In this paper, the authors study the boundedness properties of a class of multilinear strongly singular integral operator with generalized kernels on product of weighted Lebesgue spaces and product of variable exponent Lebesgue spaces, respectively. Moreover, the types L∞×⋯×L∞→BMO and BMO×⋯×BMO→BMO endpoint estimates are also obtained.
Citation: Shuhui Yang, Yan Lin. Multilinear strongly singular integral operators with generalized kernels and applications[J]. AIMS Mathematics, 2021, 6(12): 13533-13551. doi: 10.3934/math.2021786
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In this paper, the authors study the boundedness properties of a class of multilinear strongly singular integral operator with generalized kernels on product of weighted Lebesgue spaces and product of variable exponent Lebesgue spaces, respectively. Moreover, the types L∞×⋯×L∞→BMO and BMO×⋯×BMO→BMO endpoint estimates are also obtained.
For the past few years, more and more attention has been paid to the topic of multilinear singular integrals. The multilinear Calderón-Zygmund theory originated in the works of Coifman and Meyer in [1,2,3]. Recently, this topic has been studied extensively by many scholars from different perspectives, see for example [4,5,6,7,8,9,10,11,12,13,14].
Lin in [15] introduced the multilinear strongly singular Calderón-Zygmund operator. The kernel does not need any size condition and is more singular near the diagonal than the standard case. It is defined as follows.
Definition 1.1. Suppose K(y0,y1,…,ym) is a function defined away from the diagonal y0=y1=⋯=ym in (Rn)m+1, where m∈N+. For some ε>0 and 0<α≤1, it satisfies
|K(x,y1,…,ym)−K(x′,y1,…,ym)|≤C|x−x′|ε(|x−y1|+⋯+|x−ym|)mn+ε/α, | (1.1) |
whenever |x−x′|α≤12max1≤j≤m|x−yj|.
T is an m-linear operator with the kernel K given by the integral representation
T(f1,…,fm)(x)=∫Rn⋯∫RnK(x,y1,…,ym)m∏j=1fj(yj)dy1⋯dym, | (1.2) |
where fj∈C∞c(Rn)(j=1,…,m) and x∉∩mj=1suppfj.
For some 1≤r1,…,rm<∞ with 1/r=1/r1+⋯+1/rm, T is bounded from Lr1×⋯×Lrm to Lr,∞, and for some 1≤l1,…,lm<∞ with 1/l=1/l1+⋯+1/lm, T is bounded from Ll1×⋯×Llm to Lq,∞, where 0<l/q≤α. Then T is called an m-linear strongly singular Calderón-Zygmund operator.
Lin in [15], Lin-Lu-Lu in [16] and Lin-Han in [17] established the sharp maximal estimates, the boundedness on product of weighted Lebesgue spaces and product of variable exponent Lebesgue spaces for the multilinear strongly singular Calderón-Zygmund operators, their multilinear commutators and multilinear iterated commutators, respectively. Moreover, the types L∞×⋯×L∞→BMO, BMO×⋯×BMO→BMO and LMO×⋯×LMO→LMO endpoint estimates were obtained. In [18], Spanne introduced the function space LMO, which is a subspace of BMO space, equipped with semi-norm:
[f]LMO=sup0<r<11+|lnr||Br|∫Br|f(x)−fBr|dx+supr≥11|Br|∫Br|f(x)−fBr|dx, |
where Br denotes by the ball in Rn with radius r. Lin and Yan in [19] got the boundedness on the product of generalized Morrey spaces and weighted Morrey spaces for multilinear strongly singular Calderón-Zygmund operators, their multilinear commutators and multilinear iterated commutators, respectively. Other related results of this class of operators can be seen in [20] and so on.
In this paper, we will study a class of more general multilinear strongly singular integral operators T defined by (1.2). And instead of (1.1) the kernel K satisfies a weaker condition: there exist ε>0, 0<α≤1 and p0>1, such that for any k1,⋅⋅⋅,kh∈N+, h∈{1,…,m},
(∫Ii1∫Ii2⋅⋅⋅∫Iih|K(x,y1,…,ym)−K(x′,y1,…,ym)|p0dyi1dyi2⋅⋅⋅dyih)1p0 |
≤C|x−x′|ε−t[n(m−hp0)+εα]h∏i=12−ki[n(mh−1p0)+εhα], | (1.3) |
where Iis={yis:2ks|x−x′|t≤|yis−x′|≤2ks+1|x−x′|t}, s=1,⋯,h, and t=1 when |x−x′|≥1, t=α when |x−x′|<1.
Remark 1.1. It is easy to see that the condition (1.1) implies the condition (1.3) as follows:
(∫Ii1∫Ii2⋅⋅⋅∫Iih|K(x,y1,…,ym)−K(x′,y1,…,ym)|p0dyi1dyi2⋅⋅⋅dyih)1p0≤(∫Ii1∫Ii2⋅⋅⋅∫Iih(C|x−x′|ε(|x′−y1|+⋯+|x′−ym|)mn+ε/α)hp0hdyi1dyi2⋅⋅⋅dyih)1p0≤C|x−x′|ε(∫Ii1(1|x′−yi1|mn+ε/α)p0hdyi1)1p0⋯(∫Iih(1|x′−yih|mn+ε/α)p0hdyih)1p0≤C|x−x′|ε−t[n(m−hp0)+εα]h∏i=12−ki[n(mh−1p0)+εhα]. |
Definition 1.2. Let T be an m-linear operator with kernel K defined by (1.2). T is called an m-linear strongly singular integral operator with generalized kernel if it satisfies the condition (1.3), and for some 1≤r1,…,rm<∞ with 1/r=1/r1+⋯+1/rm, T is bounded from Lr1×⋯×Lrm to Lr,∞, and for some 1≤l1,…,lm<∞ with 1/l=1/l1+⋯+1/lm, T is bounded from Ll1×⋯×Llm to Lq,∞, where 0<l/q≤α.
In order to establish our main results, we need some notations as follows.
Definition 1.3. The Hardy-Littlewood maximal operator M is defined by
Mf(x)=supB∋x1|B|∫B|f(y)|dy. |
Denote by Ms(f)=[M(|f|s)]1/s, where 0<s<∞.
Definition 1.4. The sharp maximal function is defined by
M♯(f)(x)=supB∋x1|B|∫B|f(y)−fB|dy∼supB∋xinfa∈C1|B|∫B|f(y)−a|dx, |
where the supremum is taken over all balls B containing x and fB=1|B|∫B|f(x)|dx.
Denote by M♯s(f)=[M♯(|f|s)]1/s, where 0<s<∞.
Definition 1.5. Suppose w is a non-negative measurable function. It belongs to Muckenhoupt class Ap with 1<p<∞ if
supQ(1|Q|∫Qw(x)dx)(1|Q|∫Qw(x)1−p′dx)p−1<∞, |
where 1/p+1/p′=1.
