Atomic Decompositions and John-Nirenberg Theorem of Grand Martingale Hardy Spaces with Variable Exponents
Abstract
Let θ ≥ 0 and p(·) be a variable exponent, and we introduce a new class of function spaces Lp(·),θ in a probabilistic setting which unifies and generalizes the variable Lebesgue spaces with θ = 0 and grand Lebesgue spaces with p(·) ≡ p and θ = 1. Based on the new spaces, we introduce a kind of Hardy-type spaces, grand martingale Hardy spaces with variable exponents, via the martingale operators. The atomic decompositions and John-Nirenberg theorem shall be discussed in these new Hardy spaces.
1. Introduction
The martingale theory is widely studied in the field of mathematical physics, stochastic analysis, and probability. Weisz [1] presented the atomic decomposition theorem for martingale Hardy spaces. Herz [2] established the John-Nirenberg theorem for martingales. Since then, the study of martingale Hardy spaces associated with various functional spaces has attracted a steadily increasing interest. For instance, martingale Orlicz-type Hardy spaces were investigated in [3–6], martingale Lorentz Hardy spaces were studied in [7–9], and variable martingale Hardy spaces were developed in [10–14].
Such spaces can be used to integrate the Jacobian under minimal hypotheses [15]. The grand Lebesgue spaces as a kind of Banach function space were investigated in the papers of Capone et al. [16, 17], Fiorenza et al. [18–21], Kokilashvili et al. [22, 23], and so forth. In particular, grand Lebesgue spaces with variable exponents were studied in [24, 25].
We find that the framework of grand Lebesgue spaces with variable exponents has not yet been studied in martingale theory. This paper is aimed at discussing the variable grand Hardy spaces defined on the probabilistic setting and showing the atomic decompositions and John-Nirenberg theorem in these new Hardy spaces. More precisely, we first present the atomic characterization of grand Hardy martingale spaces with variable exponents. To do so, we introduce the following new notations of atom.
Definition 1. Let p(·) be a variable exponent and θ ≥ 0. A measurable function a is called a (1, p(·), θ) -atom (resp. (2, p(·), θ) -atom, (3, p(·), θ) -atom) if there exists a stopping time τ such that
(a1), ∀ n ≤ τ
(a2)
See Theorem 11 for the details. This conclusion improves the recent results [12, 26], respectively.
Throughout this paper, ℤ, ℕ, and ℂ denote the integer set, nonnegative integer set, and complex numbers set, respectively. We denote by C the absolute positive constant, which can vary from line to line. The symbol A≲B stands for the inequality A ≤ CB. If we write A ≈ B, then it stands for A≲B≲A.
2. Preliminaries
2.1. Grand Lebesgue Spaces with Variable Exponents
Based on this, we begin with the definition of the grand Lebesgue space with variable exponent.
Definition 2. Suppose that and θ ≥ 0. We define the grand Lebesgue space with variable exponent Lp(·),θ = Lp(·),θ(Ω) as the set of all -measurable functions f satisfying
The Grand Lebesgue space with variable exponent can unify and generalize the various function spaces. To be precise, if θ = 0, Lp(·),θ degenerates to the variable Lebesgue space Lp(·). If θ = 1 and p(·) ≡ p, Lp(·),θ becomes the grand Lebesgue space Lp).
2.2. Martingale Grand Hardy Spaces via Variable Exponents
Remark 3. If θ = 0, then we obtain the definitions of , , , Qp(·), and Dp(·), respectively (see [10, 12, 27]). If we consider the special case θ = 1 and p(·) ≡ p with the notations above, we obtain the definitions of , , , Qp), and Dp), respectively (see [26]). In addition, if p(·) ≡ p and θ = 0, we obtain the martingale Hardy spaces , , , Qq, and Dq, respectively (see [28]).
Refer to [29, 30] for more information on martingale theory.
3. Atomic Characterization
The method of atomic characterization plays an useful tool in martingale theory (see for instance [1, 4, 6, 31–33]). We shall construct the atomic characterizations for grand Hardy martingale spaces with variable exponents in this section.
Theorem 4. Let and θ ≥ 0. If the martingale , then there exists a sequence of triplet so that for each n ≥ 0,
Conversely, if the martingale f has a decomposition of (14), then
Proof. Let . Now consider the stopping time for each k ∈ ℤ:
It is easy to see that the sequence of these stopping times is nondecreasing. For each stopping time τ, denote . It is easy to write that
For each k ∈ ℤ, let . If μk ≠ 0, we set
If μk = 0, we set for each n ∈ ℕ. For each fixed k ∈ ℤ, is a martingale. Since , we get
We can easily check that is a bounded L2-martingale. Hence, there exists an element ak ∈ L2 such that . If n ≤ τk, then , and . Consequently, it implies that ak is really a (1, p(·), θ)-atom.
