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Volume 2008, Article ID 373050,17pages doi:10.1155/2008/373050

Research Article

A Class of Commutators for Multilinear Fractional

Integrals in Nonhomogeneous Spaces

Jiali Lian and Huoxiong Wu

School of Mathematical Sciences, Xiamen University, Xiamen Fujian, 361005, China

Correspondence should be addressed to Huoxiong Wu,[email protected]

Received 3 March 2008; Accepted 16 July 2008

Recommended by Nikolaos Papageorgiou

Letμ be a nondoubling measure onRd. A class of commutators associated with multilinear fractional integrals and RBMOμfunctions are introduced and shown to be bounded on product of Lebesgue spaces withμ.

Copyrightq2008 J. Lian and H. Wu. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

1. Introduction

In recent years, the study of multilinear operators and their commutator has been attracting many researchers. Many results which parallel to the linear theory of classical integral operators are obtained. For details, one can see1–4, and so forth. Meanwhile, as a further development, harmonic analysis on Rd with nondoubling measures has been developed rapidly. Many results of singular integrals and the related operators on Euclidean spaces with Lebesgue measure have been generalized to the Lebesgue spaces with nondoubling measures

see5–10, etc.. Motivated by5,8, we will consider the commutators generated by a class of multilinear fractional integrals and RBMO functions with nondoubling measure, which were introduced by Tolsa in11.

Before stating our results, we recall some definitions and notations. Letμbe a Radon measure onRd satisfying the following growth condition; there exist constants C > 0 and

n∈0, d, such that

μQClQn

, 1.1

for any cubeQ ⊂ Rd with sides parallel to the coordinate axes, where lQ stands for the side length ofQ. Forr > 0,rQ will denote the cube with the same center as Q and with

(2)

Let 0≤β < n, given two cubesQRinRd, we set

KQ,Rβ 1 NQ,R

k1

μ2kQ l2kQn

1−β/n

, 1.2

whereNQ,Ris the first integerksuch thatl2kQlR. Ifβ0, thenK0Q,RKQ,R. The later quantity was introduced by Tolsa in11.

Givenβd depending ondlarge enoughe.g.,βd>2n, we say that a cubeQ⊂ Rdis doubling ifμ2QβdμQ.

Given a cube Q ⊂ Rd, let N be the smallest nonnegative integer such that 2NQ is doubling. We denote this cube byQ.

Letη > 1 be a fixed constant. We say thatbL1

locμis in RBMOμif there exists a constantC1such that for any cubeQ

1

μηQ

Q

bym

Qb dμyC1,

mQbmRb C1KQ,R, for any two doubling cubesQR, 1.3

wheremQbμQ−1

Qbydμy. The minimal constantC1is the RBMOμnorm ofb, and it will be denoted byb∗. In11, Tolsa obtained equivalent norm in the space RBMOμwith

different parametersη >1 andβd>2n.

We consider the following multilinear fractional integral operator

Iα,m

f1, . . . , fm

x

Rdm

f1

xy1

f2

xy2

· · ·fm

xym

y1, y2, . . . , ym mnα

y1

· · ·dμym

. 1.4

Form1, we denoteIα,1by, which is the Riesz potential operator related toμ. Given m ∈ N, for all 1 ≤ jm, we denote by Cm

j the family of all finite subsets

σ {σ1, . . . , σj}of{1,2, . . . , m}ofj different elements. For anyσCjm, we denoteσ {1,2, . . . , m} \σ {σj 1, . . . , σm}. Moreover, for bj ∈ RBMOμ, j 1,2, . . . , m, let

b b1, b2, . . . , bmand denote by bσ1, . . . , bσjand by x 1x· · ·bσjx. Also, we denotef f1, . . . , fm, fσ1, . . . , fσj,bσfσ bσj1fσj1, . . . , bσmfσm. We define a kind of commutator ofIα,mas follows:

b, Iα,m

fx

m

j0

σCm j

−1mjbσxIα,m

fσ, bσfσ

x. 1.5

In particular, form2, we define

b1, b2, Iα,2

f1, f2

x b1xb2xIα,2

f1, f2

x−b1xIα,2

f1, b2f2

x −b2xIα,2

b1f1, f2

x Iα,2

b1f1, b2f2

x. 1.6

Obviously, form 1, the operator defined in 1.5is the Coifman-Rochberg-Weiss type commutator of fractional integral,b, Iα. Under the assumption thatμis a nondoubling measure, Chen and Sawyer5established theLp, Lq-boundedness ofb, I

(3)

Theorem 1.1. Letμbe defined as above andμ∞,bj ∈RBMORd,j1,2,0< α <2n. Then

b1, b2, Iα,2is a bounded operator fromLqLq2 toLq with1/q 1/q11/q2−α/2n > 0and 1< q1,q2 <.

