Some new restricted maximal operators of Fej\'er means of Walsh-Fourier series in the space $H_{1/2}$
Davit Baramidze, Lars-Erik Persson, George Tephnadze

TL;DR
This paper identifies the largest subset of natural numbers for which a restricted maximal operator of Fejér means of Walsh-Fourier series remains bounded from the Hardy space $H_{1/2}$ to $L_{1/2}$, and proves the result's optimality.
Contribution
It determines the maximal subspace of natural numbers ensuring boundedness of the restricted maximal operator in Walsh-Fourier series, establishing the sharpness of this characterization.
Findings
Identified the maximal subset of natural numbers for boundedness.
Proved the boundedness of the restricted maximal operator.
Established the sharpness of the main result.
Abstract
In this paper we derive the maximal subspace of natural numbers , such that the restricted maximal operator, defined by on this subspace of Fej\'er means of Walsh-Fourier series is bounded from the martingale Hardy space to the Lebesgue space . The sharpness of this result is also proved.
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Taxonomy
TopicsAdvanced Harmonic Analysis Research · Differential Equations and Boundary Problems · Holomorphic and Operator Theory
Some now restricted maximal operators of Fejér means of Walsh-Fourier series in the space
Davit Baramidze, Lars-Erik Persson and George Tephnadze
D. Baramidze, The University of Georgia, School of science and technology, 77a Merab Kostava St, Tbilisi 0128, Georgia and Department of Computer Science and Computational Engineering, UiT - The Arctic University of Norway, P.O. Box 385, N-8505, Narvik, Norway.
L.-E. Persson, UiT The Arctic University of Norway, P.O. Box 385, N-8505, Narvik, Norway and Department of Mathematics and Computer Science, Karlstad University, 65188 Karlstad, Sweden.
G. Tephnadze, The University of Georgia, School of science and technology, 77a Merab Kostava St, Tbilisi 0128, Georgia.
Abstract.
In this paper we derive the maximal subspace of natural numbers , such that the restricted maximal operator, defined by on this subspace of Fejér means of Walsh-Fourier series is bounded from the martingale Hardy space to the Lebesgue space The sharpness of this result is also proved.
The research was supported by Shota Rustaveli National Science Foundation grant no. PHDF-21-1702.
2020 Mathematics Subject Classification. 26015, 42C10, 42B30.
Key words and phrases: Walsh system, Fejér means, martingale Hardy space, maximal operators, restricted maximal operators.
1. INTRODUCTION
All symbols used in this introduction can be found in Section 2.
In the one-dimensional case, the weak (1,1)-type inequality for the maximal operator of Fejér means with respect to the Walsh system, defined by
[TABLE]
was investigated in Schipp [19] and Pál, Simon [12] (see also [1], [10] and [16]). Fujii [3] and Simon [21] proved that is bounded from to . Weisz [32] generalized this result and proved boundedness of from the martingale space to the Lebesgue space for . Simon [20] gave a counterexample, which shows that boundedness does not hold for A counterexample for was given by Goginava [5]. Moreover, in [6] (see also [23]) he proved that there exists a martingale such that
[TABLE]
Weisz [35] proved that the maximal operator of the Fejér means is bounded from the Hardy space to the space .
The boundedness of weighted maximal operators are considered in [24], [25]. The results for summability of Fejér means of Walsh-Fourier series can be found in [2], [9], [11], [14], [28], [32].
