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Weighted multilinear p-adic Hardy operators and commutators

  • Ronghui Liu and Jiang Zhou EMAIL logo
Published/Copyright: December 29, 2017

Abstract

In this paper, the weighted multilinear p-adic Hardy operators are introduced, and their sharp bounds are obtained on the product of p-adic Lebesgue spaces, and the product of p-adic central Morrey spaces, the product of p-adic Morrey spaces, respectively. Moreover, we establish the boundedness of commutators of the weighted multilinear p-adic Hardy operators on the product of p-adic central Morrey spaces. However, it’s worth mentioning that these results are different from that on Euclidean spaces due to the special structure of the p-adic fields.

MSC 2010: 42B25; 42B35; 46B25

1 Introduction

In recent years, p-adic analysis has gathered a lot of attention by its applications in many aspects of mathematical physics, such as quantum mechanics, the probability theory and the dynamical systems [1,2]. On the other hand, it plays a crucial role in pseudo-differential equations, wavelet theory and harmonic analysis, etc. (see [3, 4, 5, 6, 7, 10]).

For a prime number p, let ℚp be the field of p-adic numbers. It is defined as the completion of the field of rational numbers ℚp with respect to the non-Archimedean p-adic norm |⋅|p. This norm is defined as follows: |0|p = 0; if any non-zero rational number x is represented as x=pγmn, where γ is an integer and the integers m, n are indivisible by p, then |x|p = pγ. It’s not hard to see that the norm satisfies the following properties:

|xy|p=|x|p|y|p,|x+y|pmax{|x|p,|y|p}.

Moreover, if |x|p ≠ |y|p, then |x+y|p = max{|x|p,|y|p}. It is well known that ℚp is a typical model of non-Archimedean local fields. From the standard p-adic analysis, we know that any non-zero element x of ℚp can be uniquely represented as a canonical form x = pγ(x0+ x1p+x2p+⋅s), where xi∈{0,1,…,p−1} and x0 ≠ 0, we then have |x|p = pγ. Let ℤp = {x ∈ ℚp:|x|p ≤ 1} be the class of all p-adic integrals in ℚp and denote Zp = ℤp∖{0}.

The space Qpn consists of elements x = (x1,x2,…,xn), where xi ∈ ℚp, i = 1,2,…,n. The p-adic norm on Qpn is

|x|p:=max1in{|xi|p},xQpn.

Denote by Bγ(a) = {x Qpn :|xa|ppγ}, the ball with center at a Qpn and radius pγ, and by Sγ(a) = {x Qpn :|xa|p = pγ} the sphere with center at a Qpn and radius pγ, γ ∈ ℤ. It is clear that Sγ(a) = Bγ(a)∖ Bγ−1(a), and we set Bγ(0) = Bγ and Sγ(0) = Sγ.

Since Qpn is a locally compact commutative group with respect to addition, it follows from the standard analysis that there exists a Haar measure dx on Qpn , which is unique up to a positive constant factor and is translation invariant, i.e., d(x+a) = dx. We normalize the measure dx such that

B0(0)dx=|B0(0)|H=1,

where |B|H denotes the Haar measure of a measure subset B of Qpn . By simple calculation, we can obtain that

|Bγ(a)|H=pγn,|Sγ(a)|H=pγn(1pn).

The classical Hardy operator 𝓗 is defined by

Hf(x):=1x0xf(t)dt,x>0,

where the function f is a nonnegative integrable function on ℝ+. A celebrated integral inequality, due to Hardy [8], states that

HfLq(R+)qq1fLq(R+),

holds for 1 < q < ∞, and the constant factor qq1 is the best value and it is the norm of the operator 𝓗, that is,

HLq(R+)Lq(R+)=qq1.

N-dimensional Hardy operator was introduced by Christ and Grafakos in [9] as follows:

Hf(x):=1Ωn|x|n|t||x|f(t)dt,xRn{0},

where Ωn is the volume of the unit ball in ℝn. The norm of 𝓗 on Lq(ℝn) was evaluated and found to be equal to that of the classical Hardy operator.

In 2012, Fu et al. [10] defined the n-dimensional p-adic Hardy operator as follows:

Hpf(x):=1|B(0,|x|p)|H|t|p|x|pf(t)dt,xQpn{0},

where f is a nonnegative measurable function on Qpn , B(0,|x|p) is a ball in Qpn with center at 0 ∈ Qpn and radius |x|p, and they proved the sharp estimate of the p-adic Hardy operator on Lebesgue spaces with power weights.