Remark 1.2. ByLemma 2.2inSection 2,Theorem 1.1for the caseμ<∞also holds provided

Iα,2,b1, b2, Iα,2,b1, Iα,2, andb2, Iα,2satisfy certainT1type conditions. For instance, ifIα,2 satisfies theT1condition, that is,I∗1

α,2 0, then we can easily obtain

Iα,2f1, f2xdμx 0 see3for the notationI∗1

α,2.

More generally, we have the following theorem.

Theorem 1.3. Letm∈N,μbe defined as above, andμ ∞,bj ∈ RBMORd,j 1,2, . . . , m, 0< α < mn. Then

b, Iα,m

fLqμC

m

j1

bjfj

Lqjμ, 1.7

where1/q1/q11/q2· · ·1/qmα/mn >0and1< qj <,j 1,2, . . . , m.

Clearly,5, Theorem 1is the special case of ourTheorem 1.3form 1. Throughout this paper, we always use the letterCto denote a positive constant that may vary at each occurrence but is independent of the essential variable.

2. Proofs of theorems

We only proveTheorem 1.1sinceTheorem 1.3can follow from the same arguments and an analogous version of the followingLemma 2.5, which can be deduced by induction onm. Before proving our results, we need to recall some notation and establish some lemmas which play important roles in the proofs.

Letfbe a function inL1locRd, we define the noncentered maximal operator

Mp,βηfx sup Qx

1

μηQ1−βp/n

Q

fy pdμy1/p

, 2.1

and the sharp maximal function

M#,βfx sup Qx

1

μ3/2Q

Q

fymQf dμy sup RQx Q,Rdoubling

mQfmRf KQ,Rβ ,

2.2

where the supremum is taken over all cubes Q with sides parallel to the coordinate axes,

mQfis the mean value offon the cubeQ. Whenβ0, we denoteMp,0ηfbyMp,ηfand M#,0fbyM#f.

We also consider the noncentered doubling maximal operatorN, defined by

Nfx sup Qx Qdoubling

1

μQ

Q

(4)

Lemma 2.1see11. Let1≤p <and1< ρ <. Thenb∈RBMOμ, if and only if for any cubeQ⊂Rd,

1

μρQ

Q

bxmQb pdμxCbp

, 2.4

and for any doubling cubesQR,

mQbmRb CKQ,Rb. 2.5 Lemma 2.2see5. LetfL1

locμwith

fdμ0ifμ<∞.For1< p <, ifinf1,Nf∈ Lpμ, then for0β < nwe have

NfLpμCM#,βf

Lpμ. 2.6

Lemma 2.3see5. Letp < r < n/αand1/q1/rα/n. Then Mα

p,ηfLqμCfLrμ, 2.7

whereη >1and0≤α < n/p.

Lemma 2.4. Supposeμis a Radon measure satisfying1.1. Letm∈Nand1/s1/r1· · ·1/rm

α/n >0with0< α < mn,1≤rj ≤ ∞. Then,

aif eachrj>1,

Iα,m

f1, . . . , fmLsμC

m

j1 fj

Lrjμ; 2.8

bifrj1for somej,

Iα,m

f1, . . . , fmLs,μC m

j1 fj

Lrjμ. 2.9

Proof. The proof follows the idea that, for the classical setting, can be found in4. For the sake of completeness, we will show it again.

Sinceα > 0, someri < ∞. If say, rl1 · · · rm ∞, 1 ≤ l < m, because α/n < 1/r1· · ·1/rll, so thatmnα >m−ln, integration inyl1, . . . , ymreduces matters to the case when allriare finiteandml. Thus, we may assume that allri<∞. Now, observe that if 0< ci,i 1, . . . , m, and 0 < α < mi1ci, we can find 0 < αi < cisuch thatαmi1αi. Apply this observation tocin/ri, and 1/si 1/ri−αi/n. Sincemi11/si1/s, 0< αi/n≤1, 1< si<∞, and

y1 nα1

y2 nα2· · · ym nαmy1, . . . , ym nmα, 2.10 whereαmi1αi. It follows that

Iα,m

f1, . . . , fm

x≤m

i1 Iαi

fi

x. 2.11

(5)

