A is independent of f∈B. According to Lemma 5.2, applied with μ+i+1≥−12 instead of μ≥−12, there exist si∈N0, si≥n, Ci>0, and, for each f∈B, a function Fi,f∈C(I) such that
x−(μ+i+1)−12(Dx−1)p−ix(p−i)+(μ+i+1)+12Fi,f(x)=˜Gi,f(x)(x∈I), |
with
‖M−1siFi,f‖q≤Ci(1≤q≤∞). |
Therefore,
x−μ−12(Dx−1)ixi+μ+12Gi,f(x)=x−μ−12(Dx−1)p+1x(p+1)+μ+12Fi,f(x)(x∈I). |
Setting
gf=∑pi=0Fi,f,m=max0≤i≤psi,C=p∑i=0Ci, |
we find that gf∈C(I),
f=x−μ−12(Dx−1)p+1x(p+1)+μ+12gf(x), |
and
‖M−1mgf‖q≤C(1≤q≤∞), |
where m∈N0 and C>0 do not depend on f∈B. Thus, (ii) implies (iii).
It is apparent that (iii) implies (iv).
To prove that (iv) implies (v), assume that there exist k,p∈N0, A>0, and, for each f∈B, a function gf∈C(I) satisfying
f=x−μ−12(Dx−1)kxk+μ+12gf(x) |
with
‖M−1pgf‖q≤A |
for some q, 1≤q≤∞. The argument in the proof that (iii) implies (iv) in Theorem 5.5 allows us to find n∈N0, n>p, ˜A>0, and, for each f∈B, a function ˜gf∈C(I) such that
f=x−μ−12(Dx−1)k+1x(k+1)+μ+12˜gf(x), |
with
supx∈I|˜gf(x)Mn(x)|≤C{∫∞0|gf(ξ)Mp(ξ)|qdξ}1q≤˜A, |
if 1≤q<∞, or
supx∈I|˜gf(x)Mn(x)|≤Csupξ∈I|gf(ξ)Mp(ξ)|≤˜A, |
if q=∞. This establishes (v).
Finally, (v) and (5.21), with gf (f∈B) instead of F, yield (i).
Next, we shall describe sequential convergence in the dual of Sμ. Under (A), (M), and (N), Sμ is Montel and, hence, reflexive (Theorem 4.4 and Proposition 2.12). Thus, the weak and weak* topologies of S′μ coincide, and weak* and strong sequential convergence are equivalent in this space [36, Proposition Ⅱ.34.6, Corollary 1].
Theorem 5.7. For μ≥−12, the following statements are equivalent:
(i) The sequence {fj}∞j=0 converges (weakly, weakly*, strongly) to zero in S′μ.
(ii) For each q, 1<q≤∞, there exist p∈N0 and measurable functions gk,j (k∈N0, 0≤k≤p) such that
fj=x−μ−12p∑k=0(Dx−1)kxk+μ+12gk,j(x)(j∈N0), |
with limj→∞∑pk=0‖M−1pgk,j‖q=0.
(iii) There exist k,p∈N0 and Fj∈C(I) (j∈N0) such that
fj=x−μ−12(Dx−1)kxk+μ+12Fj(x)(j∈N0) | (5.24) |
and
limj→∞‖M−1pFj‖q=0 | (5.25) |
for any q, 1≤q≤∞.
(iv) There exist k,p∈N0 and Fj∈C(I) (j∈N0) satisfying (5.24) and (5.25) for some q, 1≤q≤∞.
(v) There exist k,p∈N0 and Fj∈C(I) (j∈N0) satisfying (5.24) and (5.25) for q=∞.
(vi) There exist k,p∈N0, C>0, and Fj∈C(I) (j∈N0) satisfying (5.24), with
‖M−1pFj‖∞≤C(j∈N0) |
and limj→∞Fj(x)=0 for almost all x∈I.
Proof. To show that (i) implies (ii), suppose that {fj}∞j=0 converges to zero in S′μ. Then [24, Equation (5.7)], there exist p∈N0 and positive constants {Cj}∞j=0 such that
|⟨fj,φ⟩|≤Cj‖φ‖μ,∞,p(φ∈Sμ, j∈N0) |
and limj→∞Cj=0. On the other hand (Proposition 4.6), given q, 1<q≤∞, there exist C>0 and r∈N0 such that
‖φ‖μ,∞,p≤Cρμq,r(φ)(φ∈Sμ). |
It follows that
|⟨fj,φ⟩|≤Cjρμq,r(φ)(φ∈Sμ, j∈N0), | (5.26) |
where the redefined sequence {Cj}∞j=0 still satisfies
limj→∞Cj=0. | (5.27) |
Now, it suffices to provide the same argument as in the proof of Theorem 5.4, using (5.26) instead of (5.9) and keeping in mind (5.27) in relation to (5.11).
Parts (iv) and (vi) follow trivially from (iii) and (v), respectively.
The arguments in the proof of the corresponding results for Theorems 5.5 and 5.6, in combination with Lemma 5.3 instead of Lemmas 5.1 and 5.2, allow us to establish that (ii) implies (iii) and (iv) implies (v); we omit the details.
Finally, assuming that (vi) holds, to obtain (i), it suffices to choose n∈N0, n>p, according to (N) and apply Lebesgue's dominated convergence theorem to the following integrals:
⟨fj,φ⟩=(−1)k∫∞0Fj(x)Mp(x)Mp(x)Mn(x)Mn(x)Tμ,kφ(x)dx(φ∈Sμ, j∈N0). |
This completes the proof.