When p=1, we say that w belongs to A1, if there exists a constant C>0 such that for any cube Q,
1|Q|∫Qw(y)dy≤Cw(x),a.e.x∈Q. |
Denote by A∞=⋃p≥1Ap.
Definition 1.6. For the measurable function p(⋅):Rn→[1,∞), the variable exponent Lebesgue space Lp(⋅)(Rn) is defined by
Lp(⋅)(Rn)={fismeasurable:∫Rn(|f(x)|λ)p(x)dx<∞forsomeconstantλ>0}. |
As well-known that the set Lp(⋅)(Rn) becomes a Banach space with respect to the norm
‖f‖Lp(⋅)(Rn)=inf{λ>0:∫Rn(|f(x)|λ)p(x)dx≤1}. |
Denote by P(Rn) the set of all measurable functions p(⋅):Rn→[1,∞) such that
1<p−:=essinfx∈Rnp(x)andp+:=esssupx∈Rnp(x)<∞. |
Denote by B(Rn) the set of all p(⋅)∈P(Rn) such that the Hardy-Littlewood maximal operator M is bounded on Lp(⋅)(Rn).
This paper will be organized as follows. The boundedness properties of multilinear strongly singular integral operators with generalized kernels on product of weighted Lebesgue spaces and product of variable exponent Lebesgue spaces will be obtained, respectively. Moreover, the types L∞×⋯×L∞→BMO and BMO×⋯×BMO→BMO endpoint estimates are also obtained as main results in Section 2. In Section 3, we will provide some necessary lemmas to prove the main results. Finally, in Section 4 we will give the proof details of the main results.
Theorem 2.1. Suppose T is an m-linear strongly singular integral operator with generalized kernel and p′0≥max{r1,…,rm,l1,…,lm}, 1/p0+1/p′0=1, where p0, rj and lj are given by Definition 1.2, j=1,…,m. For any p′0<p1,…,pm<∞ with 1/p=1/p1+⋯+1/pm, (w1,…,wm)∈(Ap1/p′0,…,Apm/p′0) and w=∏mj=1wp/pjj, there is
‖T(→f)‖Lp(w)≤Cm∏j=1‖fj‖Lpj(wj). |
Theorem 2.2. Suppose T is an m-linear strongly singular integral operator with generalized kernel and p′0≥max{r1,…,rm,l1,…,lm}, 1/p0+1/p′0=1, where p0, rj and lj are given by Definition 1.2, j=1,…,m. Suppose p(⋅),p1(⋅),…,pm(⋅)∈B(Rn) and 1/p(⋅)=1/p1(⋅)+⋯+1/pm(⋅). Let qj0 be given by Lemma 3.5 for pj(⋅), j=1,…,m. If p′0≤min1≤j≤mqj0, then
‖T(→f)‖Lp(⋅)(Rn)≤Cm∏j=1‖fj‖Lpj(⋅)(Rn). |
Theorem 2.3. Suppose T is an m-linear strongly singular integral operator with generalized kernel, p0, q, rj, lj are given by Definition 1.2, j=1,…,m and q>1, p′0≥max{r1,…,rm,l1,…,lm}, 1/p0+1/p′0=1. Then
‖T(→f)‖BMO≤Cm∏j=1‖fj‖∞. |
Theorem 2.4. Suppose T is an m-linear strongly singular integral operator with generalized kernel, p0, q, rj, lj are given by Definition 1.2, j=1,…,m and q>1, p′0≥max{r1,…,rm,l1,…,lm}, 1/p0+1/p′0=1, and T(f1,⋯,fj−1,1,fj+1,⋯,fm)=0(j=1,…,m). Then
‖T(→f)‖BMO≤Cm∏j=1‖fj‖BMO. |
Lemma 3.1. [9,21] Let 0<p<r<∞, then there exists a constant C=Cp,r>0 such that for any measurable function f there has
|Q|−1/p‖f‖Lp(Q)≤C|Q|−1/r‖f‖Lr,∞(Q). |
Lemma 3.2. Let T be an m-linear strongly singular integral operator with generalized kernel and p′0≥max{r1,…,rm,l1,…,lm}, 1/p0+1/p′0=1, where p0, rj and lj are given by Definition 1.2, j=1,…,m. If 0<δ<1/m, then
M♯δ(T(→f))(x)≤Cm∏j=1Mp′0(fj)(x), |
for all m-tuples →f=(f1,…,fm) of bounded measurable functions with compact support.
Proof of Lemma 3.2. Let us just consider the case m=2 in order to simplify the proof. In fact, a similar procedure can be applied to all other situations.
Let f1,f2 be bounded measurable functions with compact support. Then for any ball B=B(x0,rB) containing x with rB>0, we will take into account two cases, respectively.
Case 1: rB≥14.
