Let be multilinear fractional integral operator and let . In this paper, the estimates of , the m-linear commutators and the iterated commutators on the generalized weighted Morrey spaces are established.
MSC:42B35, 42B20.
Hinweise
Competing interests
The authors declare that they have no competing interests.
Authors’ contributions
The authors completed the paper together. They also read and approved the final manuscript.
1 Introduction and results
The classical Morrey spaces were introduced by Morrey [1] in 1938, have been studied intensively by various authors, and together with weighted Lebesgue spaces play an important role in the theory of partial differential equations; they appeared to be quite useful in the study of local behavior of the solutions of elliptic differential equations and describe local regularity more precisely than Lebesgue spaces. See [2‐4] for details. Moreover, various Morrey spaces have been defined in the process of this study. Mizuhara [5] introduced the generalized Morrey space ; Komori and Shirai [6] defined the weighted Morrey spaces ; Guliyev [7] gave the concept of generalized weighted Morrey space , which could be viewed as an extension of both and . The boundedness of some operators on these Morrey spaces can be seen in [5‐9].
Let be the n-dimensional Euclidean space, be the m-fold product space (), and let be a collection of m functions on . Given and . We consider the multilinear fractional integral operators defined by
(1.1)
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The corresponding m-linear commutators and the iterated commutators defined by, respectively,
(1.2)
and
(1.3)
As is well known, multilinear fractional integral operator was first studied by Grafakos [10], subsequently, by Kenig and Stein [11], Grafakos and Kalton [12]. In 2009, Moen [13] introduced weight function and gave weighted inequalities for multilinear fractional integral operators; In 2013, Chen and Wu [14] obtained the weighted norm inequalities for the multilinear commutators and . More results of the weighted inequalities for multilinear fractional integral and its commutators can be found in [15‐17].
The aim of the present paper is to investigate the boundedness of multilinear fractional integral operator and its commutator on the generalized weighted Morrey spaces. Our results can be formulated as follows.
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Theorem 1.1Letand let . Suppose , , and , satisfy thecondition with , and , , satisfy the condition
(1.4)
where , . If , then there exists a constantCindependent ofsuch that
(1.5)
If , and , then there exists a constantCindependent ofsuch that
(1.6)
Theorem 1.2Letand let . Supposewith , and , satisfy thecondition with , , and , , satisfy the condition
(1.7)
where , . If , then there exists a constantindependent ofsuch that
(1.8)
and
(1.9)
2 Definitions and preliminaries
A weight ω is a nonnegative, locally integrable function on . Let denote the ball with the center and radius . For any ball B and , λB denotes the ball concentric with B whose radius is λ times as long. For a given weight function ω and a measurable set E, we also denote the Lebesgue measure of E by and set weighted measure .
The classical weight theory was first introduced by Muckenhoupt in the study of weighted boundedness of Hardy-Littlewood maximal functions in [18]. A weight ω is said to belong to for , if there exists a constant C such that for every ball ,
(2.1)
where is the dual of p such that . The class is defined by replacing the above inequality with
(2.2)
A weight ω is said to belong to if there are positive numbers C and δ so that
(2.3)
for all balls B and all measurable . It is well known that
(2.4)
We need another weight class introduced by Muckenhoupt and Wheeden in [19]. A weight function ω belongs to for if there is a constant such that, for every ball ,
(2.5)
When , ω is in the class with if there is a constant such that, for every ball ,
(2.6)
Let us recall the definition of multiple weights. For m exponents , we write . Let , , and let . Given , set . We say that satisfies the condition if it satisfies
Let , andwith . Assume thatand . Then for any ballB, there exists a constantsuch that
(2.9)
Let , let φ be a positive measurable function on , and let ω be a nonnegative measurable function on . Following [7], we denote by the generalized weighted Morrey space and the space of all functions with finite norm
(2.10)
where
Furthermore, by we denote the weak generalized weighted Morrey space of all function for which
(2.11)
where
(1)
If and with , then is the classical Morrey space.
(2)
If , then is the weighted Morrey space.
(3)
If , then is the two weighted Morrey space.
(4)
If , then is the generalized Morrey space.
(5)
If , then .
Let us recall the definition and some properties of . A locally integrable function b is said to be in if
Letfbe a real-valued nonnegative function and measurable onE. Then
(2.16)
At the end of this section, we list some known results about weighted norm inequalities for the multilinear fractional integrals and their commutators.