Theorems 5.4–5.7 characterize the structure, boundedness, and convergence in the dual of a wide range of spaces that arise in the context of the Hankel transformation (see Sections 2 and 3.4). For illustrative purposes, in Corollary 5.8, some of those results have been specialized for the Zemanian space Hμ, which, as already mentioned (Example 2.2), is none other than the Hankel-K{Mp} space defined by the sequence of weights {(1+x2)p}∞p=0.
The application of Theorem 5.4 to Hμ is as stated in [4, Theorem 5.5]. However, the representation of the elements in H′μ obtained as a consequence of Theorem 5.5 is an improvement upon the result of [4] in three ways. First, it involves the Tμ,k-distributional derivative (k∈N0) of a single continuous function F. Second, the representing function F is not dependent on the exponent q; in fact, the products of F and the inverses of the weights belong to all classes Lq(I), 1≤q≤∞. Finally, as we have just highlighted, and unlike what occurs in Theorem 5.4, q=1 is included in the range of exponents for which the representation is valid.
Remarks analogous to the preceding ones can be made regarding Theorem 5.7; particularly, the application of part (ii) to the space Hμ is as stated in [4, Theorem 5.4], while parts (iii) to (v) improve upon this result along the lines described above.
Reference [4] contains no analogue of Theorem 5.6.
Corollary 5.8. Let H′μ be the dual space of Hμ. Then, the following holds:
(i) A functional f belongs to H′μ if, and only if, there exist k,p∈N0 and a function F∈C(I) such that
f=x−μ−12(Dx−1)kxk+μ+12F(x), |
with
(1+x2)−pF(x)∈Lq(I)(1≤q≤∞). |
(ii) A set B⊂H′μ is (weakly, weakly*, strongly) bounded if, and only if, there exist k,p∈N0, C>0, and, for every f∈B, a function gf∈C(I) such that
f=x−μ−12(Dx−1)kxk+μ+12gf(x), |
with
‖(1+x2)−pgf(x)‖q≤C(1≤q≤∞). |
(iii) A sequence {fj}∞j=0 converges (weakly, weakly*, strongly) to zero in H′μ if, and only if, there exist k,p∈N0 and gj∈C(I) such that
fj=x−μ−12(Dx−1)kxk+μ+12gj(x)(j∈N0), |
with
limj→∞‖(1+x2)−pgj(x)‖q=0(1≤q≤∞). |
In Friedman's opinion [10, p. 37], one of the most interesting and important problems in the theory of generalized functions or distributions is to find their structure, that is, to express them in terms of differential operators acting on functions or on measures. This paper provides novel results in this direction for the spaces of type Hankel-K{Mp}. Namely, here it was shown that, for μ≥−12, and under certain conditions on the weights {Mp}∞p=0, the elements, the (weakly, weakly*, strongly) bounded subsets, and the (weakly, weakly*, strongly) convergent sequences in the dual of a space Kμ of type Hankel-K{Mp} can be represented as distributional derivatives of functions and of measures that satisfy good properties, not only in terms of the differential operator x−1D and of the Bessel operator Sμ=x−μ−12Dx2μ+1Dx−μ−12, but also in terms of suitable iterations Tμ,k (k∈N0) of the Zemanian differential operator Nμ=xμ+12Dx−μ−12. To this end, new descriptions for the usual topology of Kμ in terms of the latter iterations were given.
The operators Tμ,k are defined by Tμ,k=Nμ+k−1⋯Nμ for k∈N, while Tμ,0 is the identity operator. The interest of such operators lies in their symmetric behavior with respect to hμ, the Hankel transformation of order μ. Indeed, given φ∈L1(I), we define
(hμφ)(y)=∫∞0φ(x)(xy)12Jμ(xy)dx(y∈I), |
where I=]0,∞[ and Jμ is the Bessel function of the first kind and order μ. For a sufficiently smooth φ with a good boundary behavior, the identity
(−y)mTμ,k(hμφ)(y)=∫∞0(−x)kTμ,mφ(x)(xy)12Jμ+k+m(xy)dx=hμ+k+m[(−x)kTμ,mφ(x)](y)(y∈I, m,k∈N0) |
holds [40, Proof of Theorem 5.4-1]. This rule closely resembles its Fourier counterpart and facilitates the operational calculus of the Hankel transformation, particularly when dealing with the Zemanian space Hμ [38,39], which can be regarded as a paradigm for the spaces of type Hankel-K{Mp}. In fact, the specialization to Hμ of the results obtained in our work improves upon previous results from [4]. The findings of the present paper are thus expected to pave the way for a time-frequency analysis of the spaces Kμ.
Samuel García-Baquerín and Isabel Marrero: Conceptualization, Methodology, Investigation, Writing – Original Draft, Writing – Review & Editing. All authors of this article have contributed equally. Isabel Marrero: Supervision, Project Administration. All authors have read and approved the final version of the manuscript for publication.
The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.
Samuel García-Baquerín would like to thank the Departamento de Análisis Matemático and the Instituto de Matemáticas y Aplicaciones (IMAULL) at the Universidad de La Laguna for their hospitality during the preparation of this paper.
The authors declare they have no conflict of interest.
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