Write
f1=f1χ32B+f1χ(32B)c:=f11+f21,f2=f2χ32B+f2χ(32B)c:=f12+f22. |
Choose a z0∈6B∖5B and take a c0=T(f21,f12)(z0)+T(f11,f22)(z0)+T(f21,f22)(z0), then
(1|B|∫B||T(f1,f2)(z)|δ−|c0|δ|dz)1/δ≤(1|B|∫B|T(f1,f2)(z)−c0|δdz)1/δ≤C(1|B|∫B|T(f11,f12)(z)|δdz)1/δ+C(1|B|∫B|T(f21,f12)(z)−T(f21,f12)(z0)|δdz)1/δ+C(1|B|∫B|T(f11,f22)(z)−T(f11,f22)(z0)|δdz)1/δ+C(1|B|∫B|T(f21,f22)(z)−T(f21,f22)(z0)|δdz)1/δ:=4∑j=1Ij. |
Notice that 0<δ<r<∞, where r is given as in Definition 1.2. By Lemma 3.1 and the boundedness of T from Lr1×Lr2 to Lr,∞, we have
I1≤C|B|−1/δ‖T(f11,f12)‖Lδ(B)≤C|B|−1/r‖T(f11,f12)‖Lr,∞(B)≤C(1|32B|∫32B|f1(y1)|r1dy1)1r1(1|32B|∫32B|f2(y2)|r2dy2)1r2≤CMr1(f1)(x)Mr2(f2)(x)≤CMp′0(f1)(x)Mp′0(f2)(x). |
For z∈B and y1∈(32B)c, there are 2|z−z0|≤|y1−z0|, 4rB≤|z−z0|≤7rB and |z−z0|≥1. By Hölder's inequality and the condition (1.3) of the kernel, we have
I2≤C1|B|∫B|T(f21,f12)(z)−T(f21,f12)(z0)|dz≤C1|B|∫B∞∑k=1∫2k|z−z0|≤|y1−z0|≤2k+1|z−z0|∫32B|K(z,y1,y2)−K(z0,y1,y2)||f1(y1)||f2(y2)|dy2dy1dz≤C1|B|∫B∞∑k=1(∫32B(∫2k|z−z0|≤|y1−z0|≤2k+1|z−z0||K(z,y1,y2)−K(z0,y1,y2)|p0dy1)1p0×(∫2k|z−z0|≤|y1−z0|≤2k+1|z−z0||f1(y1)|p′0dy1)1p′0|f2(y2)|dy2)dz≤C1|B|∫B∞∑k=1|B|2−k(n(2−1p0)+εα)|z−z0|ε−(n(2−1p0)+εα)(2k+1|z−z0|)np′0dzMp′0(f1)(x)M(f2)(x)≤C∞∑k=12−k(n+εα)∫B|z−z0|−n−εα+εdzMp′0(f1)(x)Mp′0(f2)(x)≤C∞∑k=12−k(n+εα)rε−εαBMp′0(f1)(x)Mp′0(f2)(x)≤CMp′0(f1)(x)Mp′0(f2)(x). |
Similarly we can also get that
I3≤CMp′0(f1)(x)Mp′0(f2)(x). |
For z∈B and y1,y2∈(32B)c, there are 2|z−z0|≤|y1−z0|, 2|z−z0|≤|y2−z0|, 4rB≤|z−z0|≤7rB and |z−z0|≥1. By Hölder's inequality and the condition (1.3) of the kernel, we have
I4≤C1|B|∫B|T(f21,f22)(z)−T(f21,f22)(z0)|dz≤C1|B|∫B∞∑k1=1∞∑k2=1∫2k1|z−z0|≤|y1−z0|≤2k1+1|z−z0|∫2k2|z−z0|≤|y2−z0|≤2k2+1|z−z0||K(z,y1,y2)−K(z0,y1,y2)|×|f1(y1)||f2(y2)|dy2dy1dz≤C1|B|∫B∞∑k1=1∞∑k2=1(∫2k1|z−z0|≤|y1−z0|≤2k1+1|z−z0|∫2k2|z−z0|≤|y2−z0|≤2k2+1|z−z0||K(z,y1,y2)−K(z0,y1,y2)|p0dy2dy1)1p0(∫2k1|z−z0|≤|y1−z0|≤2k1+1|z−z0||f1(y1)|p′0dy1)1p′0(∫2k2|z−z0|≤|y2−z0|≤2k2+1|z−z0||f2(y2)|p′0dy2)1p′0dz≤C1|B|∫B∞∑k1=1∞∑k2=12∏i=12−ki(n(1−1p0)+ε2α)|z−z0|ε−(n(2−2p0)+εα)2∏i=1(2ki+1|z−z0|)np′0dzMp′0(f1)(x)×Mp′0(f2)(x)≤C1|B|∞∑k1=1∞∑k2=12∏i=12−kiε2α∫B|z−z0|ε−εαdzMp′0(f1)(x)Mp′0(f2)(x)≤C∞∑k1=1∞∑k2=12∏i=12−kiε2αrε−εαBMp′0(f1)(x)Mp′0(f2)(x)≤CMp′0(f1)(x)Mp′0(f2)(x). |
Case 2: 0<rB<14.
Denote by ˜B=B(x0,rαB). Write
f1=f1χ16˜B+f1χ(16˜B)c:=˜f11+˜f21,f2=f2χ16˜B+f2χ(16˜B)c:=˜f12+˜f22. |
Choose a ˜z0∈3B∖2B and take a ˜c0=T(˜f21,˜f12)(˜z0)+T(˜f11,˜f22)(˜z0)+T(˜f21,˜f22)(˜z0), then
(1|B|∫B||T(f1,f2)(z)|δ−|˜c0|δ|dz)1/δ≤C(1|B|∫B|T(˜f11,˜f12)(z)|δdz)1/δ+C(1|B|∫B|T(˜f21,˜f12)(z)−T(˜f21,˜f12)(~z0)|δdz)1/δ+C(1|B|∫B|T(˜f11,˜f22)(z)−T(˜f11,˜f22)(˜z0)|δdz)1/δ+C(1|B|∫B|T(˜f21,˜f22)(z)−T(˜f21,˜f22)(˜z0)|δdz)1/δ:=4∑j=1˜Ij. |
Notice that 0<δ<q<∞ and 0<l/q≤α, where l and q are given as in Definition 1.2. By Lemma 3.1, we have
˜I1≤C|B|−1/δ‖T(˜f11,˜f12)‖Lδ(B)≤C|B|−1/q‖T(˜f11,˜f12)‖Lq,∞(B)≤C|B|−1/q|˜B|1/l(1|16˜B|∫16˜B|f1(y1)|l1dy1)1l1(1|16˜B|∫16˜B|f2(y2)|l2dy2)1l2≤Crn(αl−1q)BMl1(f1)(x)Ml2(f2)(x)≤CMp′0(f1)(x)Mp′0(f2)(x). |
For z∈B and y1∈(16˜B)c, there are |z−˜z0|α≤(4rB)α≤12|y1−˜z0|, rB≤|z−˜z0|≤4rB and |z−˜z0|<1. By Hölder's inequality and the condition (1.3) of the kernel, we have
˜I2≤C1|B|∫B|T(˜f21,˜f12)(z)−T(˜f21,˜f12)(˜z0)|dz≤C1|B|∫B∞∑k=1∫2k|z−˜z0|α≤|y1−˜z0|≤2k+1|z−˜z0|α∫16˜B|K(z,y1,y2)−K(˜z0,y1,y2)||f1(y1)||f2(y2)|dy2dy1dz≤C1|B|∫B∞∑k=1∫16˜B(∫2k|z−˜z0|α≤|y1−˜z0|≤2k+1|z−˜z0|α|K(z,y1,y2)−K(˜z0,y1,y2)|p0dy1)1p0×(∫2k|z−˜z0|α≤|y1−˜z0|≤2k+1|z−˜z0|α|f1(y1)|p′0dy1)1p′0|f2(y2)|dy2dz≤C1|B|∫B∞∑k=1|˜B|2−k(n(2−1p0)+εα)|z−˜z0|ε−α(n(2−1p0)+εα)(2k+1|z−˜z0|α)np′0dzMp′0(f1)(x)M(f2)(x)≤C1|B|∞∑k=1|˜B|2−k(n+εα)∫B|z−˜z0|−αndzMp′0(f1)(x)Mp′0(f2)(x)≤CMp′0(f1)(x)Mp′0(f2)(x). |
Similarly we can also get that
˜I3≤CMp′0(f1)(x)Mp′0(f2)(x). |
For z∈B and y1,y2∈(16˜B)c, there are 2|z−˜z0|α≤|y1−˜z0|, 2|z−˜z0|α≤|y2−˜z0|, rB≤|z−˜z0|≤4rB and |z−˜z0|<1. By Hölder's inequality and the condition (1.3) of the kernel, we have
˜I4≤C1|B|∫B|T(˜f21,˜f22)(z)−T(˜f21,˜f22)(˜z0)|dz≤C1|B|∫B∞∑k1=1∞∑k2=1(∫2k1|z−˜z0|α≤|y1−˜z0|≤2k1+1|z−˜z0|α∫2k2|z−˜z0|α≤|y2−˜z0|≤2k2+1|z−˜z0|α|K(z,y1,y2)−K(˜z0,y1,y2)|p0dy2dy1)1p0(∫2k1|z−˜z0|α≤|y1−˜z0|≤2k1+1|z−˜z0|α|f1(y1)|p′0dy1)1p′0×(∫2k2|z−˜z0|α≤|y2−˜z0|≤2k2+1|z−˜z0|α|f2(y2)|p′0dy2)1p′0dz≤C1|B|∫B∞∑k1=1∞∑k2=12∏i=12−ki(n(1−1p0)+ε2α)|z−˜z0|ε−α(n(2−2p0)+εα)2∏i=1(2ki+1|z−˜z0|α)np′0dz×Mp′0(f1)(x)Mp′0(f2)(x)≤C∞∑k1=1∞∑k2=12∏i=12−kiε2αMp′0(f1)(x)Mp′0(f2)(x)≤CMp′0(f1)(x)Mp′0(f2)(x). |
Thus, according to the estimates in both cases, there is
M♯δ(T(f1,f2))(x)∼supB∋xinfa∈C(1|B|∫B||T(f1,f2)(z)|δ−a|dz)1/δ≤CMp′0(f1)(x)Mp′0(f2)(x), |
which completes the proof of the lemma.