Lemma 2.5. Letb1, b2, Iα,2be as in1.6,0< α <2n,τ >1,b1, b2∈RBMOμ. Then there exists a constantC >0such that for allf1∈Lq,f2∈Lq, andx∈Rd,

M#,αb1, b2, Iα,2

f1, f2

x≤Cb1b2Mτ,3/2

Iα,2

f1, f2

x b1Mτ,3/2

b2, Iα,2

f1, f2

x b2Mτ,3/2b1, Iα,2

f1, f2

x

b1b2Mpα1,9/8f1xMpα2,9/8f2x

,

2.12

M#b

1, Iα,2

f1, f2

x≤Cb1

Mτ,3/2Iα,2

f1, f2

x

Mpα1,9/8f1

xMα

p2,9/8

f2

x,

2.13

M#,αb2, Iα,2

f1, f2

x≤Cb2

Mτ,3/2Iα,2

f1, f2

x

Mpα1,9/8f1

xMα

p2,9/8

f2

x,

2.14

where

b1, Iα,2

f1, f2

x b1xIα,2

f1, f2

x−Iα,2

b1f1, f2

x,

b2, Iα,2

f1, f2

x b2xIα,2

f1, f2

x−Iα,2

f1, b2f2

x. 2.15

Proof. By the definition, to obtain2.12, it suffices to prove that for anyx∈ Rd and a cube

Qx, 1

μ3/2Q

Q

b1, b2, Iα,2 f1, f2

z−hQ dμzCb1b2Mτ,3/2Iα,2

f1, f2

x

b1Mτ,3/2b2, Iα,2

f1, f2

x b2Mτ,3/2b1, Iα,2

f1, f2

x

b1b2Mpα1,9/8f1xMpα2,9/8f2x

, 2.16

and for any cubesQR, whereQis an arbitrary cube andRis doubling,

hQhR CK2

Q,RK

α

Q,Rb1b2Mτ,3/2

Iα,2

f1, f2

x

b1Mτ,3/2b2, Iα,2

f1, f2

x b2Mτ,3/2b1, Iα,2

f1, f2

x

b1b2Mpα1,9/8f1xMpα2,9/8f2x

,

2.17

where

hQ mQ

Iα,2

mQ

b1

b1

f1χRd\4/3Q,

mQ

b2

b2

f2χRd\4/3Q

, hRmR

Iα,2

mR

b1

b1

f1χRd\4/3R,

mR

b2

b2

f2χRd\4/3R

.

(6)

First of all, it is easy to see that

b1, b2, Iα,2 f1, f2

z−hQb1z−mQ

b1

b2z−mQ

b2

Iα,2

f1, f2

z

b1z−mQ

b1

Iα,2

f1,

b2z−b2

f2

z

b2z−mQ

b2

Iα,2

b1z−b2

f1, f2

z Iα,2

b1−mQb1

f1,

b1−mQb1

f2

z−hQ

:Iz IIz IIIz IVz.

2.19

Consequently,

1

μ3/2Q

Q

b1, b2, Iα,2 f1, f2

z−hQ dμzCIIIIIIIV, 2.20

where Iμ3/2Q−1QIzdμz, and II, III, IV are defined in the same way.

In what follows, we estimate I–IV, respectively. For I, by H ¨older’s inequality and

Lemma 2.1, we have

I 1

μ3/2Q

Q

Izdμz

C

1

μ3/2Q

Q

b1zm

Q

b1 τ1dμz 11

×

1

μ3/2Q

Q

b2zmQ

b2 τ2dμz 12

×

1

μ3/2Q

Q

Iα,2

f1, f2 τdμz 1

Cb1b2Mτ,3/2

Iα,2

f1, f2

x,

2.21

whereτ1>1,τ2>1 and 111121. For II, we have

II 1

μ3/2Q

Q

IIzdμz

C

1

μ3/2Q

Q

b1zmQ

b1 sdμz 1/s

× 1 μ3/2Q

Q

b2, Iα,2 f1, f2

z τdμz1

Cb1Mτ,3/2b2, Iα,2

f1, f2

x,

2.22

(7)

Similarly, we have

III≤Cb2Mτ,3/2b2, Iα,2

f1, f2

x. 2.23

It remains to estimate IV. For convenience, we setfj0 fjχ4/3Q,fj fj0fj∞,j 1,2. Then,

IVz ≤ Iα,2

b1−mQ

b1

f10,b2−mQ

b2

f20z Iα,2

b1−mQ

b1

f10,b2−mQ

b2

f2∞

z

Iα,2

b1−mQ

b1

f1,b2−mQ

b2

f20z Iα,2

b1−mQ

b1

f1∞,

b2−mQ

b2

f2∞

z−hQ

IV1z IV2z IV3z IV4z,

2.24

and so we have

1

μ3/2Q

Q

IVz dμz4

j1 1

μ3/2Q

Q

IVjzdμz:

