BOUNDEDNESS OF THE FRACTIONAL INTEGRAL OPERATOR WITH ROUGH KERNEL AND ITS COMMUTATOR IN VANISHING GENERALIZED VARIABLE EXPONENT MORREY SPACES ON UNBOUNDED SETS

MO Hui-xia, WANG Xiao-juan, HAN Zhe

(School of Science, Beijing University of Posts and Telecommunications, Beijing 100876, China)

Abstract: In this paper, we study the boundedness of fractional integral operators and their commutators in vanishing generalized Morrey spaces with variable exponent on unbounded sets.Using the properties of variable exponent functions and the pointwise estimates of operators TΩ,α and their commutators[b,TΩ,α]in Lebesgue spaces with variable exponent,we obtain the boundedness of fractional integral operators TΩ,α and their commutators [b,TΩ,α]in vanishing generalized Morrey spaces with variable exponents on unbounded sets, which extend the previous results.

Keywords: fractional integral operator with rough kernel; commutator; BMO function space; vanishing generalized Morrey space with variable exponents

1 Introduction

In recent years, the theory of variable exponent function spaces attracted ever more attention (see [1–8]for example), since Kovik and Pkosnk [1]introduced the variable exponents Lebesgue and Sobolev spaces, which are the fundamental works of variable exponent function spaces.The function spaces with variable exponent were applied widely in the image processing, fluid mechanics and partial differential equations with non-standard growth (see [9–13]for example).

Let Ω∈Ls(Sn−1) be homogeneous of degree zero on Rn, where Sn−1denotes the unit sphere of Rn(n ≥2) equipped with the normalized Lebesgue measuredσands ≥1.For 0<α

Moreover, letb ∈Then the commutator generated byTΩ,αandbcan be defined as follows

Recently, Tan and Liu [14]studied the boundedness ofTΩ,αon the variable exponent Lebesgue, Hardy and Herz-type Hardy spaces.Wang [15]et al.obtained the boundedness ofTΩ,αand its commutator [b,TΩ,α]on Morrey-Herz space with variable exponent.Tan and Zhao [16]established the boundedness ofTΩ,αand its commutator [b,TΩ,α]in variable exponent Morrey spaces.In 2016, Long and Han [17]established the boundedness of the maximal operator, potential operator and singular operator of Calden-Zygmund type in the vanishing generalized Morrey spaces with variable exponent.

Inspired by [14–17], in the paper, we consider the boundedness ofTΩ,αand its commutator [b,TΩ,α]generated byTΩ,αand BMO functions in vanishing generalized Morrey spaces with variable exponent on unbounded sets.

NotationThroughout this paper, Rnis then-dimensional Euclidean space,χAis the characteristic function of a setA ⊆Rn;Cis the positive constant, which may have different values even in the same line;ABmeans thatA ≤CBwith some positive constantCindependent of appropriate quantities and ifABandBA, we writeA≈B.

Now, let us recall some necessary definitions and notations.

Definition 1.1LetD ⊂Rnbe an open set andp(·) :D →[1,∞) be a measurable function.Then,Lp(·)(D) denotes the set of all measurable functionsfonDsuch that for someλ>0,

This set becomes a Banach function space when equipped with the Luxemburg-Nakano norm

Lp(·)(D) is regarded as variable exponent Lebesgue space.And, ifp(x)=pis a positive constant, thenLp(·)(D) is exactly the Lebesgue spaceLp(D).

Define the setsP0(D) andP(D) as followsP0(D) ={p(·) :D →[0,∞),p−> 0,p+<∞}, andP(D) ={p(·) :D →[1,∞),p−> 1,p+<∞}, wherep−=and

Definition 1.2Letf ∈then the Hardy-Littlewood maximal operator is defined by

where the supremum is taken over all balls containingx.

LetB(D) be the set ofp(·)∈P(D) such that the Hardy-Littlewood maximal operatorMis bounded onLp(·)(D).

Definition 1.3[18]LetD ⊂Rnbe an open setD ⊂Rnandp(·)∈P(Rn).p(·) is log-Hlder continuous, ifp(·) satisfies the following conditions

we denote byp(·)∈Plog(D).From Theorem 1.1 of[18],we know that ifp(·)∈Plog(D),thenp(·)∈B(D).

IfDis an unbounded set, we shall also use the assumption: there existsp(∞) =:And, we denote the subset ofwith the exponents satisfying the following decay condition,

Note that ifDis an unbounded set andp(∞)exists,then(1.4)is equivalent to condition(1.3).We would also like to remark thatif and only ifand

LetD ⊂Rnbe an open set andwhereB(x,r)is the ball centered atxand with radiusr.