In 1984, Carton-Lebrun and Fosset [11] defined the weighted Hardy average operator 𝓗φ by

Hφ(f)(x):=01f(tx)φ(t)dt,xRn,

where φ:[0,1]→[0, ∞) is a function, and showed the boundedness of 𝓗φ on Lebesgue and BMO(ℝn) spaces. Evidently the operator 𝓗φ deeply depends on the nonnegative function φ. For example, when n = 1 and φ(x) = 1 for x ∈ [0,1], the operator 𝓗φ is just reduced to the classical Hardy operator.

In 2006, Rim and Lee [13] defined the weighted p-adic Hardy operator Hφp by

Hφp(f)(x):=Zpf(tx)φ(t)dt,xQpn,

where φ is a nonnegative function defined on Zp , and gave the characterization of function φ for which Hφp is bounded on Lq( Qpn ), 1 ≤ q ≤ ∞, they also obtained the corresponding operator norm.

Morrey [12] introduced the Lq,λ(ℝn) spaces to study the local behavior of solutions to second order elliptic partial differential equations. The p-adic Morrey space is defined as follows.

Definition 1.1

([13]). Let 1 ≤ q < ∞ and λ ≥ −1/q. The p-adic Morrey space 𝓛q,λ( Qpn ) is defined by

Lq,λ(Qpn)={fLlocq(Qpn):fLq,λ(Qpn)<},

where

fLq,λ(Qpn):=supaQpn,γZ(1|Bγ(a)|1+λqBγ(a)|f(x)|q)1/q<.

Remark 1.2

It is clear that Lq,1/q(Qpn)=Lq(Qpn),Lq,0(Qpn)=L(Qpn).

In 2017, Wu and Fu [14] proved sufficient and necessary conditions of weighted functions, for which the weighted p-adic Hardy operators are bounded on p-adic central Morrey spaces.

The p-adic central Morrey space is defined as follows.

Definition 1.3

Let λ ∈ ℝ and 1 < q < ∞ . The p-adic central Morrey space Bq,λ( Qpn ) is defined by

fBq,λ(Qpn):=supγZ(1|Bγ|1+λqBγ|f(x)|q)1/q<,

where Bγ = Bγ(0). It is clear that Bq,1q(Qpn)=Lq(Qpn), when λ < −1/q, the space Bq,λ( Qpn ) reduces to {0}, therefore, we can only consider the case λ ≥ −1/q. If 1 ≤ q1q2 < ∞, by Hölder’s inequality

Bq2,λ(Qpn)Bq1,λ1(Qpn)

λ ∈ ℝ.

Definition 1.4

([10]). Let 1 ≤ q < ∞. A function fLlocq(Qpn) is said to be CMOq( Qpn ), if

fCMOq(Qpn):=supγZ(1|Bγ(0)|HBγ(0)|f(x)fBγ(0)|qdx)1/q,

where

fBγ(0)=1|Bγ(0)|HBγ(0)f(x)dx.

The study of multilinear averaging operators is traced to the multilinear singular integral operator theory [15], and motivated not only the generalization of the theory of linear ones but also their natural appearance in analysis. For a more complete account on multilinear opeartors, we refer to [16, 17, 18, 19] and the references therein.

In this paper, we consider the multilinear version of weighted p-adic Hardy operators in the p-adic fields. Firstly, we introduce the weighted multilinear p-adic Hardy operators as follows.

Definition 1.5

Let m ∈ ℕ, x Qpn , and φ be a nonnegative integrable function on Zp×Zp××Zp. The weighted multilinear p-adic Hardy operator Hφ,mp is defined as

Hφ,mp(f)(x)=(Zp)mi=1mfi(tix)φ(t)dt,

where f⃗: = (f1,…,fm), t⃗: = (t1,…,tm), dt⃗: = dt1dtm, and fi (i = 1,…,m) are measurable functions on Qpn . When m = 1, Hφ,mp is reduced to the weighted p-adic Hardy operators Hφp .

The outline of the paper is as follows. In Section 2, we furnish sharp estimate of weighted multilinear p-adic Hardy operator on the product of p-adic Lebesgue spaces, and then the result is extended to the product of p-adic central Morrey spaces, the product of p-adic Morrey spaces, respectively. In Section 3, we present the boundedness of commutators of the weighted multilinear p-adic Hardy operators.

2 Sharp estimates of weighted multilinear p-adic Hardy operator

We begin with the following sharp boundedness of Hφ,mp on the product of p-adic Lebesgue spaces.