4

j1

IVj. 2.25

To estimate IV1, sets1√p1,s2 √p2, and 1/v1/s11/s2−α/n. It follows from H ¨older’s inequality andLemma 2.4that

IV1≤ μQ

1−1/v

μ3/2QIα,2

b1−mQ

b1

f10,b2−mQ

b2

f20Lvμ

3/2Q−1/vb1−mQ

b1

f0

1Ls1μb2−mQ

b2

f0

2Ls2μ

C

μ3/2Q1/v

4/3Q

f1y1 p1dμy

1 1/p1

×

4/3Q

b1y1mQ b1 p1/

p

1−1dμy

1

p1−1/p1

×

4/3Q

f2y2 p2dμy

2

1/p2

4/3Q

b2y1mQ bi p2/

p

2−1dμy i

p2−1/p2

C 2

i1

1

μ3/2Q1−αpi/2n

4/3Q

fiyi pidμy

i

1/pi

×

1

μ3/2Q

4/3Q

biyimQ bi pi/

p

i−1dμy

i

p

i−1/pi

Cb1b2Mpα1,9/8f1xMpα2,9/8f2x.

(8)

For term IV2, byLemma 2.1, we have

IV2 1

μ3/2Q

Q

IV2zdμz

C 1 μ3/2Q

Q

Rd\4/3Q

4/3Q

× b1

y1

mQ b1 f0 1

y1 b2

y2

mQ

b2

f2y2 zy1, zy2 2nα

y1

dμy2

dμz

C

μ3/2Q

Q

4/3Q

b1ymQ b1

f10y1

y1

×

Rd\4/3Q

b2 y2

mQ

b2

f2y2 zy2 2nα

y2 dμzC 1

μ3/2Q1−αp1/2n

4/3Q

f1

y1 p1

y1 1/p1

×

1

μ3/2Q

4/3Q

b1mQ b1 p

1y

1 1/p1

×μ

3 2Q

α/2n

μQ

k1

2k4/3Q\2k−14/3Q

b2 y2

mQ

b2 f2 y2 2k2nαlQ2nα

y2

Cb1Mpα1,9/8f1x

k1

2−knα/2l

2k3 2Q

nα/2

×

2k4/3Q

b2 y2

mQ

b2

f2

y2

y2

Cb1Mpα1,9/8f1x

k1

2−knα/2l

2k3 2Q

nα/2

×

2k4/3Q

b2 y2

m2k4/3Q

b2

f2

y2

y2

m2k4/3Q

b2

mQ

b2

2k3/2Q

f2 y2

y2

Cb1Mpα1,9/8f1x

×

k1

2−knα/2

1

l2k3/2Qn

2k4/3Q

b2 y2

m2k4/3Q

b2 p

2y

2 1/p2

×

1

l2k3/2Qnαp2/2

2k4/3Q

f2

y2 p2

y2 1/p2

k1

k2−knα/2b2

1

l2k3/2Qnα/2

2k4/3Q

f2 y2

y2

Cb1b2Mpα1,9/8f1xMpα2,9/8f2x,

(9)

where the last inequality follows from the following two facts:

1

l2k3/2Qnα/2

2k4/3Q

f2 y2

y2

μ

2k4/3Q1−1/p2

l2k3/2Qnα/2

2k4/3Q

f2

y2 p2

y2 1/p2

2k14/3Q1−1/p21/p2−α/2n

l2k14/3Qnα/2

1

μ2k14/3Q1−αp2/2n

2k14/3Q

f2

y2 p2

y2 1/p2

CMpα2,9/8f2x,

2.28 andsee11

m

2k4/3Q

bj

mQ

bjCbjKQ,2k4/3QCbjKQ,2k4/3QCkbj, j1,2.