Let , letand let . For , , and , if , then there exists a constantsuch that
(2.19)
and
(2.20)
where .
3 Proof of Theorem 1.1
We first prove the following conclusions.
Theorem 3.1Letand let . Suppose , , and , satisfy thecondition with . If , then there exists a constantCindependent ofsuch that
(3.1)
If , and , then there exists a constantCindependent ofsuch that
(3.2)
where .
Proof We represent as , where , , and denotes the characteristic function of . Then
where each term of contains at least one . Since is an m-linear operator,
(3.3)
and
(3.4)
Then by (2.17), if , , we get
(3.5)
By (2.18), if , then
(3.6)
Applying Hölder’s inequality, for , , we have
for any ball . Then
Thus, for ,
From (2.7) and Lemma 2.2 we get
(3.7)
Using Hölder’s inequality,
Note that , then
(3.8)
Then for , ,
(3.9)
This gives and are majored by
(3.10)
For the other term, let us first consider the case when . For any , , we have for . Then
Applying Hölder’s inequality, it can be found that is less than
Hence,
Substituting (3.7) and (3.8) into the above, we obtain
(3.11)
Using Hölder’s inequality,
(3.12)
From (3.11) and (3.12) we know and are not greater than (3.10) for , .
Now we consider the case where exactly τ of the are ∞ for some . We only give the arguments for one of the cases. The rest is similar and can easily be obtained from the arguments below by permuting the indices. Then for any ,
Similar to the estimates for , we get
(3.13)
Then and are all less than
(3.14)
Combining the above estimates, the proof of Theorem 3.1 is completed. □
Now, we can give the proof of Theorem 1.1. From the definition of generalized weighted Morrey space, the norm of on equals
(3.15)
By Lemma 2.2 we have
(3.16)
Combining (3.1) and (3.16),
(3.17)
Since , from Lemma 2.7 and the fact are all non-decreasing functions of r, we get
(3.18)
Then
(3.19)
By (1.4) we get
(3.20)
Combining (3.15), (3.17), and (3.20), then
This completes the proof of first part of Theorem 1.1.
Similarly, the norm of on equals
(3.21)
Combining (3.2) and (3.16),
(3.22)
Substituting (3.20) into (3.22),
(3.23)
Then
This completes the proof of second part of Theorem 1.1.
4 Proof of Theorem 1.2
Theorem 4.1Letand let . Suppose , , and , satisfy thecondition with , . If , , then there exists a constantCindependent ofsuch that
(4.1)
and
(4.2)
where .
Proof We will give the proof for because the proof for is very similar but easier. Moreover, for simplicity of the expansion, we only present the case .
We represent as , where , , and denotes the characteristic function of . Then
(4.3)
Since bounded from to , we get
Then by (3.9) we get
(4.4)
Owing to the symmetry of II and , we only estimate II. Taking , then
(4.5)
Similar to the estimate of (3.13), for any we can deduce
(4.6)
By Lemma 2.1 we know . Applying Hölder’s inequality and (2.13), we have
(4.7)
Then by (4.6), (4.7), and (3.12), we have
(4.8)
For any , we have
(4.9)
Note that
(4.10)
and
(4.11)
Then
(4.12)
From Lemma 2.1 we know , then by Lemma 2.4 we get
(4.13)
By (3.7) and (3.8) we have
(4.14)
From (4.12), (4.13), and (4.14) we can deduce
(4.15)
Applying (2.13) and (3.12) we have
(4.16)
Then by (4.15) and (4.16),
(4.17)
Similarly, we also have
(4.18)
For any , with the same method of estimate for (4.15) we have
(4.19)
Then
(4.20)
Then combining (4.8), (4.17), (4.18), and (4.20) we get
(4.21)
Finally, we still decompose as follows:
(4.22)
Because each term is completely analogous to , , being slightly different, we get the following estimate without details:
(4.23)
Summing up the above estimates, (4.2) is proved for . □
In the following we give the proof of Theorem 1.2. From (3.16) and (4.2),
(4.24)
Since , , satisfy the condition (1.7), and , by (3.18) we get
(4.25)
Combining (4.24) and (4.25), we have
Acknowledgements
The authors would like to thank the referees and the Editors for carefully reading the manuscript and making several useful suggestions.
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Competing interests
The authors declare that they have no competing interests.
Authors’ contributions
The authors completed the paper together. They also read and approved the final manuscript.