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Research article

Some new characterizations of boundedness of commutators of p-adic maximal-type functions on p-adic Morrey spaces in terms of Lipschitz spaces

  • Received: 12 March 2024 Revised: 27 May 2024 Accepted: 28 May 2024 Published: 17 June 2024
  • MSC : 26A51, 26A33, 26D10

  • In this note, we investigate some new characterizations of the p-adic version of Lipschitz spaces via the boundedness of commutators of the p-adic maximal-type functions, including p-adic sharp maximal functions, p-adic fractional maximal functions, and p-adic fractional maximal commutators on p-adic Morrey spaces, when a symbol function b belongs to the Lipschitz spaces.

    Citation: Naqash Sarfraz, Muhammad Bilal Riaz, Qasim Ali Malik. Some new characterizations of boundedness of commutators of p-adic maximal-type functions on p-adic Morrey spaces in terms of Lipschitz spaces[J]. AIMS Mathematics, 2024, 9(7): 19756-19770. doi: 10.3934/math.2024964

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  • In this note, we investigate some new characterizations of the p-adic version of Lipschitz spaces via the boundedness of commutators of the p-adic maximal-type functions, including p-adic sharp maximal functions, p-adic fractional maximal functions, and p-adic fractional maximal commutators on p-adic Morrey spaces, when a symbol function b belongs to the Lipschitz spaces.



    In the contemporary era, p-adic analysis is so significant that there is a lot of research being done on theories that are only concerned with p-adic objects, a case in point is the p-adic Hodge theory [1], Coleman's theory of p-adic integration [2], p-adic geometry [3], the theory of p-adic differential equations [4], the p-adic Langlands correspondence [5], study of p-adic cohomologies [6], and the study of p-adic modular forms [7]. In this connection, numerous of these concepts and advancements are present in the proof of Fermet's last theorem [8]. Recently, they have been applied in mathematical physics [9] and harmonic analysis [10,11,12,13,14,15,16].

    Ostrowski's theorem states that any nontrivial norm on the field of rational numbers Q is either the p-adic norm ||p, or the real norm ||, where p is a prime number. The former norm is stated as follows, if any rational number r is represented as r=pθmn, where θ=θ(x)Z, (p,m,n)=1 and m,nZ, then

    |0|p=0,|r|p=pθr0.

    This norm exhibits an ultrametric property

    |r+s|pmax{|r|p,|s|p}.

    A symbol Qp is the field of p-adic numbers, and is the completion of field of rational numbers Q with respect to the norm ||p. Any Qpr0 is uniquely represented as, see [9]

    r=pθk=0γkpk, (1.1)

    where γk,θZ, γkZpZp,γ00. It is eminent that the series in (1.1) is convergent as |γkpk|=pk.

    The n-dimensional field Qnp is defined as n-tuples of p-adic numbers, (r1,r2,,rn), where Qprk, k=1,2,,n. The n-dimensional p-adic numbers inherit many properties from the p-adic numbers. They form a complete metric space with respect to the n-dimensional p-adic metric d(r,s)=|rs|p, which measures the divisibility of n-tuples by powers of p. The n-dimensional p-adic metric induces a topology on Qnp, allowing for the study of continuity, convergence, and limit concepts in this space. The norm on Qnp is

    |r|p=max1kn|rk|p.

    The p-adic ball Bθ(x) and p-adic sphere Sθ(x) with radius pθ and center x are defined by

    Bθ(x)={rQnp:|rx|ppθ}, Sθ(x)={rQnp:|rx|p=pθ}.

    Since Qnp is a locally compact commutative group, then there exists a Haar measure dy on the additive group Qnp, which is normalized by

    B0(0)dy=1.

    From standard analysis, we get |Bθ(x)|h=pnθ and |Sθ(x)|h=pnθ(1pn), for any xQnp.

    A measurable function b defined on Qnp is in Lp(Qnp) (1p), if it satisfies

    bLp(Qnp)=(Qnp|b(x)|pdx)1/p<,1p<,
    bL(Qnp)=esssupxQnp|b(x)|<.