Lemma 3.3. [9] Let 0<p,δ<∞ and w∈A∞. Then there exists a constant C>0 depending only on the A∞ constant of w such that
∫Rn[Mδ(f)(x)]pw(x)dx≤C∫Rn[M♯δ(f)(x)]pw(x)dx, |
for every function f such that the left-hand side is finite.
Lemma 3.4. [22] For (w1,…,wm)∈(Ap1,…,Apm) with 1≤p1,…,pm<∞, and for 0<θ1,…,θm<1 such that θ1+⋯+θm=1, we have wθ11⋯wθmm∈Amax{p1,…,pm}.
Lemma 3.5. [23] Let p(⋅)∈P(Rn). Then Mq0 is bounded on Lp(⋅)(Rn) for some 1<q0<∞ if and only if M is bounded on Lp(⋅)(Rn).
Lemma 3.6. [24] Given a family F of ordered pairs of measurable functions, suppose for some fixed 0<~p0<∞, every (f,g)∈F and every w∈A1,
∫Rn|f(x)|~p0w(x)dx≤C0∫Rn|g(x)|~p0w(x)dx. |
Let p(⋅)∈P(Rn) with ~p0≤p−. If (p(⋅)~p0)′∈B(Rn), then there exists a constant C>0 such that for all (f,g)∈F, ‖f‖Lp(⋅)(Rn)≤C‖g‖Lp(⋅)(Rn).
Lemma 3.7. [25] Let p(⋅),p1(⋅),…,pm(⋅)∈P(Rn) with 1/p(x)=1/p1(x)+⋯+1/pm(x). Then for any fj∈Lpj(⋅)(Rn), j=1,…,m, there has
‖m∏j=1fj‖Lp(⋅)(Rn)≤2m−1m∏j=1‖fj‖Lpj(⋅)(Rn). |
Lemma 3.8. [23] Let p(⋅)∈P(Rn). Then the following conditions are equivalent.
(i) p(⋅)∈B(Rn).
(ii) p′(⋅)∈B(Rn).
(iii) p(⋅)~p0∈B(Rn) for some 1<~p0<p−.
(iv) (p(⋅)~p0)′∈B(Rn) for some 1<~p0<p−.
Lemma 3.9. [24] If p(⋅)∈P(Rn), then C∞c(Rn) is dense in Lp(⋅)(Rn).
Lemma 3.10. [26] Let f be a function in BMO. Suppose 1≤p<∞, x∈Rn, and r1,r2>0. Then
(1|B(x,r1)|∫B(x,r1)|f(y)−fB(x,r2)|pdy)1/p≤C(1+|lnr1r2|)‖f‖BMO, |
where C>0 is independent of f, x, r1 and r2.
Proof of Theorem 2.1. From the fact that wj∈Apj/p′0 and pj>p′0 (j=1,…,m), it follows that the Hardy-Littlewood maximal operator M is bounded on Lpj/p′0(wj). By Lemma 3.4, we obtain w∈Amax{p1/p′0,…,pm/p′0}⊂A∞.
Take a δ such that 0<δ<1/m, then by Lemma 3.2 and Lemma 3.3, we have
‖T(→f)‖Lp(w)≤‖Mδ(T(→f))‖Lp(w)≤C‖M♯δ(T(→f))‖Lp(w)≤C‖m∏j=1Mp′0(fj)‖Lp(w)≤Cm∏j=1‖Mp′0(fj)‖Lpj(wj)=Cm∏j=1‖M(|fj|p′0)‖1/p′0Lpj/p′0(wj)≤Cm∏j=1‖|fj|p′0‖1/p′0Lpj/p′0(wj)=Cm∏j=1‖fj‖Lpj(wj). |
This completes the proof of the theorem.
Proof of Theorem 2.2. Since p(⋅)∈B(Rn), then by Lemma 3.8, there exists a ~p0 such that 1<~p0<p− and (p(⋅)~p0)′∈B(Rn). Take a δ such that 0<δ<1/m. For any w∈A1, by Lemma 3.2 and Lemma 3.3, we can get that
∫Rn|T(→f)(x)|~p0w(x)dx≤∫Rn[Mδ(T(→f))(x)]~p0w(x)dx≤C∫Rn[M♯δ(T(→f))(x)]~p0w(x)dx≤C∫Rn[m∏j=1Mp′0(fj)(x)]~p0w(x)dx≤C∫Rn[m∏j=1Mqj0(fj)(x)]~p0w(x)dx |
holds for all m-tuples →f=(f1,…,fm) of bounded measurable functions with compact support.