2.29 Similarly,

IV3 ≤Cb1b2Mpα1,9/8f1xMpα2,9/8f2x. 2.30 For term IV4, we have

Iα,2 b1−mQ

b1

f1,b2−mQ

b2

f2∞

z−Iα,2

b1−mQ

b1

f1,b2−mQ

b2

f2∞

y

Rd\4/3Q

Rd\4/3Q

1

zy1, zy2 2nα

1

yy1, yy2 2nα

× 2

i1

bi

yi

mQ

bi

fiyi

y1

dμy2

Rd\4/3Q

Rd\4/3Q

|z−y|

yy1, yy2 2nα1

× 2

i1

bi

yi

mQ

bi

fiyi

y1

dμy2

C 2

i1

Rd\4/3Q

|z−y|1/2 yyi nα/21/2 bi

yi

mQ

bi

fiyi

yi

C 2

i1

k1

2k4/3Q\2k−14/3Q2

k/2 1

l2kQnα/2 bi

yi

mQ

bi fi

yi

yi

C 2

i1

k1 2−k/2

1

l2k3/2Qn

2k4/3Q

bi yi

mQ

bi p

iy

i

1/pi

×

1

l2k3/2Qnαpi/2

2k4/3Q

fi

yi pidμ

yi

(10)

C 2

i1

k1

2−k/2Mpα

i,9/8fix

×

1

l2k3/2Qn

2k4/3Q

bi yi

−m2k4/3Q

bi

m2k4/3Q

bi

−mQ

bi p

iy

i

1/pi

C 2

i1

k1

2−k/2kbiMpαi,9/8fix

Cb1b2Mpα1,9/8f1xMpα2,9/8f2x.

2.31

Taking the mean overyQ, we obtain

Iα,2 b1−mQ

b1f1∞,

b1−mQ

b1

f2∞

z−hQCb1b2Mpα1,9/8f1xMpα2,9/8f2x. 2.32

Thus,

IV4 1

μ3/2Q

Q

IV4zdμz≤Cb1b2Mpα1,9/8f1xMpα2,9/8f2x. 2.33

Combing2.20–2.33, we obtain2.16.

Now we turn to estimate2.17. For any cubes,QRwithxQ, whereQis arbitrary andRis doubling. We denoteNQ,R1 simply byN, write

hQhR mQ Iα,2

b1−mQb1

f1,b2−mQb2

f2∞ −mR

Iα,2

b1−mRb1

f1,b2−mRb2

f2∞ ≤ mR

Iα,2

b1−mQb1

f1χRd\2NQ,

b2−mQb2

f2χRd\2NQ

mQ

Iα,2

b1−mQb1

f1χRd\2NQ,

b2−mQb2

f2χRd\2NQ

mR

Iα,2

b1−mRb1

f1χRd\2NQ,

b2−mRb2

f2χRd\2NQ

mR

Iα,2

b1−mQb1

f1χRd\2NQ,

b2−mQb2

f2χRd\2NQ

mQ

Iα,2

b1−mQb1

f1χ2NQ\4/3Q,

b2−mQb2

f2χRd\4/3Q

mQ

Iα,2

b1−mQb1

f1χRd\2NQ,

b2−mQb2

f2χ2NQ\4/3Q

mR

Iα,2

b1−mRb1

f1χRd\4/3R,

b2−mRb2

f2χ2NQ\4/3R

mR

Iα,2

b1−mRb1

f1χ2NQ\4/3R,b2mRb2f2χRd\2NQ

6

i1 Ai.

2.34

By the similar arguments used in proving2.33, we obtain that

A1 ≤C

KQ,R

2

(11)

To estimateA2, we write

Iα,2

b1−mR

b1

f1χRd\2NQ,

b2−mR

b2

f2χRd\2NQ

z −Iα,2

b1−mQ

b1

f1χRd\2NQ,

b2−mQ

b2

f2χRd\2NQ

z mR b2 −mQ

b2

Iα,2

b1−mR

b1

f1χRd\2NQ, f2χRd\2NQ

z mR b1 −mQ

b1

Iα,2

f1χRd\2NQ,

b2−mR

b2

f2χRd\2NQ

z mR b1 −mQ

b1 mR b2 −mQ

b2

Iα,2

f1χRd\2NQ, f2χRd\2NQ

z.

2.36

Then,

A2≤ mR

b2

mQ

b2

μR1

R

Iα,2

b1−mR

b1

f1χRd\2NQ, f2χRd\2NQ

zdμz mR b1 −mQ

b1

μR1

R

Iα,2

f1χRd\2NQ,b2mRb2f2χRd\2NQzdμz

mR b1 −mQ

b1 mR

b2

mQ

b2

μR1

R

Iα,2

f1χRd\2NQ, f2χRd\2NQ

zdμz

A21A22A23.