    The commutators of harmonic analysis are vital integral operators and play a crucial role in examining the regularity characteristics of solutions to various partial differential equations, for instance [17,18,19,20]. Suppose T is a classical singular integral operator with an another function b, then the commutator [b,T] generated by T is defined as follows:

    [b,T](f)=bT(f)T(bf). (1.2)

    In [21], authors have studied the Lp boundedness of (1.2) with bB˙MO(Rn). These results were extended with bΛδ(Rn) in [22]. Since then, a great attention has been paid with studying the commutators of operators; see for instance, [17,23,24,25].

    In what follows, for fL1loc(Qnp), we define the p-adic sharp maximal function Mp, and p-adic fractional maximal function Mpα as

    Mp,f(x)=supθZ1|Bθ(x)|hBθ(x)|f(t)fBθ(x)|dt (1.3)

    and

    Mpαf(x)=supθZ1|Bθ(x)|1αnhBθ(x)|f(t)|dt, (1.4)

    where fBθ(x)=1|Bθ(x)|hBθ(x)f(t)dt. When α=0, we get the Hardy Littlewood maximal function Mp, which is defined as:

    Mpf(x)=supθZ1|Bθ(x)|hBθ(x)|f(t)|dt.

    Significant work has been done intensively in the past on Mp by many researchers; see for example, [26,27,28] and the references therein.

    The p-adic fractional commutator of Mpα with bL1loc(Qnp) is defined by

    Mpα,bf(x)=supθZ1|Bθ(x)|1αnhBθ(x)|b(x)b(t)||f(t)|dt.

    On the other hand, nonlinear commutators of respectively Mp, and Mpα with a locally integrable function b are defined by

    [b,Mp,](f)(x)=b(x)Mp,(f)(x)Mp,(bf)(x) (1.5)

    and

    [b,Mpα](f)(x)=b(x)Mpα(f)(x)Mpα(bf)(x). (1.6)

    When α=0, [b,Mpα] reduces to [b,Mp], see [29]. In p-adic setting, boundedness of commutators of p-adic maximal function is a new area, and we only found some work in [29]. In that paper, the authors acquired the boundedness of commutators of Mp on p-adic function spaces with bB˙MO(Qnp). However, in the case of Euclidean, commutators of maximal-type functions have spotlighted many researchers. For example, in [17], Bastero et al. obtained the boundedness of commutators of maximal and sharp functions on Lebesgue spaces with bB˙MO(Rn). Furthermore, the results of [17] are extended in [30]. Zhang [31] further obtained the characterizations of nonlinear commutators of the Hardy Littlewood maximal function and sharp maximal function in variable exponent Lebesgue spaces with bΛδ(Rn). Recently, Xuechun et al. [32] established new characterizations of Lipschitz space in terms of the boundedness of [b,M] and [b,Mα] in the context of variable Lipschitz space.

    As we observed in the above work, the characterization of nonlinear commutators of Mp, and Mpα remains widely open. Therefore, we obtain some characterizations of p-adic versions of Lipschitz spaces via the boundedness of Mp, and Mpα on p-adic Morrey spaces, by considering b from Lipschitz spaces under certain assumptions. Throughtout this article, a letter C represents a constant with different or the same values at different places, and χBθ is the characteristic function of Bθ(x).

    Definition 1.1. Let 1p< and 0λn. The p-adic Morrey space Lp,λ(Qnp) is defined as follows:

    Lp,λ(Qnp)={bLploc(Qnp):bLp,λ(Qnp)<}, (1.7)

    where

    bLp,λ(Qnp)=supθZxQnp(1|Bθ(x)|λ/nhBθ(x)|b(x)|pdx)1/p.

    Remark 1.1. It is evident that Lp,1/p(Qnp)=Lp(Qnp) and Lp,0(Qnp)=L(Qnp).

    Definition 1.2. The Lipschitz space Λδ(Qnp), (δR+) is the space of all measurable functions b on Qnp such that

    bΛδ(Qnp)=supt,hQnp,h0|b(t+h)b(t)||h|δp<.

    Next, we have the p-adic version of the Lipschitz space ˜Λδ(Qnp), which is the space of all measurable functions b on Qnp with the following norm:

    b˜Λδ(Qnp)=supxQnp,θZ1|Bθ(x)|1+δnhBθ(x)|b(t)bBθ(x)|dt<,

    where bBθ(x)=1|Bθ(x)|hBθ(x)b(t)dt.