Theorem 2.1

Let 1 < q,qi < ∞, i = 1,…,m and 1q=1q1++1qm. Then Hφ,mp is bounded from Lq1(Qpn)×Lq2(Qpn)××Lqm(Qpn)toLq(Qpn) if and only if

Am:=(Zp)mi=1m|ti|pn/qiφ(t)dt<. (1)

Moreover,

Hφ,mpLq1(Qpn)×Lq2(Qpn)××Lqm(Qpn)Lq(Qpn)=Am.

Proof

Without loss of generality, we consider only the situation when m = 2. Actually, a similar procedure works for all m ∈ ℕ.

Suppose that (1) holds. Using Minkowski’s inequality yields

Hφ,2p(f1,f2)Lq(Qpn)=(Qpn|(Zp)2f1(t1x)f2(t2x)φ(t1,t2)dt1dt2|qdx)1/q(Zp)2(Qpn|f1(t1x)f2(t2x)|qdx)1/qφ(t1,t2)dt1dt2.

By Hölder’s inequality with 1q=1q1+1q2, we see that

Hφ,2p(f1,f2)Lq(Qpn)(Zp)2i=12(Qpn|fi(tix)|qidx)1/qiφ(t1,t2)dt1dt2(i=12fiLqi(Qpn))(Zp)2(i=12|ti|pn/qi)φ(t1,t2)dt1dt2.

Thus, Hφ,2p maps the product of p-adic Lebesgue spaces Lq1(Qpn)×Lq2(Qpn) to Lq(Qpn) and

Hφ,2pLq1(Qpn)×Lq2(Qpn)×Lq(Qpn)A2. (2)

To see the necessity, for any 0 < ε < 1 and |ε|p > 1, we take

fiε(x)=0,|xi|p<1,|xi|pnqiq2εqi,|xi|p1. (3)

An elementary calculation gives that

f1εLq1(Qpn)q1=f2εLq2(Qpn)q2=1pn1pεq2.

Consequently, we have

Hφ,2p(f1ε,f2ε)Lq(Qpn)={Qpn|x|pnq2ε(1|x|p|t1|p<11|x|p|t2|p<1|t1|pnq1q2εq1|t2|pnq1εφ(t1,t2)dt1dt2)qdx}1/q{|x|p1|x|pnq2ε(1|x|p|t1|p<11|x|p|t2|p<1|t1|pnq1q2εq1|t2|pnq1εφ(t1,t2)dt1dt2)qdx}1/q{|x|p|ε|p|x|pnq2ε(1|ε|p|t1|p<11|ε|p|t2|p<1|t1|pnq1q2εq1|t2|pnq1εφ(t1,t2)dt1dt2)qdx}1/q=(1|ε|p|t1|p<11|ε|p|t2|p<1|t1|pnq1q2εq1|t2|pnq1εφ(t1,t2)dt1dt2)(|x|p|ε|p|x|pnq2εdx)1/q=(1|ε|p|t1|p<11|ε|p|t2|p<1|t1|pnq1q2εq1|t2|pnq1εφ(t1,t2)dt1dt2)|ε|pεq2i=12fiεLqi(Qpn).

Therefore,

1|ε|p|t1|p11|ε|p|t2|p1|t1|pnq1q2εq1|t2|pnq1εφ(t1,t2)dt1dt2C|ε|pεq2.

Now take ε = pk, k = 1,2,⋯. Then |ε|p = pk > 1. Letting k approach to ∞, then ε approaches to 0 and |ε|pεq2=pkq2pk approaches to 1. Then by Fatou’s Lemma, we obtain

ZpZp|t1|pn1/q1|t2|pn2/q2φ(t1,t2)dt1dt2<.

and

Hφ,2pLq1(Qpn)×Lq2(Qpn)×Lq(Qpn)A2. (4)

Combining (2) and (4) then finishes the proof. □

Next, we extend the result in Theorem 2.1 to the product of p-adic central Morrey spaces.

Theorem 2.2

Let 1 < q < qi < ∞, 1q=1q1++1qm, λ = λ1+⋯+λm and −1/qiλi < 0, i = 1,…,m.

  1. If

    A~m:=(Zp)mi=1m|ti|pnλiφ(t)dt<. (5)

    Then, Hφ,mp is bounded from Bq1,λ1(Qpn)×Bq2,λ2(Qpn)××Bqm,λm(Qpn)toBq,λ(Qpn) with its operator norm not more that 𝓐͠m.

  2. Assume that λ1q1 = ⋯ = λmqm. In the case the condition (5) is also necessary for the boundedness of Hφ,mp:Bq1,λ1(Qpn)×Bq2,λ2(Qpn)××Bqm,λm(Qpn)Bq,λ(Qpn). Moreover,

    Hφ,mpBq1,λ1(Qpn)×Bq2,λ2(Qpn)××Bqm,λm(Qpn)Bq,λ(Qpn)=A~m.