2.37

It is obvious that

A23≤CKQ,R2 b1b2Mτ,3/2Iα,2

f1, f2

x. 2.38

In order to estimate termA21, we write

Iα,2

b1−mRb1

f1χRd\2NQ, f2χRd\2NQ

z Iα,2

b1−mRb1

f1, f2

z−Iα,2

b1−mRb1

f1χ2NQχ4/3R, f2χ4/3R

z −Iα,2

b1−mRb1

f1χ4/3R, f2χ2NQχ4/3R

z Iα,2

b1−mRb1

f1χ2NQχ4/3R, f2χ2NQχ4/3Rz

Iα,2

b1−mRb1

f1χRd\4/3R, f2χ2NQz

Iα,2

b1−mRb1

f1χ2NQ, f2χRd\4/3R

z Iα,2

b1−mRb1

f1χ2NQ\4/3R, f2χ2NQ\4/3R

z

7

j1 Bjz.

2.39

ForB1z, we write Iα,2

b1−mRb1

f1, f2

z ≤ Iα,2

b1−b1z

f1, f2

z Iα,2

b1z−mRb1

f1, f2

(12)

By H ¨older’s inequality and the fact thatRis doubling, we have

1

μR

R

Iα,2

b1−mRb1

f1, f2

zdμz≤Cb1Mτ,3/2

Iα,2

f1, f2

x,

1

μR

R

Iα,2

b1−b1z

f1, f2

zdμz≤CMτ,3/2b1, Iα,2

f1, f2

x,

2.41

which imply

mRB1 Cb1

Mτ,3/2

Iα,2

f1, f2

x Mτ,3/2

b1, Iα,2

f1, f2

x. 2.42

ForB2z, sets1√p1,s2p2, and 1/v1/s11/s2−α/n. Using H ¨older’s inequality and

Lemma 2.4, we have

1

μR

R

B2zdμz≤C

μR1−1/v

μR Iα,2

b1−mR

b1

f1χ2NQχ4/3R, f2χ4/3R

Lvμ

3 2R

−1/v

b1mR b1

f1χ2NQχ4/3R

Ls1μf2χ4/3RLs2μ

3 2R

1/v

4/3R

f2y p2dμy

1/p2

4/3R

f1x p1dμy

1/p1

×

4/3R

b1ymR b1 p1/

p

1−1dμy

p1−1/p1

C

1

μ3/2R1−αp1/2n

4/3R

f1y p1dμy

1/p1

×

1

μ3/2R

4/3R

b1ymR b1 p1/

p

1−1dμy

p 1−1/p1

×

1

μ3/2R1−αp2/2n

4/3Q

f2y p2dμy

1/p2

Cb1Mpα1,9/8f1xMpα2,9/8f2x,

2.43

which implies

mRB2 Cb1Mα

p1,9/8f1xM

α

p2,9/8f2x. 2.44 Similarly,

mRB3 Cb1

Mpα1,9/8f1xM

α

p2,9/8f2x,

mRB4 Cb1

Mpα1,9/8f1xM

α

p2,9/8f2x.

(13)

ForB5z, sincez∈R, we have

B5z 2NQ

Rd\4/3Q

b1mR b1

f1 f2

y2 zy1, zy2 2nα

y1

dμy2

2NQ

f2 y2

y2

Rd\4/3Q

b1 y1

mR

b1

f1 zy1 2nα

y1

C l2Rnα/2

2NQ

f2 y2

y2

×∞

k1

2−kn

l2k4/3nα/2

2k4/3R\2k−14/3R

b1 y1

mR

b1

f1

y1

C 1 l2Rnα/2

2NQ

f2 y2

y2

×∞

k1

2−kn

l2k4/3Rnα/2

×

2k4/3R

b1 y1

m2k4/3R

b1

f1

y1

2k4/3R

m2k4/3R

b1

mR

b1

y1 f1

y1

y1

C 1 l2Rnα/2

2NQ

f2 y2

y2

×∞

k1 2−kn

1

l2k4/3Rn

2k4/3R

b1 y1

m2k4/3R

b1 p

1y

1 1/p1

× 1

l2k4/3Rnαp1/2

2k4/3R

f1 p1

dμy1 1/p1

Cb1 1

l2k4/3Rnα/2

2k4/3R

f1 y1

C 1 l2Rnα/2

2NQ

f2 y2

y2

k1

2−knb1

Mpα1,9/8f1x Mp1,9/8f1x

C

N

k1 1

l2Rnα/2

2kQ\2k−1Q

f2 y2

y2b1Mpα1,9/8f1x

1

l2Rnα/2

Q

f2 y2

y2b1Mpα1,9/8f1x

C

N

k0 1

l2Rnα/2

2kQ

f2 y2

(14)

C

N

k0

μ2k1Q1−α/2n l2k1Qnα/2

l2k1Qnα/2 l2Rnα/2

1

μ2k1Q1−α/2n

×

2kQ

f2 y2

y2b1Mpα1,9/8f1x

C

N

k0

μ2k1Q1−α/2n l2k1Qnα/2

1

μ9/82kQ1−α/2n

2kQ

f2 y2

y2b1Mpα1,9/8f1x

CKQ,Rαb1Mpα1,9/8f1xMpα2,9/8f2x.