    In the following section, we state some characterizations of the p-adic version of Lipschitz spaces via the boundedness of the commutators of [b,Mp,], Mαα,b, and [b,Mpα].

    Theorem 2.1. Suppose b is a locally integrable function, 1<q<n/δ, 0<λ<nqδ, δ(0,1), and 1p+δnλ=1q. Then, [b,Mp,]: Lq,λ(Qnp)Lp,λ(Qnp) if and only if bΛδ(Qnp) with b0.

    Theorem 2.2. Suppose b is a locally integrable function, 1<q<n/δ, 0<λ<nqδ, δ(0,1), and 1p+δ+αnλ=1q. Then, Mpα,b: Lq,λ(Qnp)Lp,λ(Qnp) if and only if bΛδ(Qnp).

    Theorem 2.3. Suppose b is a locally integrable function, 1<q<n/δ, 0<λ<nqδ, δ(0,1), and 1p+δ+αnλ=1q. Then, [b,Mpα]:Lq,λ(Qnp)Lp,λ(Qnp) if and only if bΛδ(Qnp) with b0.

    Since Lp,1/p(Qnp)=Lp(Qnp). So, we have the characterizations in terms of the boundedness of operators [b,Mp,], Mpb, and [b,Mp] on Lebesgue spaces.

    Corollary 2.1. Suppose b is a locally integrable function, 1<q<n/δ, δ(0,1), and 1p+δn=1q. Then, [b,Mp,]: Lq(Qnp)Lp(Qnp) if and only if bΛδ(Qnp) with b0.

    Corollary 2.2. Suppose b is a locally integrable function, 1<q<n/δ, 0<λ<nqδ, δ(0,1), and 1p+δ+αn=1q. Then, Mpα,b: Lq(Qnp)Lp(Qnp) if and only if bΛδ(Qnp).

    Corollary 2.3. Suppose b is a locally integrable function, 1<q<n/δ, 0<λ<nqδ, δ(0,1), and 1p+δ+αn=1q. Then, [b,Mpα]:Lq(Qnp)Lp(Qnp) if and only if bΛδ(Qnp) with b0.

    In order to prove the above results, we need some lemmas and remarks. We begin with a very useful result.

    Lemma 2.1. The p-adic space Λδ(Qnp) coincides with ˜Λδ(Qnp), for 0<δ<1.

    Proof. Consider a ball Bθ(x) and tBθ(x), then from the definition (1.2), we have

    |b(t)bBθ(x)|1|Bθ(x)|hBθ(x)|b(t)b(z)|dzbΛδ(Qnp)1|Bθ(x)|hBθ(x)|tz|δhdzCbΛδ(Qnp)1|Bθ(x)|h|Bθ(x)|δnhBθ(x)dzCbΛδ(Qnp)|Bθ(x)|δnh.

    We further proceed as

    Bθ(x)|b(t)bBθ(x)|dtCbΛδ(Qnp)Bθ(x)|Bθ(x)|δnhdtCbΛδ(Qnp)|Bθ(x)|1+δ/nh,

    which implies that

    1|Bθ(x)|1+δ/nhBθ(x)|b(t)bBθ(x)|dtCbΛδ(Qnp).

    Therefore,

    b˜Λδ(Qnp)CbΛδ(Qnp). (2.1)

    On the other hand, let b˜Λδ(Qnp). For any t,zQnp with tz. We set B=B(t,|tz|p) and B=B(z,|tz|p). Then we have

    |b(t)b(z)||b(t)bB|+|b(z)bB|+|bBbB|. (2.2)

    Estimates of all terms on the right-hand side of (2.2) are more or less the same. So, we will estimate the first term. Let Bj=B(t,pj|tx|p) for j1 and B0=B. We proceed as

    |b(t)bB|limθ(|b(t)bBθ|+θ1j=0|bBj+1bBj|)Cj=11|Bj|hBj|b(z)bBj|dzCb˜Λδ(Qnp)j=1|Bj|δ/nhCb˜Λδ(Qnp)j=1pδj+logp|tz|δpC|tz|δpb˜Λδ(Qnp).

    Consequently,

    bΛδ(Qnp)Cb˜Λδ(Qnp). (2.3)

    From (2.1) and (2.3), we have completed the proof.