Proof

By similarity, we only give the proof in the case m = 2.

When −1/qi = λi, i = 1,2, then Theorem 2.2 is just Theorem 2.1.

Next we consider the case that −1/qi < λi < 0, i = 1,2. Let γ ∈ ℤ, tiBγ = B(0,|ti|ppγ) and 𝓐͠2 < ∞. Since 1/q = 1/q1+1/q2, by Minkowski’s inequality and Hölder’s inequality, we see that, for all balls B = B(0,pγ),

(1|Bγ|H1+λqBγ|Hφ,2p(f)(x)|qdx)1/q(Zp)2(1|Bγ|H1+λqBγ|i=12fi(tix)|qdx)1/qφ(t)dt(Zp)2i=12(1|Bγ|H1+λiqiBγ|fi(tix)|qidx)1/qiφ(t)dt=(Zp)2|t1|pnλ1|t2|pnλ2i=12(1|tiBγ|H1+λiqitiBγ|fi(x)|qidx)1/qiφ(t)dtf1Bq1,λ1(Qpn)f2Bq2,λ2(Qpn)(Zp)2|t1|pnλ1|t2|pnλ2φ(t)dt.

This means that

Hφ,2pBq1,λ1(Qpn)×Bq2,λ2(Qpn)Bq,λ(Qpn)A~2. (6)

For the necessity when λ1q1 = λ2q2, let f1(x)=|x|pnλ1 and f2(x)=|x|pnλ2 for all x Qpn ∖{0}, and f1(0) = f2(0): = 0. Then for any B = B(0,pγ), we have

(1|Bγ|H1+λiqiBγ|fi(x)|qidx)1/qi=(pnγ(1+λiqi)k=γSkpnkλiqidx)1/qi=((1pn)pnγ(1+λiqi)k=γpnk(1+λiqi))1/qi=(1pn1pn(1+λiqi))1/qi,

where the series converge due to λi > −1/qi. Then fiBqi,λi( Qpn ). Since λ = λ1+λ2 and −1/qiλi < 0, 1 < q < qi < ∞, i = 1,2, we have

(1|Bγ|H1+λqBγ|Hφ,2p(f)(x)|qdx)1/q=(1|Bγ|H1+λqBγ|x|pnλqdx)1/q(Zp)2|t1|pnλ1|t2|pnλ2φ(t)dt=(1pn1pn(1+λq))1/q(Zp)2|t1|pnλ1|t2|pnλ2φ(t)dt=f1Bq1,λ1(Qpn)f2Bq2,λ2(Qpn)(1pn(1+λ1q1))1/q1(1pn(1+λ2q2))1/q2(1pn(1+λq))1/q×(Zp)2|t1|pnλ1|t2|pnλ2φ(t)dt=f1Bq1,λ1(Qpn)f2Bq2,λ2(Qpn)(Zp)2|t1|pnλ1|t2|pnλ2φ(t)dt,

since λ1q1 = λ2q2. Then,

A~2Hφ,2pBq1,λ1(Qpn)×Bq2,λ2(Qpn)Bq,λ(Qpn)<. (7)

Combining (6) and (7) then concludes the proof. This finishes the proof of the Theorem 2.2.

We remark that Theorem 2.2 when m = 1 goes back to [14] Theorem 2.3. □

Next, we give sharp estimate of weighted multilinear p-adic Hardy operator on the product of p-adic Morrey spaces.

Theorem 2.3

Let 1 < q < qi < ∞, 1q=1q1++1qm, λ = λ1 + ⋯ + λm and −1/qi < λi < 0, i = 1, …, m.

  1. If

    Bm:=(Zp)mi=1m|ti|pnλiφ(t)dt<. (8)

    Then, Hφ,mp is bounded from Lq1,λ1(Qpn)×Lq2,λ2(Qpn)××Lqm,λm(Qpn)toLq,λ(Qpn) with its operator norm not more that 𝓑m.

  2. Assume that λ1q1 = ⋯ = λmqm. In the case the condition (8) is also necessary for the boundedness of Hφ,mp:Lq1,λ1(Qpn)×Lq2,λ2(Qpn)××Lqm,λm(Qpn)Lq,λ(Qpn). Moreover,

    Hφ,mpLq1,λ1(Qpn)×Lq2,λ2(Qpn)××Lqm,λm(Qpn)Lq,λ(Qpn)=Bm.