To study convergence of subsequences of Fejér means and their restricted maximal operators on the martingale Hardy spaces for the central role is played by the fact that any natural number can be uniquely expression as
[TABLE]
where only a finite numbers of differ from zero and their important characters and are defined by
[TABLE]
and
[TABLE]
Weisz [34] (see also [33]) also proved that for any the maximal operator
[TABLE]
is bounded from the Hardy space to the Lebesgue space , but (for details see [17]) it is not bounded from the Hardy space to the space Persson and Tephnadze [15] generalized this result and proved that if and is a sequence of positive numbers, such that
[TABLE]
then the maximal operator defined by
[TABLE]
is bounded from the Hardy space to the Lebesgue space Moreover, if and is a sequence of positive numbers, such that
[TABLE]
then there exists a martingale such that
[TABLE]
From this fact it follows that if and is any sequence of positive numbers, then the maximal operator, defined by (2) is bounded from the Hardy space to the space if and only if the condition (1) is fulfilled. Moreover, if and is any sequence of positive numbers, then are uniformly bounded from the Hardy space to the Lebesgue space if and only if the condition (1) is fulfilled. Moreover, condition (1) is necessary and sufficient condition for the boundedness of subsequence from the Hardy space to the Hardy space
It is easy to prove that condition (1) also implies that the maximal operator (2) is bounded from the Hardy space to the Lebesgue space Moreover, for the subsequence we have that
[TABLE]
but the maximal operator
[TABLE]
is bounded from the Hardy space to the Lebesgue space
In [30] it was proved that if then there exists an absolute constant such that
[TABLE]
Moreover, if is a subsequence of positive integers such that
[TABLE]
and is any nondecreasing, nonnegative sequence, satisfying the conditions and
[TABLE]
then there exists a martingale such that
[TABLE]
It follows that if and is any sequence of positive numbers, then are bounded from the Hardy space to the space if and only if, for some
[TABLE]
Convergence of subsequences of partial sums and Fejér means of Walsh-Fourier series can be found in [13], [26], [27] and [31].
In this paper we complement the reported research above by investigating the limit case In particular, we derive the maximal subspace of natural numbers , such that restricted maximal operator, defined by on this subspace of Fejér means of Walsh-Fourier series is bounded from the martingale Hardy space to the Lebesgue space
This paper is organized as follows: In order not to disturb our discussions later on some definitions and notations are presented in Section 2. The main result and some of its consequences can be found in Section 3. For the proof of the main result we need some auxiliary statements, some of them are new and of independent interest (see Propositions 1 and 2). These results are presented in Section 4. The detailed proofs are given in Section 5.
2. Definitions and Notations
Let denote the set of the positive integers, Denote by the discrete cyclic group of order 2, that is where the group operation is the modulo 2 addition and every subset is open. The Haar measure on is given so that the measure of a singleton is 1/2.
Define the group as the complete direct product of the group with the product of the discrete topologies of . The elements of are represented by sequences where
It is easy to give a base for the neighborhood of
[TABLE]
Denote and for . Then it is easy to prove that
[TABLE]
If then every can be uniquely expressed as where and only a finite numbers of differ from zero.
Let
[TABLE]
that is Set
[TABLE]
Define the variation of with binary coefficients by
[TABLE]
Every can be also represented as For such a representation of we denote numbers
[TABLE]
Let For such which can be written as
[TABLE]
where we define
[TABLE]
where We note that
Let us denote the cardinality of the set by , that is
[TABLE]
It is evident that
[TABLE]
Moreover, if and only if
We note that if then each has bounded variation
[TABLE]
and
Therefore, if we consider blocks (intervals)
[TABLE]
then it is easy to see that it contains different blocks. Therefore, the dyadic representation of different natural numbers, which contains blocks from (6), can be at most which is a finite number and the set is finite for all , from which it follows that
[TABLE]
Summing up, we can conclude that if and only if the set is finite for all and each has bounded variation, that is, conditions (5) and (7) are fullfiled.
The norms (or quasi-norm) of the spaces and are, respectively, defined by
[TABLE]
The -th Rademacher function is defined by
[TABLE]
Now, define the Walsh system on as:
[TABLE]
The Walsh system is orthonormal and complete in (see [18]).
If then we can define the Fourier coefficients, partial sums of Fourier series, Fejér means, Dirichlet and Fejér kernels in the usual manner:
[TABLE]
Recall that (see [18])
[TABLE]
[TABLE]
The -algebra, generated by the intervals will be denoted by Denote by a martingale with respect to (for details see e.g. [33]). The maximal function of a martingale is defined by
[TABLE]
In the case the maximal functions are also given by
[TABLE]
For the Hardy martingale spaces consist of all martingales, for which
[TABLE]
A bounded measurable function is a -atom, if there exists an interval such that
[TABLE]
It is easy to check that for every martingale and every the limit
[TABLE]
exists and it is called the -th Walsh-Fourier coefficients of
The Walsh-Fourier coefficients of are the same as those of the martingale obtained from .