Denote Λk≔{τk<∞}. Knowing that {τk<∞} = {s(f) > 2k} and τk is nondecreasing for each k ∈ ℤ, we obtain Λk+1⊆Λk. Now, we point out that
Indeed, for a fixed x0 ∈ Ω, there is k0 ∈ ℤ so that and , then we have
This means
For the converse part, according to the definition of (1, p(·), θ)-atom, we easily conclude
This implies
Taking over all the admissible representations of (14) for f, we obtain the desired result.
Next, we will characterize Qp(·),θ and Dp(·),θ by atoms, respectively. The proof is similar to the proof of Theorem 4. For the completeness of this paper, we provide some details.
Theorem 5. Suppose and θ ≥ 0. If the martingale (resp. Dp(·),θ), then there exists a sequence of triplet (resp. ) so that for each n ∈ ℕ,
Conversely, if the martingale has admissible representation (27), then f ∈ Qp(·),θ (resp. Dp(·),θ) and
Proof. The proof follows the ideas in Theorem 4, so we omit some details. Suppose (resp. Dp(·),θ). We define stopping times as follows:
Let and be defined as in the proof of Theorem 4. And replace Λk = {τk<∞} = {s(f) > 2k} by the Λk = {τk<∞} = {λ∞ > 2k}. Then, we obtain that and (28) still hold.
For the converse part, write
Clearly, is a nonnegative, nondecreasing, and adapted sequence with Sn+1(f) ≤ λn (resp.∣fn | ≤λn). Thus, we get
Taking over all the admissible representations of (27) for f, we obtain the desired result.
Remark 6. Suppose and θ ≥ 0. We conclude that the sum in Theorem 4 converges to f in as M⟶−∞, N⟶∞. Indeed, it follows by the subadditive of the operator s, we get, for any M, N ∈ ℤ with M < N,
Furthermore, we can also show the norm convergence of the summation in Theorems 5 as M⟶−∞, N⟶∞.
4. The Generalized John-Nirenberg Theorem
Definition 7. For and θ ≥ 0, the generalized BMO martingale space is defined by
Remark 8. If θ = 0, BMOp(·),θ degenerates to the variable exponent BMO martingale space BMOp(·) introduced and studied in [12]. If θ = 1 and p(·) ≡ p, BMOp(·),θ becomes the grand BMO martingale space BMOp) studied in [26].
In order to establish the generalized John-Nirenberg theorem in the framework of BMOp(·),θ, we need the following lemmas and notations.
Lemma 9 (Hölder’s inequality, see [34]). Let satisfy
Then, there exists a constant C such that for all f ∈ Lp(·) and g ∈ Lq(·), we have fg ∈ Lr(·) and
Lemma 10 (see [27].)Suppose satisfying (43).
- (1)
For each , we get
- (2)
Let satisfy (43). If r(·) satisfies
Theorem 11. Suppose that satisfies (43) and θ ≥ 0. Then, for every f ∈ BMO1, there has
Proof. If satisfies (43), then we clearly get that p(·) − η also satisfies (43) for 0 < η < p− − 1. It follows from Lemmas 9 and 10 that
This is equivalent to the following inequality:
Hence, we have
Taking the supremum over all stopping times, we deduce
Conversely, from the definition of Lp(·),θ, we get
It follows from Lemma 9 that
Hence, by (38), we deduce that
From what has been discussed above, we draw the conclusion that
Theorem 11 improves the recent results [12, 26], respectively. More precisely, if we consider the case θ = 0, then the following result holds:
Corollary 12. If p(·) satisfies (43) with 1 < p− ≤ p+ < ∞, then for f ∈ BMO1,
And especially for θ = 1 and p(·) ≡ p, we get the conclusion as follows.
Corollary 13 (see [26].)Suppose 1 < p < ∞, then for f ∈ BMO1,
Conflicts of Interest
The authors declare that they have no conflicts of interest.
Acknowledgments
This project is partially supported by the National Natural Science Foundation of China (Grant Nos. 11801001 and 12101223), Scientific Research Fund of Hunan Provincial Education Department (Grant No. 20C0780), and Scientific Research Fund of Hunan University of Science and Technology (Grant Nos. E51997 and E51998).
Open Research
Data Availability
No data is used in the manuscript.