Proof

By similarity, we only give the proof in the case m = 2. Suppose 𝓑2 < ∞. Since 1/q = 1/q1 + 1/q2, by Minkowski’s inequality and Hölder’s inequality, we see that

(1|Bγ(a)|H1+λqBγ(a)|Hφ,2p(f)(x)|qdx)1/q(Zp)2(1|Bγ(a)|H1+λqBγ(a)|i=12fi(tix)|qdx)1/qφ(t)dt(Zp)2i=12(1|Bγ(a)|H1+λiqiBγ(a)|fi(tix)|qidx)1/qiφ(t)dt=(Zp)2|t1|pnλ1|t2|pnλ2i=12(1|tiBγ(a)|H1+λiqitiBγ(a)|fi(x)|qidx)1/qiφ(t)dtf1Lq1,λ1(Qpn)f2Lq2,λ2(Qpn)(Zp)2|t1|pnλ1|t2|pnλ2φ(t)dt.

This means that

Hφ,2pLq1,λ1(Qpn)×Lq2,λ2(Qpn)Bq,λ(Qpn)B2. (9)

For the necessity when λ1q1 = λ2q2, let f1(x)=|x|pnλ1 and f2(x)=|x|pnλ2 for all x Qpn \ {0}, and f1(0) = f2(0): = 0. Then for any B = B(a,pγ), we need to show that fi ∈ 𝓛qi,λi( Qpn ). Considering the following two cases.

  1. If |a|p > pγ and xBγ(a), then |x|p = max{|xa|p, |a|p} > pγ. Since −1/qiλi < 0, we have

    1|Bγ(a)|H1+λiqiBγ(a)|x|pnλiqidx<1|Bγ(a)|H1+λiqiBγ(a)pγnλiqidx=1.
  2. If |a|ppγ and xBγ(a), then |x|p = max{|xa|p, |a|p} ≤ pγ. Therefore, xBγ(a). Recall that two balls in Qpn are either disjoint or one is contained in the other [20]. So we have Bγ(a) = Bγ, thus

    1|Bγ(a)|H1+λiqiBγ(a)|x|pnλiqidx=1|Bγ|H1+λiqiBγ|x|pnλiqidx=1pn1pn(1+λiqi).

    From the previous discussion, we can see that fi ∈ 𝓛qi,λi( Qpn ). By the similar estimates to the method of Theorem 2.2, we have

    B2Hφ,2pLq1,λ1(Qpn)×Lq2,λ2(Qpn)Lq,λ(Qpn)<. (10)

Combining (9) and (10) then yields the desired result.□

We remark that Theorem 2.3 when m = 1 goes back to [14] Theorem 2.1.

3 Boundedness of commutators of the weighted multilinear p-adic Hardy operators

Now we introduce the definition for the multilinear version of the commutator of the weighted p-adic Hardy operators. Let m ≥ 2, and φ be a nonnegative integrable function on Zp×Zp××Zp, and bi (i = 1, …, m) be locally integral functions on Qpn . We define

Hφ,mp,b:=(Zp)m(i=1mfi(tix))(i=1m(bi(x)bi(tix)))φ(t)dt,xQpn.

Then we have the following multilinear result.

Theorem 3.1

Let 1 < q < qi < ∞, 1 < ρ < ∞, −1/qi < λi < 0, i = 1, …, m, such that 1q=1q1++1qm+1ρ1++1ρm, λ = λ1 + ⋯ + λm. If

B~m:=(Zp)mi=1m|ti|pnλiφ(t)(i=1mlogp1|ti|p)dt<.

Then Hφ,mp,b is bounded from Bq1,λ1(Qpn)×Bq2,λ2(Qpn)××Bqm,λm(Qpn)toBq,λ(Qpn) for all b⃗ = (b1, b2, …, bm) ∈ CMOρ1(Qpn)×CMOρ2(Qpn)××CMOρm(Qpn).

Proof

By similarity, we only consider the case that m = 2, that is, we assume 𝓑͠2 < ∞ and just need to show that