3. The Main Result and its Consequences
Our main result reads:
Theorem 1**.**
a) Let and be a sequence of positive numbers and let be numbers such that If the sets defined by (2), are finite for all that is the cardinality of the sets are finite:
[TABLE]
then the restricted maximal operator defined by
[TABLE]
is bounded from the Hardy space to the Lebesgue space .
b) (sharpness) Let
[TABLE]
Then there exists a martingale such that the maximal operator, defined by (10), is not bounded from the Hardy space to the Lebesgue space
In particular, Theorem 1 implies the following optimal characterization:
Corollary 1**.**
Let and be a sequence of positive numbers. Then the restricted maximal operator defined by (10), is bounded from the Hardy space to the Lebesgue space if and only if any sequence of positive numbers which satisfies is finite for each and each has bounded variation, i.e.
[TABLE]
In order to be able to compare with some other results in the literature (see Remark 1) we also state the following:
Corollary 2**.**
Let . Then the restricted maximal operators defined by
[TABLE]
[TABLE]
[TABLE]
where denotes the integer part of , are all bounded from the Hardy space to the Lebesgue space .
Remark 1**.**
In [15] it was proved that if then the restricted maximal operators and defined by (12) and (13), are not bounded from the Hardy space to the Lebesgue space .
On the other hand, in [15] it was proved that if , then the restricted maximal operator defined by is bounded from the Hardy space to the Lebesgue space
We also have the following related consequence of Theorem 1:
Corollary 3**.**
Let and be a sequence of positive numbers, defined by
[TABLE]
Then the restricted maximal operator defined by
[TABLE]
is not bounded from the Hardy space to the Lebesgue space
Remark 2**.**
We note that in this case for any and
[TABLE]
i.e. it contains only two elements, the set
[TABLE]
and
[TABLE]
Finally, we state the following related result, which is connected to the research in [30] (see Remark 4):
Corollary 4**.**
Let and be a sequence of positive numbers, defined by
[TABLE]
Then the restricted maximal operator defined by
[TABLE]
is not bounded from the Hardy space to the Lebesgue space
Remark 3**.**
We note that now for any and
[TABLE]
and
[TABLE]
Remark 4**.**
Let and and be a sequence of positive numbers, defined in Corollaries 3 and 4. Then there exist absolute constants and such that
[TABLE]
and
[TABLE]
for any
We note that these results were proved in [30] and they follow, respectively, from the facts that
[TABLE]
4. Auxiliary Lemmas and Propositions
Lemma 1** (Weisz [34] (see also Simon [22])).**
A martingale is in if and only if there exists a sequence of p-atoms and a sequence of a real numbers, such that for every
[TABLE]
Moreover,
[TABLE]
where the infimum is taken over all decomposition of of the form (14).
Lemma 2** (Weisz [33]).**
Suppose that an operator is -linear and
[TABLE]
for every -atom , where denote the support of the atom. If is bounded from to then
[TABLE]
Lemma 3** (see e.g. [4]).**
Let Then
[TABLE]
Lemma 4** (see e.g. [7], [25]).**
Let and
[TABLE]
Then
[TABLE]
Lemma 5** (see [29]).**
Let
[TABLE]
Then, for any
[TABLE]
where
We also need the following new statement of independent interest:
Proposition 1**.**
Let
[TABLE]
Then, for any
[TABLE]
Proof.
It is evident that we always have that If then and if we apply Lemma 5 we find that
[TABLE]
Let By combining (8) and Lemma 3, for any we get that
[TABLE]
From (9), for we can conclude that
[TABLE]
[TABLE]
Suppose that Since
[TABLE]
for we find that
[TABLE]
Moreover, by combining (8) and Lemma 3 we get that
[TABLE]
For we have that
[TABLE]
Moreover, can be estimated as follows
[TABLE]
By combining (17)-(19) and putting them into (4) we obtain that
[TABLE]
If we get that . Hence, by using (15) we find that
[TABLE]
By simple calculations we get that
[TABLE]
[TABLE]
and
[TABLE]
We insert (22)-(24) into (21) and find that
[TABLE]
The proof is complete by just combining the estimates (20) and (25). ∎
Corollary 5**.**
Let
[TABLE]
Then, for any
[TABLE]
and
[TABLE]
where
Our second auxiliary result of independent interest is the following:
Proposition 2**.**
Let
[TABLE]
Then
[TABLE]
Proof.
