p-Adic Riesz Potential and Its Commutators on Morrey-Herz Spaces
Abstract
In this paper, we establish the boundedness of p-adic Riesz potential on Morrey-Herz spaces, as well as the λ-central BMO estimates for multilinear commutators of p-adic Riesz potential on Morrey-Herz spaces.
1. Introduction
- (i)
|x|p ≥ 0, ∀x ∈ ℚp, and |x|p = 0⇔x = 0
- (ii)
|xy|p = |x|p|y|p, ∀x, y ∈ ℚp
- (iii)
|x + y|p ≤ max(|x|p, |y|p), ∀x, y ∈ ℚp and when |x|p ≠ |y|p, we have |x + y|p = max(|x|p, |y|p)
In the last several decades, there has been growing interest in the p-adic models appearing in various branches of science. The p-adic analysis has cemented its role in the field of mathematical physics (see, for example, [4, 5]). Many researchers have also paid relentless attention to harmonic analysis on the p-adic fields [6–18]. It is well known that the Riesz potential operator in harmonic analysis is one of the most important operators and plays an important role in many areas such as Sobolev spaces, potential theory, and PDE, to name a few.
When n = 1, Haran [6, 7] obtained the explicit formula of the Riesz potential on ℚp. Taibleson [3] gave the fundamental analytic properties of on local fields. In particular, Kim [8] gave the p-adic Hardy-Littlewood-Sobolev theorem on , which implies is bounded from to when q > 1 and is of weak type (q, r) when q = 1, where 0 < Re(α) < n and 1/r = 1/q − Re(α)/n > 0. Later on, Volosivets [11, 12] extended the theorem to p-adic generalized Morrey spaces and showed analogs of the results in Euclidean space ℝn given by Nakai [19]. Also, Wu and Fu [9] established counterparts of the theorem on p-adic central Morrey spaces. Additionally, Lu and Xu [20] extended Morrey spaces and introduced Morrey-Herz spaces in the setting of ℝn, and they also gave the Hardy-Littlewood-Sobolev inequalities on the spaces, which led many scholars to study the boundedness of on Morrey-Herz spaces, for details, see [21, 22]. The first aim of the current paper is to study the boundedness of the Riesz potential on Morrey-Herz spaces over the p-adic fields.
Theorem 1. Let α be a complex number with 0 < Re(α) < n, 1/r = 1/q − Re(α)/n with 1 ≤ q < r < ∞, λ ≥ 0, λ − n/q + Re(α) < σ < n(1 − 1/q), 0 < l ≤ s ≤ ∞. If q > 1, then, there exists a constant C > 0 such that
Moreover, if q = 1, then, there exists a constant C > 0 such that
Remark 2. The definitions of the homogeneous Morrey-Herz spaces and weak homogeneous Morrey-Herz spaces will be given in Section 2, here, we point out that for 1 ≤ r < ∞. We observe that Theorem 1 is counterparts of famous Hardy-Littlewood-Sobolev theorem on p-adic Morrey-Herz spaces. In addition, Theorem 1 coordinates with those on Morrey-Herz spaces in the setting of ℝn, which was proved by Lu and Xu [20].
Moreover, let b = (b1, b2, ⋯, bm), where for 1 ≤ i ≤ m, m ∈ ℕ. Then, multilinear commutator generated by b and can be defined as follows:
When m = 1, Wu and Fu [9] obtained the λ-central BMO estimates for commutator on p-adic central Morrey spaces. Furthermore, Mo et al. [13] considered multilinear case for m ≥ 1 and established the boundedness of with symbols in Campanato spaces on p-adic generalized Morrey spaces. Motivated by the works, our second goal is to show the λ-central BMO estimates for the multilinear commutator on Morrey-Herz spaces over the p-adic fields.
Theorem 3. Let α be a complex number with 0 < Re(α) < n, 1/r = 1/q1 + 1/q2 + ⋯+1/qm + 1/q − Re(α)/n, where r > n/(n − Re(α)) and 1 < q, q1, ⋯, qm < ∞. λ ≥ 0, 0 < l ≤ s ≤ ∞, ν = ν1 + ν2 + ⋯+νm with 0 ≤ ν1, ν2, ⋯, νm < 1/n, nν + λ − n/q + Re(α) < σ1 < n(1 − 1/q) + λ, σ2 = σ1 − n(1/q1 + 1/q2+⋯+1/qm + ν). If , then, there exists a constant C > 0 such that
We notice that the important particular case of λ-central BMO spaces is defined in [14] when λ = 0. Hence, if let ν1 = ν2 = ⋯ = νm = 0 in Theorem 3, we obtain the following conclusion.