Hφ,2p,b(f)Bq,λ(Qpn)CB~2f1Bq1,λ1(Qpn)f2Bq2,λ2(Qpn),

where b⃗ = (b1, b2) ∈ CMOρ1(Qpn)×CMOρ2(Qpn). By Minkowski’s inequality we have

(1|Bγ|HBγ|Hφ,2p,b(f)(x)|qdx)1/q(1|Bγ|HBγ(ZpZpi=12|fi(tix)|i=12|bi(x)bi(tix)|φ(t1,t2)dt1dt2)qdx)1/qZpZp(1|Bγ|HBγ(i=12|fi(tix)|i=12|bi(x)bi(tix)|)qdx)1/qφ(t1,t2)dt1dt2:=I1+I2+I3+I4+I5+I6,

where

I1=ZpZp(1|Bγ|HBγ(i=12|fi(tix)|i=12|bi(x)bi,Bγ|)qdx)1/qφ(t1,t2)dt1dt2,I2=ZpZp(1|Bγ|HBγ(i=12|fi(tix)|i=12|bi(tix)bi,tiBγ|)qdx)1/qφ(t1,t2)dt1dt2,I3=ZpZp(1|Bγ|HBγ(i=12|fi(tix)|i=12|bi,Bγbi,tiBγ|)qdx)1/qφ(t1,t2)dt1dt2,I4=ZpZp(1|Bγ|HBγ(i=12|fi(tix)|D(i,j)|bi(x)bi,Bγ||bj,Bγbj,tjBγ|)qdx)1/qφ(t1,t2)dt1dt2,I5=ZpZp(1|Bγ|HBγ(i=12|fi(tix)|D(i,j)|bi(x)bi,Bγ||bj(tjx)bj,tjBγ|)qdx)1/qφ(t1,t2)dt1dt2,I6=ZpZp(1|Bγ|HBγ(i=12|fi(tix)|D(i,j)|bi,Bγbi,tiBγ||bj(tjx)bj,tjBγ|)qdx)1/qφ(t1,t2)dt1dt2,

and

D(i,j):={(i,j):(1,2),(2,1)},bi,Bγ=1|Bγ|HBγbi,i=1,2.

Choose q < s1 < ∞, q < s2 < ∞ such that 1/s1 = 1/q1 + 1/ρ1, 1/s2 = 1/q2 + 1/ρ2. Then by Hölder’s inequality, we know that

I1ZpZpi=12(1|Bγ|HBγ|fi(tix)|qidx)1/qii=12(1|Bγ|HBγ|bi(x)bi,Bγ|ρidx)1/ρiφ(t1,t2)dt1dt2|Bγ|HλZpZpi=12|ti|pnλii=12(1|tiBγ|H1+λiqitiBγ|fi(x)|qidx)1/qi×i=12(1|Bγ|HBγ|bi(x)bi,Bγ|ρidx)1/ρiφ(t1,t2)dt1dt2|Bγ|Hλb1CMOρ1(Qpn)b1CMOρ1(Qpn)f1Bq1,λ1(Qpn)f2Bq2,λ2(Qpn)×ZpZpi=12|ti|pnλiφ(t1,t2)dt1dt2.

Similarly, we obtain

I2ZpZpi=12(1|Bγ|HBγ|fi(tix)|qidx)1/qii=12(1|Bγ|HBγ|bi(tix)bi,tiBγ|ρidx)1/ρiφ(t1,t2)dt1dt2|Bγ|HλZpZpi=12|ti|pnλii=12(1|tiBγ|H1+λiqitiBγ|fi(x)|qidx)1/qi×i=12(1|tiBγ|HtiBγ|bi(x)bi,tiBγ|ρidx)1/ρiφ(t1,t2)dt1dt2|Bγ|Hλb1CMOρ1(Qpn)b1CMOρ1(Qpn)f1Bq1,λ1(Qpn)f2Bq2,λ2(Qpn)×ZpZpi=12|ti|pnλiφ(t1,t2)dt1dt2.

It follows from 1/q = 1/s1 + 1/s2 that 1 = q/s1 + q/s2. From 1/s1 = 1/q1 + 1/ρ1, 1/s2 = 1/q2 + 1/ρ2 and Hölder’s inequality, we deduce that

I3=ZpZp(1|Bγ|HBγ(i=12|fi(tix)|i=12|bi,Bγbi,tiBγ|)qdx)1/qφ(t1,t2)dt1dt2ZpZpi=12(1|Bγ|HBγ|fi(tix)|sidx)1/si(i=12|bi,Bγbi,tiBγ|)φ(t1,t2)dt1dt2|Bγ|HλZpZpi=12|ti|pnλii=12(1|tiBγ|H1+λiqitiBγ|fi(x)|qidx)1/qi×(i=12|bi,Bγbi,tiBγ|)φ(t1,t2)dt1dt2|Bγ|Hλf1Bq1,λ1(Qpn)f2Bq2,λ2(Qpn)l=0k=0{pl1<|t1|ppl}{pk1<|t2|ppk}|t1|pnλ1|t2|pnλ2×(j=0l|b1,pjBγb1,pj1Bγ|+|b1,pl1Bγb1,tiBγ|)×(j=0k|b2,pjBγb2,pj1Bγ|+|b2,pk1Bγb2,tiBγ|)φ(t1,t2)dt1dt2C|Bγ|Hλb1CMOρ1(Qpn)b1CMOρ1(Qpn)f1Bq1,λ1(Qpn)f2Bq2,λ2(Qpn)×ZpZpi=12|ti|pnλilogpp|t1|plogpp|t2|pφ(t1,t2)dt1dt2,