Definition 1.4[3] For 0<λ(·)

Definition 1.5LetD ⊂Rnbe an unbounded open set and Π⊆D,ϕ(x,r) belongs to the classof non-negative functions on Π × [0,∞), which are positive on Π × (0,∞).Then for 1≤p(x)≤p+<∞, the generalized Morrey space with variable exponent is defined by

and

Definition 1.6LetD ⊂Rnbe an unbounded open set.The vanishing generalized Morrey space with variable exponentis defined as the space of functionsf ∈such that

Naturally, it is suitable to impose onϕ(x,r) with the following conditions

and

Noting that, if we replaceθp(x,r) withp(x) in Definition 1.5 and Definition 1.6, thenis the class vanishing generalized Morrey spaces with variable exponent,see[17]for example.Particularly,ifθp(x,r)=p(x),ϕ(x,r)=rλ(x)and Π =D,then the generalized Morrey space with variable exponentis exactly the Morrey space with variable exponentLp(·),λ(·)(D).

Definition 1.7Forb ∈then the space of functions of bounded mean oscillation is defined by BMO(Rn)=where

In the following, let us state the main results of the paper.

2 Main Results

Theorem 2.1Assume thatD ⊆Rnis an unbounded open set.Let 0<α

Theorem 2.2Assume thatD ⊆Rnis an unbounded open set and Π⊂D.Let 0<α

for eachδ>0, and

wherec0does not depend onx ∈Π andr>0.

Theorem 2.3Assume thatD ⊆Rnis an unbounded open set.Let 0<α

Theorem 2.4Assume thatD ⊆Rnis an unbounded open set and Π⊂D.Let 0<α

wherec0does not depend onx ∈Π andr>0.

3 Some Lemmas

In this part, we give some requisite lemmas.

Lemma 3.1(see [19, 20])(Generalized Hlder’s inequality) LetD ⊆Rn,p(·),q(·)∈P(Rn) such thatandg ∈Lq(·)(D), then

In general, ifp1(·),p2(·)...pm(·)∈P(Rn) such thatx ∈D.Then forfi ∈Lpi(·)(D),i=1,2,...,m, we have

Lemma 3.2(see[21]) LetIfp+

Lemma 3.3(see [5], Corollary 4.5.9) IfDis an unbounded set andthen

Lemma 3.4(see [22]) Letb ∈BMO(Rn),1

Lemma 3.5LetD ⊆Rnbe an unbounded open set,b ∈BMO(Rn)andp(·)Then for anyx ∈D,0

ProofLetsuch thatx ∈D.Then by Lemma 3.2, Lemma 3.3 and Lemma 3.4, we obtain

Lemma 3.6(see [23]) Letp(·),q(·)∈P(Rn),0then there existsC>0 such that

Lemma 3.7(see[23]) Letb ∈BMO(Rn),p(·),q(·)∈P(Rn),0withthen there exists a constantC>0 such that

4 Proof of Main Results

In this section, we will give the proofs of the main results.

Proof of Theorem 2.1Letthen we havef=f1+f2.By the sublinearity of the operatorTΩ,α, we obtain that

For the other part, let us estimate|TΩ,α(f2)(x)| for

Whenx ∈it is easy to see that|x0−y|≈|x −y|.Letx ∈D.Then by the generalized Hlder’s inequality and Lemma 3.3, we obtain

Combining the estimates of (4.1), (4.2) and (4.6) we have

which completes the proof of Theorem 2.1.

Proof of Theorem 2.2For everywe need to prove that

Now, let us show that

For 0

For anyε>0, now we choose a fixedδ0such that whenever 0

wherec0andCare constants from (2.3) and (4.7), which is possible since

This allows us to estimate the first term uniformly for 0

By choosingrsmall enough, we obtain the estimate of the second term.Indeed, by (2.2),we get

wherecδ0is the constant from (2.2).Sinceψsatisfies condition (1.6), we can choosersmall enough such that

Combining the estimates of (4.8) and (4.9), we obtain

Proof of Theorem 2.3Letthen we havef=f1+f2.Thus, it follows that

For the second part of (4.10), let us estimatefirst.It is easy to see that

From (4.5), it is easy to see that

Thus, according to Lemma 3.3 and Lemma 3.5, we deduce that

Whenx ∈B(x0,r) andit is easy to see that|x0−y|≈|x −y|.Letx ∈D.Then forby Lemma 3.1,we obtain

From (4.4) and Lemma 3.5, we have

and

Thus

From (4.12) and (4.16), we get

Combining the estimates of(4.10),(4.11)and(4.17),we completed the proof of Theorem 2.3.

Proof of Theorem 2.4The proof is similar to that of Theorem 2.2.From Theorem 2.3 and (2.6), it is easy to see thatSo, we just have to show that

For 0

where

and

For anyε>0, now we choose a fixedδ0>0 such that whenever 0

whereandCare constants from (2.6) and (4.18), respectively.It is possible sincef ∈This allows us to estimate the first term uniformly for 0

For the second part, from (2.5), it follows that

wherecδ0is the constant from(2.5).Sinceψsatisfies condition(1.6), it is possible to choosersmall enough such that

Thus

So, from the estimates of (4.19) and (4.20), it follows that

which means that

Therefore, the proof of Theorem 2.4 is completed.