    In what follows, taking into account the characteristic function χBθ(x), we have the following property:

    Lemma 2.2. Suppose 1q< and 0<λ<n, then

    χBθ(x)Lq,λ(Qnp)=|Bθ(x)|nλnqh=pθ(nλ)q.

    Next, the fractional integral operator on Qnp is introduced by Taibleson [33] and is defined by

    Tpαf(x)=1pα1pαnQnpf(t)|xt|αnpdt,0<α<n.

    The following lemma shows the boundedness of Tpα on p-adic Morrey spaces, which is proved in a book [33].

    Lemma 2.3. Suppose 1<q<n/α, 0<α<n, 0<λ<nq, and 1p+αnλ=1q, then Tpα is bounded from Lq,λ(Qnp) to Lp,λ(Qnp).

    Remark 2.1. From the condition of Lemma 2.3, we get

    |Tpα(|f|)(x)|=|Qnp|f(t)||xt|αpdt|Bθ(x)|f(t)||xt|αpdt1pθ(nα)Bθ(x)|f(t)|dt.

    Therefore,

    |Mpα(f)(x)|CTpα(|f|)(x).

    From here, we deduce that Mpα is bounded from Lq,λ(Qnp) to Lp,λ(Qnp).

    Proof of Theorem 2.1. Consider any bΛδ(Qnp) with b0, we prove that [b,Mp,]: Lq,λ(Qnp)Lp,λ(Qnp). Let fLq,λ(Qnp). From definition (1.2), we deduce

    |[b,Mp,](f)(x)|=|supθZb(x)|Bθ(x)|hBθ(x)|f(t)fBθ(x)|dtsupθZ1|Bθ(x)|hBθ(x)|b(t)f(t)(bf)Bθ(x)|dt|supθZ1|Bθ(x)|hBθ(x)(|b(t)b(x)||f(t)|+|b(x)fBθ(x)(bf)Bθ(x)|)dtbΛδ(Qnp)supθZ1|Bθ(x)|hBθ(x)|tx|δ(x)p|f(t)|dt+supθZ|b(x)|Bθ(x)|hBθ(x)f(y)dy1|Bθ(x)|hBθ(x)b(y)f(y)dy|bΛδ(Qnp)supθZ1|Bθ(x)|hBθ(x)|tx|δ(x)p|f(t)|dt+supθZ1|Bθ(x)|hBθ(x)|b(x)b(y)||f(y)|dybΛδ(Qnp)supθZ1|Bθ(x)|hBθ(x)|tx|δ(x)p|f(t)|dt+bΛδ(Qnp)supθZ1|Bθ(x)|hBθ(x)|xy|δ(x)p|f(y)|dyCbΛδ(Qnp)supθZ1|Bθ(x)|1δ(x)nhBθ(x)|f(t)|dtCbΛδ(Qnp)Mδ(x)f(x). (2.4)

    From Remark 2.1 and equation (2.4), we obtain

    [b,Mp,](f)Lp,λ(Qnp)CbΛδ(Qnp)fLq,λ(Qnp).

    Hence, [b,Mp,]: Lq,λ(Qnp)Lp,λ(Qnp).

    Conversely, suppose that [b,Mp,]: Lq,λ(Qnp)Lp,λ(Qnp). We need to show bΛδ(Qnp) and b0. Consider any fixed p-adic ball Bθ(x), and tBθ(x). We see in [29] that

    Mp,(χBθ(x))(t)=2(p1)p2.

    By above expression, Eq (1.5) and the boundedness of [b,Mp,], we reach at

    (bp22(p1)Mp,(bχBθ(x)))χBθ(x)Lp,λ(Qnp)=p22(p1)(2(p1)p2bMp,(bχBθ(x)))χBθ(x)Lp,λ(Qnp)=p22(p1)(bMp,(χBθ(x))Mp,(bχBθ(x)))χBθ(x)Lp,λ(Qnp)
    =p22(p1)[b,Mp,](χBθ(x))Lp,λ(Qnp)CχBθ(x)Lq,λ(Qnp),

    which implies that

    (bp22(p1)Mp,(bχBθ(x))χBθ(x)Lp,λ(Qnp)χBθ(x))Lq,λ(Qnp)C. (2.5)

