Volume 2022, Issue 1 7227544
Research Article
Open Access

p-Adic Riesz Potential and Its Commutators on Morrey-Herz Spaces

Yanlong Shi

Corresponding Author

Yanlong Shi

Zhejiang Pharmaceutical University, Ningbo, Zhejiang 315100, China

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Yafeng Shi

Yafeng Shi

School of Science, Ningbo University of Technology, Ningbo, Zhejiang 315211, China nbut.cn

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Shenbao Chen

Shenbao Chen

Zhejiang Business Technology Institute, Ningbo, Zhejiang 315012, China zjbti.net.cn

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First published: 16 May 2022
Citations: 3
Academic Editor: Andrea Scapellato

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

For a prime number p, the field of p-adic numbers p is defined as the completion of the field of rational numbers with respect to the non-Archimedean p-adic normal |·|p, which is defined as follows: if x = 0, |0|p = 0; if x ≠ 0 is an arbitrary rational number with the unique representation x = pγm/n, where m, n are not divisible by p, γ = γ(x) ∈ , then, |x|p = pγ. This norm satisfies the following properties:
  • (i)

    |x|p ≥ 0, ∀xp, and |x|p = 0⇔x = 0

  • (ii)

    |xy|p = |x|p|y|p, ∀x, yp

  • (iii)

    |x + y|p ≤ max(|x|p, |y|p), ∀x, yp and when |x|p ≠ |y|p, we have |x + y|p = max(|x|p, |y|p)

The space consists of all points x = (x1, ⋯, xn), where xjp, j = 1, 2, ⋯, n, n ≥ 1. The p-adic norm of is defined by
(1)
Denote by
(2)
the ball of radius pγ with center at and by
(3)
the sphere of radius pγ with center at , where γ. For convenience, we denote Bγ = Bγ(0) and Sγ = Sγ(0), it is easy to see that the equalities x0 + Bγ = Bγ(x0), x0 + Sγ = Sγ(x0), and Bγ(a) = ⋃kγSk(a) hold for any .
Since the space is a locally compact commutative group under addition, there exists the Haar measure dx on the additive group of normalized by
(4)
where |E| denotes the Haar measure of a measurable set . Then, by a simple calculation, we can obtain that
(5)
for any . We should mention that the Haar measure takes value in , there also exist p-adic valued measures [1, 2]. For a complete introduction to the p-adic analysis, one can refer to [3] or [4] and references therein.

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 [618]. 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.

On the p-adic field, let Γn(α) = (1 − pαn)/1 − pα with α\{0}, then, the Riesz potential is defined by
(6)

When n = 1, Haran [6, 7] obtained the explicit formula of the Riesz potential on p. 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 n 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 n, 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, λn/q + Re(α) < σ < n(1 − 1/q), 0 < ls ≤ ∞. If q > 1, then, there exists a constant C > 0 such that

(7)

Moreover, if q = 1, then, there exists a constant C > 0 such that

(8)

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 n, which was proved by Lu and Xu [20].

Moreover, let b = (b1, b2, ⋯, bm), where for 1 ≤ im, m. Then, multilinear commutator generated by b and can be defined as follows:

(9)

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 < ls ≤ ∞, ν = ν1 + ν2 + ⋯+νm with 0 ≤ ν1, ν2, ⋯, νm < 1/n, nν + λn/q + Re(α) < σ1 < n(1 − 1/q) + λ, σ2 = σ1n(1/q1 + 1/q2+⋯+1/qm + ν). If , then, there exists a constant C > 0 such that

(10)

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 < ls ≤ ∞, λn/q + Re(α) < σ1 < n(1 − 1/q) + λ, σ2 = σ1n(1/q1 + 1/q2+⋯+1/qm). If , then, there exists a constant C > 0 such that

(11)

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 < ls ≤ ∞. If q > 1, then, there exists a constant C > 0 such that

(12)

Moreover, if q = 1, then, there exists a constant C > 0 such that

(13)

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 < ls ≤ ∞, ν = ν1 + ν2 + ⋯+νm with 0 ≤ ν1, ν2, ⋯, νm < 1/n, nνn/q + Re(α) < σ1 < n(1 − 1/q), σ2 = σ1n(1/q1 + 1/q2+⋯+1/qm + ν). If , then, there exists a constant C > 0 such that

(14)

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 < ls ≤ ∞, Re(α) − n/q < σ1 < n(1 − 1/q), σ2 = σ1n(1/q1 + 1/q2+⋯+1/qm). If , then, there exists a constant C > 0 such that

(15)

Throughout this paper, for t > 0 and α, we always assume that tα takes the principal branch, that is

(16)

Thus, we have

(17)

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 and 0 < s, r ≤ ∞. The homogeneous Herz space is defined by

(18)
where
(19)

for s < ∞, and the usual modifications should be made when s = ∞.