2.46

Taking the mean onzoverR, we obtain

mRB5 CKα

Q,Rb1∗Mpα1,9/8f1xM

α

p2,9/8f2x. 2.47 Similarly, we have

mRB6 CKα

Q,Rb1∗Mpα1,9/8f1xM

α

p2,9/8f2x,

mRB7 CKα

Q,Rb1∗Mpα1,9/8f1xM

α

p2,9/8f2x.

2.48

Summing up the estimates2.39–2.48, we obtain

A21≤CKQ,RKQ,Rαb1b2Mτ,3/2Iα,2

f1, f2

x

b2Mτ,3/2b1, Iα,2

f1, f2

x b1b2Mp1,9/8f1xMp2,9/8f2x

.

2.49

By the same arguments, we can get

A22≤CKQ,RKQ,Rαb1b2Mτ,3/2

Iα,2

f1, f2

x

b1Mτ,3/2b2, Iα,2

f1, f2

x b1b2Mp1,9/8f1xMp2,9/8f2x

.

2.50

Consequently,

A2≤CKQ,R2 K α

Q,Rb1∗b2Mτ,3/2Iα,2

f1, f2

x

b1Mτ,3/2b2, Iα,2

f1, f2

x b2Mτ,3/2b1, Iα,2

f1, f2

x b1b2Mp1,9/8f1xMp2,9/8f2x

.

2.51

Using the similar arguments to those used in provingB5z, we can conclude that

A3A4A5A6 ≤CK2Q,RK

α

(15)

Therefore, we obtain

hQhR CK2

Q,RK

α

Q,Rb1b2Mτ,3/2

Iα,2

f1, f2

x

b1Mτ,3/2b2, Iα,2

f1, f2

x b2Mτ,3/2b1, Iα,2

f1, f2

x b1b2Mp1,9/8f1xMp2,9/8f2x

,

2.53

which implies2.17.

Finally, we show how to derive 2.12 from 2.16 and 2.17. From 2.16, if Q is doubling andxQ, we have

mQ

b1, b2, Iα,2

f1, f2

hQ ≤ 1

μQ

Q

b1, b2, Iα,2 f1, f2

z−hQ dμz

Cb1b2Mτ,3/2Iα,2

f1, f2

x b1Mτ,3/2b2, Iα,2

f1, f2

x b2Mτ,3/2b1, Iα,2

f1, f2

x b1b2Mp1,9/8f1xMp2,9/8f2x

.

2.54

Also, for any cubeQwithxQ,KQ,QCandK α

Q,QC, by2.16,2.17, and2.54, we have

1

μ3/2Q

Q

b1, b2, Iα,2 f1, f2

z−mQ

b1, b2, Iα,2

f1, f2 dμz

≤ 1

μ3/2Q b1, b2, Iα,2

f1, f2

z−hQ dμz

1

μ3/2Q

Q

mQ

b1, b2, Iα,2

f1, f2

hQ dμz

1

μ3/2Q

Q

hQhQ dμz

Cb1b2Mτ,3/2Iα,2

f1, f2

x b1Mτ,3/2b2, Iα,2

f1, f2

x b2Mτ,3/2b1, Iα,2

f1, f2

x b1b2Mp1,9/8f1xMp2,9/8f2x

.

2.55

On the other hand, for all doubling cubesQRwithxQ, such thatKQ,Rα, where is the constant in5, Lemma 6, by2.17, we have

hQhR CK2

Q,RPαb1b2Mτ,3/2Iα,2

f1, f2

x b1Mτ,3/2b2, Iα,2

f1, f2

x b2Mτ,3/2b1, Iα,2

f1, f2

x b1b2Mp1,9/8f1xMp2,9/8f2x

.