    Now, consider a p-adic ball Bθ(x)Qnp. From [29], we see that for any tBθ(x),

    |bBθ(x)|p22(p1)Mp,(bχBθ(x))(t). (2.6)

    Now to achieve bΛδ(Qnp), we let A={tBθ(x):b(t)bBθ(x)}. Moreover, consider any tA and we get b(t)bBθ(x)|bBθ(x)|2Mp,(bχBθ(x))(t), then

    |b(t)bBθ(x)||b(t)p22(p1)Mp,(bχBθ(x))(t)|. (2.7)

    Since 1p=1qδnλ, then using (2.7) along with Hölder's inequality, Lemma 2.2, and (2.5), we ultimately have

    1|Bθ(x)|1+δ/nhBθ(x)|b(t)bBθ(x)|dt=2|Bθ(x)|1+δ/nhA|b(t)bBθ(x)|dt2|Bθ(x)|1+δ/nhBθ(x)|b(t)p22(p1)Mp,(bχBθ(x))(t)|dt2|Bθ(x)|1+δ/nh(Bθ(x)|b(t)p22(p1)Mp,(bχBθ(x))(t)|pdt)1/p×(Bθ(x)χBθ(x)(t)dt)1/p2|Bθ(x)|1+δ/nh.|Bθ(x)|λ/nph(1|Bθ(x)|λ/nhBθ(x)|b(t)p22(p1)Mp,(bχBθ(x))(t)|pdt)1/p×(Bθ(x)χBθ(x)(t)dt)1/p2|Bθ(x)|1+δ/nλ/nph(bp22(p1)Mp,(bχBθ(x)))(χBθ(x))Lp,λ(Qnp)×χBθ(x)Lp(Qnp)=2χBθ(x)Lq,λ(Qnp)(bp22(p1)Mp,(bχBθ(x)))(χBθ(x))Lp,λ(Qnp)C. (2.8)

    This shows that b˜Λδ(Qnp). This, along with Lemma 2.1, shows bΛδ(Qnp).

    The final task is to show that b0. For this its suffices to show b=0, where b=min{b,0} and b+=|b|b. Consider a p-adic ball Bθ(x). Using (2.6), we observe that

    p22(p1)Mp,(bχBθ(x))(t)b(t)|bBθ(x)|b+(t)+b(t),

    for any tBθ(x).

    Now averaging on a ball Bθ(x), we deduce that

    1|Bθ(x)|hBθ(x)|p22(p1)Mp,(bχBθ(x))(t)b(t)|dt1|Bθ(x)|hBθ(x)(|bBθ(x)|b+(t)+b(t))dt=|bBθ(x)|1|Bθ(x)|hBθ(x)b(t)dt+1|Bθ(x)|hBθ(x)b(t)dt. (2.9)

    On the other hand, from (2.8), we have

    1|Bθ(x)|1+δ/nhBθ(x)|p22(p1)Mp,(bχBθ(x))(t)b(t)|dtC. (2.10)

    From this and (2.9), we get

    (|bBθ(x)|1|Bθ(x)|hBθ(x)b+(t)dt+1|Bθ(x)|hBθ(x)b(t)dt)C|Bθ(x)|δ/nh. (2.11)

    By letting θ with tBθ(x), the Lebesgue differentiation theorem in the p-adic field ensures that

    0=|bBθ(x)|b+(t)+b(t)=2b(t)=2|b(t)|.

    Consequently, b=0, and hence b0 holds true, which complete the proof of theorem.

    Proof of Theorem 2.2. Suppose bΛδ(Qnp). We show that Mα,b: Lq(Qnp)Lp(Qnp). From the definition of (1.2) and Eq (1.4), we deduce

    |Mα,b(f)(x)|=supθZ1|Bθ(x)|1αnhBθ(x)|b(x)b(t)||f(t)|dtbΛδ(Qnp)supθZ1|Bθ(x)|1αnhBθ(x)|tx|δ(x)p|f(t)|dtbΛδ(Qnp)supθZ1|Bθ(x)|1α+δ(x)nhBθ(x)|f(t)|dtbΛδ(Qnp)Mα+δx(f)(x).