Theorem 4. Let α be a complex number with 0 < Re(α) < n, 1/r = 1/q1 + 1/q2 + ⋯+1/qm + 1/q − Re(α)/n, where r > n/n − Re(α) and 1 < q, q1, ⋯, qm < ∞. λ ≥ 0, 0 < l ≤ s ≤ ∞, λ − n/q + Re(α) < σ1 < n(1 − 1/q) + λ, σ2 = σ1 − n(1/q1 + 1/q2+⋯+1/qm). If , then, there exists a constant C > 0 such that
On the other hand, it is eminent that and . Therefore, by letting λ = 0 in Theorem 1, 3, and 4, respectively, we will get counterparts on p-adic Herz spaces.
Corollary 5. Let α be a complex number with 0 < Re(α) < n, 1/r = 1/q − Re(α)/n with 1 ≤ q < r < ∞, Re(α) − n/q < σ < n(1 − 1/q), 0 < l ≤ s ≤ ∞. If q > 1, then, there exists a constant C > 0 such that
Moreover, if q = 1, then, there exists a constant C > 0 such that
Corollary 6. Let α be a complex number with 0 < Re(α) < n, 1/r = 1/q1 + 1/q2 + ⋯+1/qm + 1/q − Re(α)/n, where r > n/n − Re(α) and 1 < q, q1, ⋯, qm < ∞. 0 < l ≤ s ≤ ∞, ν = ν1 + ν2 + ⋯+νm with 0 ≤ ν1, ν2, ⋯, νm < 1/n, nν − n/q + Re(α) < σ1 < n(1 − 1/q), σ2 = σ1 − n(1/q1 + 1/q2+⋯+1/qm + ν). If , then, there exists a constant C > 0 such that
Corollary 7. Let α be a complex number with 0 < Re(α) < n, 1/r = 1/q1 + 1/q2 + ⋯+1/qm + 1/q − Re(α)/n, where r > n/n − Re(α) and 1 < q, q1, ⋯, qm < ∞. 0 < l ≤ s ≤ ∞, Re(α) − n/q < σ1 < n(1 − 1/q), σ2 = σ1 − n(1/q1 + 1/q2+⋯+1/qm). If , then, there exists a constant C > 0 such that
Throughout this paper, for t > 0 and α ∈ ℂ, we always assume that tα takes the principal branch, that is
Thus, we have
The letter C will be used to denote various constants, and the various uses of the letter do not, however, denote the same constant.
2. Some Notations and Lemmas
We start with some notations and definitions. Here and in what follows, denote by χk the characteristic function of the sphere Sk.
Definition 8 (see [15].)Let σ ∈ ℝ and 0 < s, r ≤ ∞. The homogeneous Herz space is defined by
for s < ∞, and the usual modifications should be made when s = ∞.
Definition 9 (see [15].)Let σ ∈ ℝ, 0 < s, r ≤ ∞, and λ be a nonnegative real number. Then, the homogeneous Morrey-Herz space is defined by
Here, we introduce the p-adic weak Herz spaces and p-adic weak Morrey-Herz spaces.
Definition 10. Let σ ∈ ℝ, 0 < s, r ≤ ∞. The weak homogeneous Herz space defined by
Definition 11. Let σ ∈ ℝ, 0 < s, r ≤ ∞, and λ be a nonnegative real number. The weak homogeneous Morrey-Herz space defined by
Definition 12 (see [9].)Given λ < 1/n, 1 < q < ∞, the λ -central bounded mean oscillation space is defined as the set of all functions such that
Lemma 13 (see [10].)Suppose that 0 ≤ λ < 1/n, 1 < q < ∞, and j, k ∈ ℤ. Then
Lemma 14 (see [8].)Let α be a complex number with 0 < Re(α) < n, 1/r = 1/q − Re(α)/n with 1 ≤ q < r < ∞.If q > 1, then, there exists a constant C > 0 such that
Moreover, if q = 1, there is a constant C > 0 such that
Lemma 15. Let α be a complex number with 0 < Re(α) < n, 1/r = 1/q − Re(α)/n with 1 ≤ q < r < ∞. Then. there exists a constant C > 0 such that and
Proof. Obviously, by the properties of |·|p, it is not difficult to check that
Therefore, Lemma 15 is completely proved.