(16)

Hence, by5, Lemma 6, we get

hQhR CKα

Q,Rb1∗b2Mτ,3/2Iα,2

f1, f2

x

b1Mτ,3/2b2, Iα,2

f1, f2

x b2Mτ,3/2

b1, Iα,2

f1, f2

x b1b2Mp1,9/8f1xMp2,9/8f2x

,

2.57

for all doubling cubesQRwithxQ. Invoking2.55yields that

mQ

b1, b2, Iα,2

f1, f2

mR

b1, b2, Iα,2

f1, f2 ≤ mQ

b1, b2, Iα,2

f1, f2

hQ hRmR

b1, b2, Iα,2

f1, f2 hQhR

CKQ,Rαb1b2Mτ,3/2Iα,2

f1, f2

x

b1Mτ,3/2b2, Iα,2

f1, f2

x b2Mτ,3/2b1, Iα,2

f1, f2

x b1b2Mp1,9/8f1xMp2,9/8f2x

.

2.58

From this estimate and the definition of the sharp maximal function, we complete the proof of2.12. Similarly, we can deduce2.13and2.14. The details are omitted.

Now we are in the position to proveTheorem 1.1.

Proof ofTheorem 1.1. By the Lebesgue differentiation theorem, it is easy to see that for any

fL1 locRd,

fx ≤ Nfx, 2.59

forμ− a.e.x∈Rd, see11for details. By Lemmas2.22.5, we have

b1, b2, Iα,2

f1, f2Lq≤N

b1, b2, Iα,2

f1, f2Lq

M#,βb1, b2, Iα,2

f1, f2Lq

Cb1b2Mτ,3/2Iα,2

f1, f2Lq

b1Mτ,3/2b2, Iα,2

f1, f2Lq

b2Mτ,3/2b1, Iα,2

f1, f2Lq

b1b2Mpα1,9/8f1xMpα2,9/8f2Lq

Cb1b2f1Lq1f2Lq2

b1b2, Iα,2

f1, f2Lq

b2b1, Iα,2

f1, f2Lq

(17)

Cb1b2f1Lq1f2Lq2

b1M#

b2, Iα,2

f1, f2Lp1

b2M#

b1, Iα,2

f1, f2Lp2

Cb1b2f1Lq1f2Lq2.

2.60

This provesTheorem 1.1.

Acknowledgments

The authors would like to express their deep thanks to the referees for their valuable remarks and suggestions. Huoxiong Wu was partially supported by the NSF of ChinaG10571122.

References

1 C. P´erez and R. H. Torres, “Sharp maximal function estimates for multilinear singular integrals,” inHarmonic analysis at Mount Holyoke, vol. 320 ofContemporary Mathematics, pp. 323–331, American Mathematical Society, Providence, RI, USA, 2003.

2 C. P´erez and R. Trujillo-Gonz´alez, “Sharp weighted estimates for multilinear commutators,”Journal of the London Mathematical Society, vol. 65, no. 3, pp. 672–692, 2002.

3 L. Grafakos and R. H. Torres, “Multilinear Calder ´on-Zygmund theory,”Advances in Mathematics, vol. 165, no. 1, pp. 124–164, 2002.

4 C. E. Kenig and E. M. Stein, “Multilinear estimates and fractional integration,”Mathematical Research Letters, vol. 6, no. 1, pp. 1–15, 1999.

5 W. Chen and E. Sawyer, “A note on commutators of fractional integrals with RBMOμfunctions,” Illinois Journal of Mathematics, vol. 46, no. 4, pp. 1287–1298, 2002.

6 J. Garc´ıa-Cuerva and J. Mar´ıa-Martell, “Two-weight norm inequalities for maximal operators and fractional integrals on non-homogeneous spaces,”Indiana University Mathematics Journal, vol. 50, no. 3, pp. 1241–1280, 2001.

7 J. Xu, “Boundedness of multilinear singular integrals for non-doubling measures,” Journal of Mathematical Analysis and Applications, vol. 327, no. 1, pp. 471–480, 2007.

8 J. Xu, “Boundedness in Lebesgue spaces for commutators of multilinear singular integrals and RBMO functions with non-doubling measures,”Science in China. Series A, vol. 50, no. 3, pp. 361–376, 2007.

9 G. Hu, Y. Meng, and D. Yang, “Multilinear commutators for fractional integrals in non-homogeneous spaces,”Publicacions Matem`atiques, vol. 48, no. 2, pp. 335–367, 2004.

10 G. Hu, Y. Meng, and D. Yang, “Multilinear commutators of singular integrals with non doubling measures,”Integral Equations and Operator Theory, vol. 51, no. 2, pp. 235–255, 2005.

11 X. Tolsa, “BMO,H1, and Calder ´on-Zygmund operators for non doubling measures,”Mathematische

Annalen, vol. 319, no. 1, pp. 89–149, 2001.

References

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