where we use the fact that

|b1,Bγb1,t1Bγ|=j=0l|b1,pjBγb1,pj1Bγ|+|b1,pl1Bγb1,t1Bγ|C(l+1)b1CMOρ1(Qpn)Clogpp|t1|pb1CMOρ1(Qpn),

and

|b2,Bγb2,t2Bγ|Clogpp|t2|pb2CMOρ2(Qpn).

We now estimate I4. Similarly, we choose 1 < s < ∞ such that 1/q = 1/q1 + 1/q2 + 1/s and 1/s = 1/q1 + 1/q2. Using Minkowski’s inequality and Hölder’s inequality yields

I4=ZpZp(1|Bγ|HBγ(i=12|fi(tix)|D(i,j)|bi(x)bi,Bγ||bj,Bγbj,tjBγ|)qdx)1/qφ(t1,t2)dt1dt2ZpZp[(1|Bγ|HBγ((i=12|fi(tix)|)(|b1(x)b1,Bγ||b2,Bγb2,t2Bγ|))qdx)1/q+(1|Bγ|HBγ((i=12|fi(tix)|)(|b2(x)b2,Bγ||b1,Bγb1,t1Bγ|))qdx)1/q]φ(t1,t2)dt1dt2ZpZpi=12(1|Bγ|HBγ|fi(tix)|qidx)1/qi{(1|Bγ|HBγ|b1(x)b1,Bγ|sdx)1/s×|b2,Bγb2,t2Bγ|+(Bγ|b2(x)b2,Bγ|sdx)1/s|b1,Bγb1,t1Bγ|}φ(t1,t2)dt1dt2|Bγ|HλZpZpi=12|ti|pnλii=12(1|tiBγ|H1+λiqitiBγ|fi(x)|qidx)1/qi×{(1|Bγ|HBγ|b1(x)b1,Bγ|sdx)1/s|b2,Bγb2,t2Bγ|+(Bγ|b2(x)b2,Bγ|sdx)1/s|b1,Bγb1,t1Bγ|}φ(t1,t2)dt1dt2|Bγ|Hλf1Bq1,λ1(Qpn)f2Bq2,λ2(Qpn)ZpZpi=12|ti|pnλi×{(1|Bγ|HBγ|b1(x)b1,Bγ|sdx)1/s|b2,Bγb2,t2Bγ|+(Bγ|b2(x)b2,Bγ|sdx)1/s|b1,Bγb1,t1Bγ|}φ(t1,t2)dt1dt2C|Bγ|Hλb1CMOρ1(Qpn)b1CMOρ1(Qpn)f1Bq1,λ1(Qpn)f2Bq2,λ2(Qpn)×ZpZpi=12|ti|pnλiφ(t1,t2)(i=12logpp|ti|p)dt1dt2.

It is apparent from the estimates of I1, I2, I3 and I4 that

I5|Bγ|Hλb1CMOρ1(Qpn)b1CMOρ1(Qpn)f1Bq1,λ1(Qpn)f2Bq2,λ2(Qpn)×ZpZpi=12|ti|pnλiφ(t1,t2)dt1dt2,

and

I6|Bγ|Hλb1CMOρ1(Qpn)b1CMOρ1(Qpn)f1Bq1,λ1(Qpn)f2Bq2,λ2(Qpn)×ZpZpi=12|ti|pnλiφ(t1,t2)(i=12logpp|ti|p)dt1dt2.

Combining the estimates of I1, I2, I3, I4, I5 and I6 gives

(1|Bγ|H1+λqBγ|Hφ,2p,b(f)(x)|qdx)1/qCb1CMOρ1(Qpn)b1CMOρ1(Qpn)f1Bq1,λ1(Qpn)f2Bq2,λ2(Qpn)×ZpZpi=12|ti|pnλiφ(t1,t2)(i=12logp1|ti|p)dt1dt2.

This finishes the proof of Theorem 3.1.□

Acknowledgement

The authors would like to thank the anonymous reviewer for his/her comments which help to develop the manuscript. The research was supported by the National Natural Science Foundation of China (Grant No. 11661075).