    By this and boundedness of Mα+δ from Lq,λ(Qnp) to Lp,λ(Qnp) (see Remark 2.1), we eventually have

    Mα,b(f)Lp,λ(Qnp)CbΛδ(Qnp)Mα+δ(f)Lp,λ(Qnp)CbΛδ(Qnp)fLq,λ(Qnp).

    Conversely, suppose that [Mα,b]: Lq,λ(Qnp)Lp,λ(Qnp), we show that bΛδ(Qnp). For this, consider a p-adic ball Bθ(x), we are down to

    |(b(t)bBθ(x))χBθ(x)(t)||Bθ(x)|αnhMα,b(χBθ(x))(t). (2.12)

    From (2.12) and that [Mα,b]: Lq,λ(Qnp)Lp,λ(Qnp), we obtain

    (b(t)bBθ(x))χBθ(x)Lp,λ(Qnp)|Bθ(x)|αnhMα,b(χBθ(x))Lp,λ(Qnp)C|Bθ(x)|αnhχBθ(x)Lq,λ(Qnp),

    which implies that

    (b(t)bBθ(x))χBθ(x)Lp,λ(Qnp)χBθ(x)Lq,λ(Qnp)C|Bθ(x)|αnh. (2.13)

    Since 1p=1qδ+αn, making use of Hölder's inequality, Lemma 2.2, and (2.13), we have

    1|Bθ(x)|1+δ/nhBθ(x)|b(t)bBθ(x)|dt1|Bθ(x)|1+δ/nλ/nph(1|Bθ(x)|λ/nhBθ(x)|b(t)bBθ(x)|pdt)1/p×(Bθ(x)χBθ(x)(t)dt)1/p1|Bθ(x)|1+δ/nλ/nph(bbBθ(x))χBθ(x)Lp,λ(Qnp)χBθ(x)Lp(Qnp)=1χBθ(x)Lq(Qnp)(bbBθ(x))χBθ(x)Lp,λ(Qnp)|Bθ(x)|αnhC. (2.14)

    This shows that b~Λδ(Qnp). From this and Lemma 2.1, we have bΛδ(Qnp), which finishes the proof.

    Before proving Theorem 2.3, we define the p-adic fractional maximal operator MpBθ(x) with respect to a p-adic ball as follows:

    MpBθ(x)(f)(t)=supBθ0(t)Bθ(x)1|Bθ0(t)|1θnhBθ0(t)|f(t)|dt,θ0,

    where supremum is taken over all balls Bθ0(t) such that Bθ0(t)Bθ(x).

    Proof of Theorem 2.3. Assume that bΛδ(Qnp) and b0. We show that [b,Mα]: Lq,λ(Qnp)Lp,λ(Qnp). Let fLq,λ(Qnp). From definitions of (1.2), we reach at

    |[b,Mα](f)(x)|=|supθZ1|Bθ(x)|1αnhBθ(x)b(x)|f(t)|dtsupθZ1|Bθ(x)|1αnhBθ(x)|b(t)f(t)|dt|supθZ1|Bθ(x)|1αnhBθ(x)|b(x)b(t)||f(t)|dt=Mpα,b(f)(x). (2.15)

    From (2.15) and Theorem 2.2, we acquire

    [b,Mpα](f)Lp,λ(Qnp)Mpα,b(f)Lp,λ(Qnp)CbΛδ(Qnp)fLq,λ(Qnp).

    Consequently, [b,Mpα]: Lq,λ(Qnp)Lp,λ(Qnp).

    Conversely, suppose [b,Mpα]: Lq,λ(Qnp)Lp,λ(Qnp). We need to show that

    bΛδ(Qnp)andb0. (2.16)

    First, we opt for the former one, and in order to do so, we need the following preparation:

    Consider a p-adic ball Bθ(x). For all tBθ(x), we have

    Mα(χBθ(x))(t)=Mα,Bθ(x)(χBθ(x))(t)=|Bθ(x)|αnh

    and

    Mα(bχBθ(x))(t)=Mα,Bθ(x)(b)(t).