Definition 9 (see [15].)Let σ, 0 < s, r ≤ ∞, and λ be a nonnegative real number. Then, the homogeneous Morrey-Herz space is defined by

(20)
where
(21)
for s < ∞, and the usual modifications should be made when s = ∞.

Here, we introduce the p-adic weak Herz spaces and p-adic weak Morrey-Herz spaces.

Definition 10. Let σ, 0 < s, r ≤ ∞. The weak homogeneous Herz space defined by

(22)
where
(23)
for s < ∞, and the usual modifications should be made when s = ∞.

Definition 11. Let σ, 0 < s, r ≤ ∞, and λ be a nonnegative real number. The weak homogeneous Morrey-Herz space defined by

(24)
where
(25)
for s < ∞, and the usual modifications should be made when s = ∞.

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

(26)
where
(27)

Lemma 13 (see [10].)Suppose that 0 ≤ λ < 1/n, 1 < q < ∞, and j, k. Then

(28)

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

(29)

Moreover, if q = 1, there is a constant C > 0 such that

(30)

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

(31)
for any integers j and k.

Proof. Obviously, by the properties of |·|p, it is not difficult to check that

(32)
for any xSk, ySj. Thus, by applying the Hölder’s inequality, we have
(33)
(34)
(35)

Therefore, Lemma 15 is completely proved.

3. Proof of Theorems

Proof of Theorem 16. Suppose that , we decompose f in the following way

(36)

First, we prove that for q > 1. By the decomposition of f above and the fact ls, we get

(37)

If k − 1 ≤ jk + 1, by the Lr-boundedness of (see Lemma 14), we can obtain the estimates of by

(38)

If jk − 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

(39)

If jk + 2, Lemma 15 shows the estimates for by

(40)

For , using similar methods as that for , by the fact σ > λn/q + Re(α) ≥ −n/q + Re(α), Jensen’s inequality, and Hölder’s inequality, we obtain

(41)
(42)

For , one can see from the definition of Morrey-Herz space that

(43)

Here, by the estimates (43) and the fact σ > λn/q + Re(α) ≥ −n/q + Re(α), we obtain

(44)

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

(45)

For , applying the weak type property (1, r) of the operator (see Lemma 14) and the estimates (43). Notice that λn + Re(α) < σ < 0 when q = 1, λ ≥ 0, so we can conclude that

(46)

For , by the Chebychev inequality, Lemma 15, the estimates (43), and the fact λn + Re(α) < σ < 0, we have

(47)

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

(48)

When m = 1, denote by , we consider

(49)

Let us first estimate , note that

(50)

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 = σ1n(1/q1 + ν1), Hölder’s inequality, Minkowski inequality, the boundedness of from to and from to , we have

(51)

Therefore, we get

(52)

Now, let us turn to the estimates of and . If xSk, we can easily deduce that

(53)

Then, using the facts 1/r = 1/q1 + 1/q − Re(α)/n, σ2 = σ1n(1/q1 + ν1), |jk| ≥ 2, Lemma 13, and Hölder’s inequality, we can get

(54)

Thus, the fact nν1 + λn/q + Re(α) < σ1 < n(1 − 1/q) + λ and (43) imply

(55)
(56)

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 ≤ im, 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

(57)
(58)
(59)
where and .

We write

(60)

Let us first estimate , we can obtain

(61)

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 = σ1n(1/q1+⋯+1/qm + ν1+⋯+νm), we obtain

(62)

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 = σ1n(1/q1+⋯+1/qm + ν1+⋯+νm), we get

(63)

For , we denote by

(64)
and 1/ω = 1/z + 1/q − Re(α)/n, then 1/r = 1/h + 1/ω. Using Hölder’s inequality and the Lω-boundedness of , we have
(65)

Then, similarly to the method estimating for , it is not difficult for us to get

(66)

Next, we will estimate and . Let

(67)

Therefore, by Minkowski’s inequality, Hölder’s inequality, and Lemma 13, it follows that

(68)

Thus, similarly to the method estimating for and , we get

(69)
(70)

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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