References

[1] Vladimirov V.S., Volovich I.V., Zelenov E.I., p-adic Analysis and Mathematical Physics, World Scientific, Singapore, 199410.1142/1581Search in Google Scholar

[2] Vladimirov V.S., Volovich I.V., p-adic quantum mechanics, Comm. Math. Phys., 1989, 123, 659-67610.1007/BF01218590Search in Google Scholar

[3] Chuong N.M., Ciarlet P.G., Lax P., Mumford D. and Phong D.H., Advances in deterministic and stochastic snalysis, World Scientific, Singapore, 200710.1142/6374Search in Google Scholar

[4] Chuong N.M., Egorov Yu.V., Khrennikov A., Meyer Y. and Mumford D., Harmonic, wavelet and p-adic analysis, World Scientific, Singapor, 200710.1142/6373Search in Google Scholar

[5] Taibleson, M., Fourier analysis on local fields, Princeton Univ. Press, Princeton, 1975Search in Google Scholar

[6] Rim Y.C., Carleson measures and the BMO space on the p-adic vector space, Math. Z., 2009, 282, 1470-147710.1002/mana.200610806Search in Google Scholar

[7] Wu Q.Y., Fu Z.W., Sharp estimates of m-linear p-adic Hardy and Hardy-Littlewood-Pólya operators, J. Appl. Math., 2011, 2011,137-15010.1155/2011/472176Search in Google Scholar

[8] Hardy G.H., Note on a theorem of Hilbert, Math. Z., 1920, 6, 314-31710.1007/BF01199965Search in Google Scholar

[9] Christ M., Grafakos, L., Best constants for two nonconvolution inequalities, Proc. Am. Math. Soc., 1995, 123, 1687-169310.1090/S0002-9939-1995-1239796-6Search in Google Scholar

[10] Fu Z.W., Wu Q.Y., Lu S.Z., et al., Sharp estimates of p-adic Hardy and Hardy-Littlewood-Pólya operators, Acta Math. Sin. (Engl. Ser.), 2012 29, 137-15010.1007/s10114-012-0695-xSearch in Google Scholar

[11] Carton-Lebrun C., Fosset M., Moyennes et quotients de Taylor dans BMO, Bull. Soc. Roy. Sci. Liege., 1984, 53(2), 85-87Search in Google Scholar

[12] Morrey C.B., On the solutions of quasi-linear elliptic partial differential equations, Trans. Amer. Math. Soc., 1938, 43, 126-16610.1090/S0002-9947-1938-1501936-8Search in Google Scholar

[13] Rim K.S., Lee J., Estimates of weighted Hardy-Littlewood averages on the p-adic vector space, J. Math. Anal. Appl., 2006, 324, 1470-147710.1016/j.jmaa.2006.01.038Search in Google Scholar

[14] Wu Q.Y., Fu Z.W., Weighted p-adic Hardy operators and their commutators on p-adic central Morrey spaces, Bull. Malays. Math. Sci. Soc., 2017, 40, 1-2010.1007/s40840-017-0444-5Search in Google Scholar

[15] Coifman R.R., Meyer Y., On commutators of singular integrals and bilinear singular integrals, Trans. Amer. Math. Soc., 1975, 212, 315-33110.1090/S0002-9947-1975-0380244-8Search in Google Scholar

[16] Bényi Á., Oh T., Best constants for certain multilinear integral operators, J. Inequal. Appl. 2006, Article ID 2858210.1155/JIA/2006/28582Search in Google Scholar

[17] Wang S.M., Lu S.Z., Yan D.Y., Explicit constants for Hardy’s inequality with power weight on n-dimensional product spaces, Sci. China Math., 2012, 55, 2469-248010.1007/s11425-012-4453-4Search in Google Scholar

[18] Muckenhoupt B., Weighted norm inequalities for classical operators, Proc. Symp. Pure Math., 1979, 35, 69-8310.1090/pspum/035.1/545240Search in Google Scholar

[19] Pachpatte B.G., On multivariate Hardy type inequalities, An. stiint. Univ. Al.I. Cuza Iasi, Mat., 1992, 38, 355-361Search in Google Scholar

[20] Albeverio S., Khrennikov A.Yu. and Shelkovich M., Theory of p-adic distributions: linear and nonlinear models, Lodon Mathematical Lecture Note series, Vol. 370, Canbridge University Press, Cambridge, 201010.1017/CBO9781139107167Search in Google Scholar

Received: 2017-6-26
Accepted: 2017-11-24
Published Online: 2017-12-29

© 2017 Liu and Zhou

This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 License.

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