By Lemma 3.9, we can get that C^{\infty}_{c}(\mathbb{R}^{n}) is dense in L^{p_j(\cdot)}(\mathbb{R}^{n})(j = 1, 2, \cdots, m) . For f_j\in C^{\infty}_{c}(\mathbb{R}^{n}) , applying Lemma 3.6 to the pair \bigl(T(\vec{f}), \prod_{j = 1}^{m}M_{q_{0}^{j}}(f_{j})\bigr) , we have
\|T(\vec{f})\|_{L^{p(\cdot)}(\mathbb{R}^{n})}\leq C\biggl\|\prod\limits_{j = 1}^{m}M_{q_{0}^{j}}(f_{j})\biggr\|_{L^{p(\cdot)}(\mathbb{R}^{n})}. |
Then by Lemma 3.5 and Lemma 3.7, we have
\|T(\vec{f})\|_{L^{p(\cdot)}(\mathbb{R}^{n})}\leq C\prod\limits_{j = 1}^{m}\|M_{q_{0}^{j}}(f_{j})\|_{L^{p_{j}(\cdot)}(\mathbb{R}^{n})} \leq C\prod\limits_{j = 1}^{m}\|f_{j}\|_{L^{p_{j}(\cdot)}(\mathbb{R}^{n})}. |
Since the denseness of C^{\infty}_{c}(\mathbb{R}^{n}) in L^{p_j(\cdot)}(\mathbb{R}^{n})(j = 1, 2, \cdots, m) , this completes the proof of the theorem.
Proof of Theorem 2.3 . To simplify the proof, we only give the proof when m = 2 since their similarities.
Let f_1, f_2\in L^{\infty} , then for any ball B = B(x_{0}, r_{B}) with r_{B} > 0 , we will think about two cases, respectively.
Case 1: r_{B}\geq \frac{1}{4} .
Write
f_{1} = f_{1}\chi_{32B}+f_{1}\chi_{(32B)^{c}}: = f_{1}^{1}+f_{1}^{2}, \quad f_{2} = f_{2}\chi_{32B}+f_{2}\chi_{(32B)^{c}}: = f_{2}^{1}+f_{2}^{2}. |
Choose a z_{0} \in 6B\setminus5B and take a c_{0} = T(f_{1}^{2}, f_{2}^{1})(z_{0})+T(f_{1}^{1}, f_{2}^{2})(z_{0})+T(f_{1}^{2}, f_{2}^{2})(z_{0}) , then
\begin{eqnarray*} &&\dfrac{1}{|B|}\int_{B}|T(f_{1}, f_{2})(x)-c_{0}|dx\\ &&\leq \dfrac{1}{|B|}\int_{B}|T(f_{1}^{1}, f_{2}^{1})(x)|dx+\dfrac{1}{|B|}\int_{B}|T(f_{1}^{2}, f_{2}^{1})(x)-T(f_{1}^{2}, f_{2}^{1})(z_{0})|dx\\ &&\quad+\dfrac{1}{|B|}\int_{B}|T(f_{1}^{1}, f_{2}^{2})(x)-T(f_{1}^{1}, f_{2}^{2})(z_{0})|dx+\dfrac{1}{|B|}\int_{B}|T(f_{1}^{2}, f_{2}^{2})(x)-T(f_{1}^{2}, f_{2}^{2})(z_{0})|dx\\ &&: = \sum\limits_{j = 1}^{4}J_{j}. \end{eqnarray*} |
Take p_{1}, \dots, p_{m} such that \max\{p_0', m\} < p_{1}, \dots, p_{m} < \infty . Let 1/p = 1/p_{1}+\cdots+1/p_{m} , then 1 < p < \infty . By Theorem 2.1, we obtain that T is bounded from L^{p_{1}}\times \cdots \times L^{p_{m}} into L^{p} .
By Hölder's inequality and the L^{p_{1}}\times L^{p_{2}}\rightarrow L^{p} boundedness of T , we have
\begin{eqnarray*} J_{1} &\leq& \biggl(\dfrac{1}{|B|}\int_{B}|T(f_{1}^{1}, f_{2}^{1})(x)|^{p}dx\biggr)^{\frac{1}{p}}\\ &\leq& C|B|^{-1/p}\|f_{1}^{1}\|_{L^{p_{1}}}\|f_{2}^{1}\|_{L^{p_{2}}}\\ &\leq& C\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}. \end{eqnarray*} |
For x\in B and y_{1}\in (32B)^{c} , there are 2|x-z_{0}|\leq |y_{1}-z_{0}| , 4r_{B}\leq |x-z_{0}|\leq 7r_{B} and |x-z_{0}|\geq1 . By Hölder's inequality and the condition (1.3) of the kernel, we have
\begin{eqnarray*} J_{2} &\leq& \dfrac{1}{|B|}\int_{B} \int_{(32B)^{c}}\int_{32B} |K(x, y_{1}, y_{2})-K(z_{0}, y_{1}, y_{2})||f_{1}(y_{1})||f_{2}(y_{2})|dy_{2}dy_{1}dx\\ &\leq &\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}\dfrac{1}{|B|}\int_{B} \sum^{\infty}_{k = 1}\int_{2^k|x-z_{0}|\leq|y_{1}-z_{0}|\leq2^{k+1}|x-z_{0}|}\int_{32B} |K(x, y_{1}, y_{2})-K(z_{0}, y_{1}, y_{2})|dy_{2}dy_{1}dx\\ &\leq &\dfrac{1}{|B|}\int_{B} \sum^{\infty}_{k = 1}\int_{32B}\Big(\int_{2^k|x-z_{0}|\leq|y_{1}-z_{0}|\leq2^{k+1}|x-z_{0}|} |K(x, y_{1}, y_{2})-K(z_{0}, y_{1}, y_{2})|^{p_0}dy_{1}\Big)^{\frac{1}{p_0}}\\ &&\times(2^{k+1}|x-z_{0}|)^{\frac{n}{p_0'}}dy_{2}dx\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}\\ &\leq &C\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}\dfrac{1}{|B|}\int_{B} \sum^{\infty}_{k = 1}|B| 2^{-k(n(2-{\frac{1}{p_0}})+\frac{\varepsilon}{\alpha})}|x-z_{0}|^{\varepsilon-(n(2-{\frac{1}{p_0}})+\frac{\varepsilon}{\alpha})}(2^{k+1}|x-z_{0}|)^{\frac{n}{p_0'}}dx \\ &\leq &C r_B^{-\frac{\varepsilon}{\alpha}+\varepsilon}\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}\\ &\leq &C\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}. \end{eqnarray*} |
Similarly we can also get that
J_{3}\leq C\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}. |
For x\in B and y_{1}, y_{2}\in (32B)^{c} , there are 2|x-z_{0}|\leq |y_{1}-z_{0}| , 2|x-z_{0}|\leq |y_{2}-z_{0}| , 4r_{B}\leq |x-z_{0}|\leq 7r_{B} and |x-z_{0}|\geq1 . By Hölder's inequality and the condition (1.3) of the kernel, we have
\begin{eqnarray*} J_{4} &\leq& \dfrac{1}{|B|}\int_{B} \int_{(32B)^{c}}\int_{(32B)^{c}} |K(x, y_{1}, y_{2})-K(z_{0}, y_{1}, y_{2})||f_{1}(y_{1})||f_{2}(y_{2})|dy_{2}dy_{1}dx\\ &\leq &\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}\dfrac{1}{|B|}\int_{B} \sum^{\infty}_{k_1 = 1} \sum^{\infty}_{k_2 = 1}\Big(\int_{2^{k_1}|x-z_{0}|\leq|y_{1}-z_{0}|\leq2^{{k_1}+1}|x-z_{0}|}\int_{2^{k_2}|x-z_{0}|\leq|y_{2}-z_{0}|\leq2^{{k_2}+1}|x-z_{0}|}\\ && |K(x, y_{1}, y_{2})-K(z_{0}, y_{1}, y_{2})|^{p_0}dy_{2}dy_{1}\Big)^{\frac{1}{p_0}}\prod^{2}_{i = 1}(2^{k_i+1}|x-z_{0}|)^{\frac{n}{p_0}}dx\\ &\leq&C\dfrac{1}{|B|}\int_{B}\sum^{\infty}_{k_1 = 1}\sum^{\infty}_{k_2 = 1} \prod^{2}_{i = 1}2^{-k_{i}(n(1-{\frac{1}{p_0}})+\frac{\varepsilon}{2\alpha})}|x-z_{0}|^{\varepsilon-(n(2-{\frac{2}{p_0}})+\frac{\varepsilon}{\alpha})}\prod^{2}_{i = 1}(2^{k_i+1}|x-z_{0}|)^{\frac{n}{p_0}} dx\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}\\ &\leq&C\sum^{\infty}_{k_1 = 1}\sum^{\infty}_{k_2 = 1}\prod^{2}_{i = 1} 2^\frac{-k_i\varepsilon}{2\alpha}\dfrac{1}{|B|}\int_{B}|x-z_{0}|^{\varepsilon-\frac{\varepsilon}{\alpha}}dx\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}\\ &\leq& C\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}. \end{eqnarray*} |
Case 2: 0 < r_{B} < \frac{1}{4} .