3. Proof of Theorems
Proof of Theorem 16. Suppose that , we decompose f in the following way
First, we prove that for q > 1. By the decomposition of f above and the fact l ≤ s, we get
If k − 1 ≤ j ≤ k + 1, by the Lr-boundedness of (see Lemma 14), we can obtain the estimates of by
If j ≤ k − 2, applying Lemma 15, Jensen’s inequality, Hölder’s inequality, and the fact σ < n(1 − 1/q) = n/q′, we can get the estimates for by
If j ≥ k + 2, Lemma 15 shows the estimates for by
For , using similar methods as that for , by the fact σ > λ − n/q + Re(α) ≥ −n/q + Re(α), Jensen’s inequality, and Hölder’s inequality, we obtain
For , one can see from the definition of Morrey-Herz space that
Here, by the estimates (43) and the fact σ > λ − n/q + Re(α) ≥ −n/q + Re(α), we obtain
Therefore, by a combination for the estimates of , and , we can conclude that .
Next, for q = 1, we will consider the weak type boundedness of . Note that for l < s, so we only need to prove that in the case l = s. For any μ > 0, the decomposition of f shows that
For , applying the weak type property (1, r) of the operator (see Lemma 14) and the estimates (43). Notice that λ − n + Re(α) < σ < 0 when q = 1, λ ≥ 0, so we can conclude that
For , by the Chebychev inequality, Lemma 15, the estimates (43), and the fact λ − n + Re(α) < σ < 0, we have
Hence, by a combination for the estimates of , and , we can get the desired inequality .
Therefore, we complete the proof of Theorem 16.
Proof of Theorem 17. Similarly to the proof of Theorem 16, let and decompose f into
When m = 1, denote by , we consider
Let us first estimate , note that
Suppose that 1/u = 1/q − Re(α)/n, 1/t = 1/q1 + 1/q, then, it is easy to see 1/r = 1/u + 1/q1 = 1/t − Re(α)/n for q > 1 and t > 1. Applying the fact σ2 = σ1 − n(1/q1 + ν1), Hölder’s inequality, Minkowski inequality, the boundedness of from to and from to , we have
Therefore, we get
Now, let us turn to the estimates of and . If x ∈ Sk, we can easily deduce that
Then, using the facts 1/r = 1/q1 + 1/q − Re(α)/n, σ2 = σ1 − n(1/q1 + ν1), |j − k| ≥ 2, Lemma 13, and Hölder’s inequality, we can get
Thus, the fact nν1 + λ − n/q + Re(α) < σ1 < n(1 − 1/q) + λ and (43) imply
Combining the estimates for , and , which completes the proof for Theorem 3 of the case m = 1.
Now, we consider the case m ≥ 2. In order to simplify the proof, for positive integer m and 1 ≤ i ≤ m, we denote by the family of all finite subsets θ = {θ1, θ2, ⋯, θm} of {1, 2, ⋯, m} of i different elements, let θc = {1, 2, ⋯, m}\θ for any . For b = (b1, b2, ⋯, bm), let , and denote the integral average of the function bi over the set Bk, then
We write
Let us first estimate , we can obtain
For , taking 1/s = 1/q − Re(α)/n, then, 1/r = 1/q1 + 1/q2 + ⋯+1/qm + 1/s. Applying Hölder’s inequality, the boundedness of from to and the fact σ2 = σ1 − n(1/q1+⋯+1/qm + ν1+⋯+νm), we obtain
For , taking 1/h = 1/q1 + ⋯+1/qm + 1/q, then, 1/r = 1/h − Re(α)/n for h > 1. By Hölder’s inequality, the boundedness of from to and the fact σ2 = σ1 − n(1/q1+⋯+1/qm + ν1+⋯+νm), we get
For , we denote by
Then, similarly to the method estimating for , it is not difficult for us to get
Next, we will estimate and . Let
Therefore, by Minkowski’s inequality, Hölder’s inequality, and Lemma 13, it follows that
Thus, similarly to the method estimating for and , we get
So far, by a combination for the estimates of , , and , we will finish the proof for Theorem 3 of the case m ≥ 2. This completes the proof of Theorem 17.
Conflicts of Interest
The authors declare that they have no conflicts of interest.
Acknowledgments
This project is partially supported by the MOE (Ministry of Education in China) Liberal arts and Social Sciences Foundation (Grant no. 20YJC790111).
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Data Availability
No data were used to support this study.