    Then, from this and (1.6), we have

    b(t)|Bθ(x)|αnhMα,Bθ(x)(b)(t)=|Bθ(x)|αnh[b(t)|Bθ(x)|αnhMα,Bθ(x)(b)(t)]=|Bθ(x)|αnh[b(t)Mα(χBθ(x))(t)Mα(bχBθ(x))(t)]=|Bθ(x)|αnh[b,Mα](χBθ(x))(t).

    which implies that

    (b(t)|Bθ(x)|αnhMα,Bθ(x)(b)(t))χBθ(x)(t)=|Bθ(x)|αnh[b,Mα](χBθ(x))(t)χBθ(x)(t). (2.17)

    From (2.17) and the boundedness of [b,Mpα], we obtain

    (b|Bθ(x)|αnhMα,Bθ(x)(b))(χBθ(x))Lp,λ(Qnp)C|Bθ(x)|αnhχBθ(x)Lq,λ(Qnp),

    which implies that

    (b|Bθ(x)|αnhMα,Bθ(x)(b))(χBθ(x))Lp,λ(Qnp)χBθ(x)Lq,λ(Qnp)C|Bθ(x)|αnh. (2.18)

    Furthermore, consider a p-adic ball Bθ(x), suppose A={tBθ(x):b(t)Bθ(x)}. Now, for any tA, we have

    b(t)bBθ(x)|bBθ(x)||Bθ(x)|αnhMα,Bθ(x)(b)(t).

    Thus,

    |b(t)bBθ(x)||b(t)|Bθ(x)|αnhMα,Bθ(x)(b)(t)|. (2.19)

    Since 1p=1qδ+αn, from (2.19), Hölder's inequality, Lemma 2.2, and (2.18), we sum up that

    1|Bθ(x)|1+δ/nhBθ(x)|b(t)bBθ(x)|dt=2|Bθ(x)|1+δ/nhA|b(t)bBθ(x)|dt2|Bθ(x)|1+δ/nhBθ(x)|b(t)|Bθ(x)|αnhMα,Bθ(x)(b)(t)|χBθ(x)(t)|dt2|Bθ(x)|1+δ/nλ/nph(b|Bθ(x)|αnhMα,Bθ(x)(b))χBθLp,λ(Qnp)χBθLp(Qnp)CχBθ(x)Lq(Qnp)(b|Bθ(x)|αnhMα,Bθ(x)(b))χBθLp,λ(Qnp)|Bθ(x)|αnC. (2.20)

    which implies that b˜Λδ(Qnp), so, it follows from this and Lemma 2.1 that bΛδ(Qnp).

    Next, we show the latter one in equation (2.16). For this, its suffices to show b=0, where b=min{b,0} and b+=|b|b. Consider any fixed p-adic ball Bθ(x) and for any tBθ(x), we have

    0b+(t)|b(x)|Bθ(x)|αnMα,Bθ(x)(b)(t).

    Therefore, for tBθ(x), we obtain

    0b(t)|Bθ(x)|αnhMα,Bθ(x)(b)(t)b+(t)+b(t)=|Bθ(x)|αnhMα,Bθ(x)(b)(t)b(t).

    Then, by this and (2.20), we have

    1|Bθ(x)|1+δ/nhBθ(x)b(t)dt1|Bθ(x)|1+δ/nhBθ(x)|Bθ(x)|αnhMα,Bθ(x)(b)(t)b(t)C.

    Therefore,

    1|Bθ(x)|hBθ(x)b(t)dtC|Bθ(x)|δ/nh.

    By letting θ together with the Lebesgue differentiation theorem in p-adic field, we have b=0. Hence b0, which finishes the proof of theorem.

    Necessary and sufficient conditions for the boundedness of commutators of p-adic sharp maximal functions, p-adic fractional maximal functions, and p-adic fractional maximal commutators on p-adic Morrey spaces are studied by considering the symbol function as a Lipschitz spaces. Wavelet characterization of p-adic Lebesgue spaces can be obtained as a future prospect.

    Naqash Sarfraz: Conceptualization, data curation, investigation, methodology, writing-original draft; Muhammad Bilal Riaz: Formal analysis, methodology, writing-original draft; project management, funding acquisition, supervision; Qasim Ali Malik: Validation, visualization, writing-review & editing. All authors have read and approved the final version of the manuscript for publication.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    The Author Muhammad Bilal Riaz thankful to Ministry of Education, Youth and Sports of the Czech Republic for their support through the e-INFRA CZ (ID:90254).

    The authors declare that they have no conflict of interest.



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