Denote by \tilde{B} = B(x_{0}, r_{B}^{\alpha}) . Write
f_{1} = f_{1}\chi_{16\tilde{B}}+f_{1}\chi_{(16\tilde{B})^{c}}: = \tilde{f}_{1}^{1}+\tilde{f}_{1}^{2}, \quad f_{2} = f_{2}\chi_{16\tilde{B}}+f_{2}\chi_{(16\tilde{B})^{c}}: = \tilde{f}_{2}^{1}+\tilde{f}_{2}^{2}. |
Choose a \tilde{z}_{0} \in 3B\setminus2B and take a \tilde{c}_{0} = T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{1})(\tilde{z}_{0})+T(\tilde{f}_{1}^{1}, \tilde{f}_{2}^{2})(\tilde{z}_{0}) +T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{2})(\tilde{z}_{0}) , then
\begin{eqnarray*} &&\dfrac{1}{|B|}\int_{B}|T(f_{1}, f_{2})(x)-\tilde{c}_{0}|dx\\ &&\leq \dfrac{1}{|B|}\int_{B}|T(\tilde{f}_{1}^{1}, \tilde{f}_{2}^{1})(x)|dx +\dfrac{1}{|B|}\int_{B}|T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{1})(x)-T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{1})(\tilde{z}_{0})|dx\\ &&\quad+\dfrac{1}{|B|}\int_{B}|T(\tilde{f}_{1}^{1}, \tilde{f}_{2}^{2})(x)-T(\tilde{f}_{1}^{1}, \tilde{f}_{2}^{2})(\tilde{z}_{0})|dx +\dfrac{1}{|B|}\int_{B}|T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{2})(x)-T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{2})(\tilde{z}_{0})|dx\\ &&: = \sum\limits_{j = 1}^{4}\tilde{J}_{j}. \end{eqnarray*} |
Notice that 1 < q < \infty and 0 < l/q\leq \alpha , where l is given as in Definition 1.2. By Lemma 3.1, we have
\begin{eqnarray*} \tilde{J}_{1}&\leq& C|B|^{-1}\|T(\tilde{f}_{1}^{1}, \tilde{f}_{2}^{1})\|_{L^{1}(B)}\\ &\leq& C|B|^{-1/q}\|T(\tilde{f}_{1}^{1}, \tilde{f}_{2}^{1})\|_{L^{q, \infty}(B)}\\ &\leq& C|B|^{-1/q}\|\tilde{f}_{1}^{1}\|_{L^{l_{1}}}\|\tilde{f}_{2}^{1}\|_{L^{l_{2}}}\\ &\leq& C\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}r_{B}^{n({\frac{\alpha}{l}}-{\frac{1}{q}})}\\ &\leq& C\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}. \end{eqnarray*} |
For x\in B and y_{1}\in (16\tilde{B})^{c} , there are 2|x-\tilde{z}_{0}|^{\alpha}\leq |y_{1}-\tilde{z}_{0}| , r_{B}\leq |x-\tilde{z}_{0}|\leq 4r_{B} and |x-\tilde{z}_{0}| < 1 . By Hölder's inequality and the condition (1.3) of the kernel, we have
\begin{eqnarray*} \tilde{J}_{2} &\leq &\dfrac{1}{|B|}\int_{B} \int_{(16\tilde{B})^{c}}\int_{16\tilde{B}} |K(x, y_{1}, y_{2})-K(\tilde{z}_{0}, y_{1}, y_{2})|f_{1}(y_{1})||f_{2}(y_{2})|dy_{2}dy_{1}dx\\ &\leq &\dfrac{1}{|B|}\int_{B} \sum^{\infty}_{k = 1}\int_{16\tilde{B}}\Big(\int_{2^k|x-\tilde{z}_{0}|^\alpha\leq|y_{1}-\tilde{z}_{0}|\leq2^{k+1}|x-\tilde{z}_{0}|^\alpha} |K(x, y_{1}, y_{2})-K(x_{0}, y_{1}, y_{2})|^{p_0}dy_{1}\Big)^{\frac{1}{p_0}}\\ &&\times(2^{k+1}|x-\tilde{z}_{0}|^\alpha)^{\frac{n}{p_0'}} dy_{2}dx\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}\\ &\leq &C\dfrac{1}{|B|}\int_{B} \sum^{\infty}_{k = 1}|\tilde{B}| 2^{-k(n(2-{\frac{1}{p_0}})+\frac{\varepsilon}{\alpha})}|x-\tilde{z}_{0}|^{\varepsilon-{\alpha}(n(2-{\frac{1}{p_0}})+\frac{\varepsilon}{\alpha})}(2^{k+1}|x-\tilde{z}_{0}|^\alpha)^{\frac{n}{p_0'}}dx\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}\\ &\leq &C \sum^{\infty}_{k = 1}|\tilde{B}|2^{-k(n+\frac{\varepsilon}{\alpha})}\dfrac{1}{|B|}\int_{B}|x-\tilde{z}_{0}|^{-{\alpha}n}dx\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}\\ &\leq&C\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}. \end{eqnarray*} |
Similarly we can also get that
\tilde{J}_{3}\leq C\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}. |
For x\in B and y_{1}, y_{2}\in (16\tilde{B})^{c} , there are |x-\tilde{z}_{0}|^{\alpha}\leq\frac{1}{2}|y_{1}-\tilde{z}_{0}| , |x-\tilde{z}_{0}|^{\alpha}\leq\frac{1}{2}|y_{2}-\tilde{z}_{0}| , r_{B}\leq |x-\tilde{z}_{0}|\leq 4r_{B} and |x-\tilde{z}_{0}| < 1 . By Hölder's inequality and the condition (1.3) of the kernel, we have