Let By using (9) we get that
[TABLE]
For we have that
[TABLE]
[TABLE]
[TABLE]
[TABLE]
Since and
[TABLE]
we obtain that
[TABLE]
[TABLE]
Thus, by using the estimates
[TABLE]
we can conclude that
[TABLE]
Let for some Then
[TABLE]
If for some then
[TABLE]
Hence,
[TABLE]
Finally, we use the estimates (27)-(28) in (4) and the proof is complete. ∎
5. Proof of the Theorem 1
Proof.
Since is bounded from to by Lemma 2, the proof of theorem 1 will be complete, if we prove that
[TABLE]
for every 1/2-atom We may assume that is an arbitrary -atom, with support and It is easy to see that
[TABLE]
Therefore, we can suppose that
Let and for some Since
[TABLE]
by using Proposition 2 we obtain that
[TABLE]
If we denote by
[TABLE]
from (5) we can conclude that
[TABLE]
and
[TABLE]
Hence,
[TABLE]
Since we obtain that (29) holds so that Theorem 1 a) is proved if we can prove that
[TABLE]
and
[TABLE]
for all and . Indeed, if (32) and (33) hold, from (5) we get that
[TABLE]
It remains to prove (32) and (33). Let
[TABLE]
If then and if we apply Lemma 3 we obtain that
[TABLE]
Let Then and if we use Lemma 3 we get that
[TABLE]
so that
[TABLE]
Analogously to (35) we can prove that if , then
[TABLE]
so that
[TABLE]
Let
[TABLE]
Let or Since and if we apply Lemma 3 we obtain that
[TABLE]
and
[TABLE]
Let Since and if we apply Lemma 3, then we find that
[TABLE]
and
[TABLE]
Let By combining (3) with (34)-(38) for any we have that
[TABLE]
Analogously we can prove that (33) holds also for the case Hence, (33) holds and it remains to prove (32).
Let If since by using (8) we have that
[TABLE]
If then by using (8) we obtain that
[TABLE]
Let By combining (3), (39) and (40) we get that
[TABLE]
If then and apply (39) we get that
[TABLE]
and also (32) is proved by just combining (5) and (42) so part a) is complete and we turn to the proof of b).
Under condition (11), there exists an increasing sequence of positive integers, such that
[TABLE]
Let
[TABLE]
where
[TABLE]
Since \text{supp}(a_{k})=I_{\left|\alpha_{k}\right|},\ \ \ \left\|a_{k}\right\|_{\infty}\leq 2^{2\left|\alpha_{k}\right|}=\mu(\text{supp }a_{k})^{-2}\ \ and
[TABLE]
if we apply Lemma 1 and (43) we can conclude that
It is easy to prove that
[TABLE]
Let By using (44) we get that
[TABLE]
Let Then, by using (45) we find that
[TABLE]
Since
[TABLE]
we obtain that
[TABLE]
By combining the well-known estimates (see [17])
[TABLE]
we obtain that
[TABLE]
Let be natural numbers which generates the set
[TABLE]
and choose number where
[TABLE]
for some such that
Since by using Corollary 5 we get that
[TABLE]
On the other hand, we can also choose number for some such that According to the fact that by using again Corollary 5 for some and we also get that
[TABLE]
By combining (5)-(5) with Proposition 1 for sufficiently big we get that
[TABLE]
so also part b) is proved and the proof is complete. ∎
The reference list from the paper itself. Each links out to its DOI / PubMed record.
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- 2[2] I. Blahota, G. Tephnadze, Strong convergence theorem for Vilenkin-Fejér means, Publ. Math. Debrecen 85 (1-2) (2014), 181-196.
- 3[3] N. J. Fujii, A maximal inequality for H 1 subscript 𝐻 1 H_{1} functions on the generalized Walsh-Paley group, Proc. Amer. Math. Soc. 77 (1979), 111-116.
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- 5[5] U. Goginava, Maximal operators of Fejér means of double Walsh-Fourier series. Acta Math. Hungar. 115 (2007), 333–340.
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