\begin{eqnarray*} \tilde{J}_{4} &\leq &\dfrac{1}{|B|}\int_{B} \int_{(16\tilde{B})^{c}}\int_{(16\tilde{B})^{c}} |K(x, y_{1}, y_{2})-K(\tilde{z}_{0}, y_{1}, y_{2})||f_{1}(y_{1})||f_{2}(y_{2})|dy_{2}dy_{1}dx\\ &\leq &\dfrac{1}{|B|}\int_{B} \sum^{\infty}_{k_1 = 1} \sum^{\infty}_{k_2 = 1}\Big(\int_{2^{k_1}|x-\tilde{z}_{0}|^\alpha\leq|y_{1}-\tilde{z}_{0}|\leq2^{k_1+1}|x-\tilde{z}_{0}|^\alpha}\int_{2^{k_2}|x-\tilde{z}_{0}|^\alpha\leq|y_{2}-\tilde{z}_{0}|\leq2^{k_2+1}|x-\tilde{z}_{0}|^\alpha}\\ &&|K(x, y_{1}, y_{2})-K(\tilde{z}_{0}, y_{1}, y_{2})|^{p_0}dy_{2}dy_{1}\Big)^{\frac{1}{p_0}} \prod^{2}_{i = 1}(2^{k_i+1}|x-\tilde{z}_{0}|^\alpha)^{\frac{n}{p_0'}}dx\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}\\ &\leq&C\dfrac{1}{|B|}\int_{B}\sum^{\infty}_{k_1 = 1}\sum^{\infty}_{k_2 = 1} \prod^{2}_{i = 1}2^{-k_{i}(n(1-{\frac{1}{p_0}})+\frac{\varepsilon}{2\alpha}))}|x-\tilde{z}_{0}|^{\varepsilon-\alpha(n(2-{\frac{2}{p_0}})+\frac{\varepsilon}{\alpha})}\prod^{2}_{i = 1}(2^{k_i+1}|x-\tilde{z}_{0}|^\alpha)^{\frac{n}{p_0'}}dx \|f_{1}\|_{\infty}\|f_{2}\|_{\infty}\\ &\leq&C\sum^{\infty}_{k_1 = 1}\sum^{\infty}_{k_2 = 1}\prod^{2}_{i = 1} 2^\frac{-k_i\varepsilon}{2\alpha}\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}\\ &\leq& C\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}. \end{eqnarray*} |
Thus, according to the estimates in both cases, there is
\|T(f_{1}, f_{2})\|_{BMO}\sim \sup\limits_{B} \inf\limits_{a\in \mathbb{C}}\dfrac{1}{|B|}\int_{B}|T(f_{1}, f_{2})(x)-a|dx \leq C\|f_{1}\|_{\infty}\|f_{2}\|_{\infty}, |
which completes the proof of the theorem.
Proof of Theorem 2.4 . We only give the proof when m = 2 .
Let f_1, f_2\in BMO , then for any ball B = B(x_{0}, r_{B}) with r_{B} > 0 , we will consider two cases, respectively.
Case 1: r_{B}\geq \frac{1}{4} .
Write
f_{1} = (f_{1})_{32B}+(f_{1}-(f_{1})_{32B})\chi_{32B}+(f_{1}-(f_{1})_{32B})\chi_{(32B)^{c}}: = f_{1}^{1}+f_{1}^{2}+f_{1}^{3}, |
f_{2} = (f_{2})_{32B}+(f_{2}-(f_{2})_{32B})\chi_{32B}+(f_{2}-(f_{2})_{32B})\chi_{(32B)^{c}}: = f_{2}^{1}+f_{2}^{2}+f_{2}^{3}. |
It follows from the hypothesis of the theorem that
T(f_{1}, f_{2}) = T(f_{1}^{2}, f_{2}^{2})+T(f_{1}^{2}, f_{2}^{3})+T(f_{1}^{3}, f_{2}^{2})+T(f_{1}^{3}, f_{2}^{3}). |
Choose a z_{0} \in 6B\setminus5B and take a d_{0} = T(f_{1}^{2}, f_{2}^{3})(z_{0})+T(f_{1}^{3}, f_{2}^{2})(z_{0})+T(f_{1}^{3}, f_{2}^{3})(z_{0}) , then
\begin{eqnarray*} &&\dfrac{1}{|B|}\int_{B}|T(f_{1}, f_{2})(x)-d_{0}|dx\\ &&\leq \dfrac{1}{|B|}\int_{B}|T(f_{1}^{2}, f_{2}^{2})(x)|dx+\dfrac{1}{|B|}\int_{B}|T(f_{1}^{2}, f_{2}^{3})(x)-T(f_{1}^{2}, f_{2}^{3})(z_{0})|dx\\ &&\quad+\dfrac{1}{|B|}\int_{B}|T(f_{1}^{3}, f_{2}^{2})(x)-T(f_{1}^{3}, f_{2}^{2})(z_{0})|dx +\dfrac{1}{|B|}\int_{B}|T(f_{1}^{3}, f_{2}^{3})(x)-T(f_{1}^{3}, f_{2}^{3})(z_{0})|dx\\ &&: = \sum\limits_{j = 1}^{4}L_{j}. \end{eqnarray*} |
Take p_{1}, \dots, p_{m} such that \max\{p_0', m\} < p_{1}, \dots, p_{m} < \infty . Let 1/p = 1/p_{1}+\cdots+1/p_{m} , then 1 < p < \infty . By Theorem 2.1, we obtain the boundedness of T from L^{p_{1}}\times \cdots \times L^{p_{m}} into L^{p} . By Hölder's inequality, we have
\begin{eqnarray*} L_{1} &\leq& \biggl(\dfrac{1}{|B|}\int_{B}|T(f_{1}^{2}, f_{2}^{2})(x)|^{p}dx\biggr)^{\frac{1}{p}}\\ &\leq& C\biggl(\dfrac{1}{|32B|}\int_{32B}|f_{1}(y_{1})-(f_{1})_{32B}|^{p_{1}}dy_{1}\biggr)^{\frac{1}{p_{1}}} \biggl(\dfrac{1}{|32B|}\int_{32B}|f_{2}(y_{2})-(f_{2})_{32B}|^{p_{2}}dy_{2}\biggr)^{\frac{1}{p_{2}}}\\ &\leq& C\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}. \end{eqnarray*} |
For x\in B and y_{2}\in (32B)^{c} , there are 2|x-z_{0}|\leq |y_{2}-z_{0}| , 4r_{B}\leq |x-z_{0}|\leq 7r_{B} and |x-z_{0}|\geq1 . By Hölder's inequality, Lemma 3.10 and the condition (1.3) of the kernel, we have
\begin{eqnarray*} L_{2} &\leq& \dfrac{1}{|B|}\int_{B} \int_{(32B)^{c}}\int_{32B} |K(x, y_{1}, y_{2})-K(z_{0}, y_{1}, y_{2})||f_{1}(y_{1})-(f_{1})_{32B}||f_{2}(y_{2})-(f_{2})_{32B}|dy_{1}dy_{2}dx\\ &\leq & \dfrac{1}{|B|}\int_{B} \sum^{\infty}_{k = 1}\int_{32B}\Big(\int_{2^k|x-z_{0}|\leq|y_{2}-z_{0}|\leq2^{k+1}|x-z_{0}|} |K(x, y_{1}, y_{2})-K(z_{0}, y_{1}, y_{2})|^{p_0}dy_{2}\Big)^{\frac{1}{p_0}}\\ &&\times\Big(\int_{2^k|x-z_{0}|\leq|y_{2}-z_{0}|\leq2^{k+1}|x-z_{0}|}|f_{2}(y_{2})-(f_{2})_{32B}|^{p_0'}dy_{2}\Big)^{\frac{1}{p_0'}} |f_{1}(y_{1})-(f_{1})_{32B}|dy_{1}dx\\ &\leq &C\dfrac{1}{|B|}\int_{B} \sum^{\infty}_{k = 1}|B| 2^{-k(n(2-{\frac{1}{p_0}})+\frac{\varepsilon}{\alpha})}|x-z_{0}|^{\varepsilon-(n(2-{\frac{1}{p_0}})+\frac{\varepsilon}{\alpha})}dx \Big(\int_{2^{k+5}B}|f_{2}(y_{2})-(f_{2})_{32B}|^{p_0'}dy_{2}\Big)^{\frac{1}{p_0'}}\|f_{1}\|_{BMO} \\ &\leq &C r_B^{\frac{n}{p_0'}}\sum^{\infty}_{k = 1}2^{-k(n+\frac{\varepsilon}{\alpha})}\Big(1+\ln\dfrac{2^{k+5}r_B}{32r_B}\Big)\int_{B}|x-z_{0}|^{-2n-\frac{\varepsilon}{\alpha}+\varepsilon+{\frac{n}{p_0}}}dx \|f_{1}\|_{BMO}\|f_{2}\|_{BMO}\\ &\leq &C\sum^{\infty}_{k = 1}k2^{-k(n+\frac{\varepsilon}{\alpha})} r_B^{-\frac{\varepsilon}{\alpha}+\varepsilon}\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}\\ &\leq& C\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}. \end{eqnarray*} |
Similarly we also can get that
L_{3}\leq C\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}. |
For x\in B and y_{1}, y_{2}\in (32B)^{c} , there are 2|x-z_{0}|\leq |y_{1}-z_{0}| , 2|x-z_{0}|\leq |y_{2}-z_{0}| , 4r_{B}\leq |x-z_{0}|\leq 7r_{B} and |x-z_{0}|\geq1 . By Hölder's inequality, Lemma 3.10 and the condition (1.3) of the kernel, we have
\begin{eqnarray*} L_{4} &\leq& \dfrac{1}{|B|}\int_{B} \int_{(32B)^{c}}\int_{(32B)^{c}} |K(x, y_{1}, y_{2})-K(z_{0}, y_{1}, y_{2})||f_{1}(y_{1})-(f_{1})_{32B}|\\ &&\times|f_{2}(y_{2})-(f_{2})_{32B}|dy_{2}dy_{1}dx\\ &\leq &\dfrac{1}{|B|}\int_{B} \sum^{\infty}_{k_1 = 1} \sum^{\infty}_{k_2 = 1}\Big(\int_{2^{k_1}|x-z_{0}|\leq|y_{1}-z_{0}|\leq2^{{k_1}+1}|x-z_{0}|}\int_{2^{k_2}|x-z_{0}|\leq|y_{2}-z_{0}|\leq2^{{k_2}+1}|x-z_{0}|}\\ &&|K(x, y_{1}, y_{2})-K(z_{0}, y_{1}, y_{2})|^{p_0}dy_{2}dy_{1}\Big)^{\frac{1}{p_0}}\Big(\int_{2^{k_1+5}B}|f_{1}(y_{1})-(f_{1})_{32B}|^{p_0'}dy_{1}\Big)^{\frac{1}{p_0'}}\\ &&\times\Big(\int_{2^{k_2+5}B}|f_{2}(y_{2})-(f_{2})_{32B}|^{p_0'}dy_{2}\Big)^{\frac{1}{p_0'}}dx\\ &\leq&C\dfrac{1}{|B|}\int_{B}\sum^{\infty}_{k_1 = 1}\sum^{\infty}_{k_2 = 1} \prod^{2}_{i = 1}2^{-k_{i}(n(1-{\frac{1}{p_0}})+\frac{\varepsilon}{2\alpha})}|x-z_{0}|^{\varepsilon-(n(2-{\frac{2}{p_0}})+\frac{\varepsilon}{\alpha})}\prod^{2}_{i = 1}\Big((2^{k_i+5}r_B)^{\frac{n}{p_0'}}\\ &&\times\Big(1+\ln\dfrac{2^{k_i+5}r_B}{32r_B}\Big)\Big)dx\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}\\ &\leq&C\sum^{\infty}_{k_1 = 1}\sum^{\infty}_{k_2 = 1} \prod^{2}_{i = 1}k_{i}2^{\frac{-k_{i}\varepsilon}{2\alpha}}r_B^{-\frac{\varepsilon}{\alpha}+\varepsilon}\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}\\ &\leq& C\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}. \end{eqnarray*} |
Case 2: 0 < r_{B} < \frac{1}{4} .
Denote by \tilde{B} = B(x_{0}, r_{B}^{\alpha}) . Write
f_{1} = (f_{1})_{16\tilde{B}}+(f_{1}-(f_{1})_{16\tilde{B}})\chi_{16\tilde{B}}+(f_{1}-(f_{1})_{16\tilde{B}})\chi_{(16\tilde{B})^{c}} : = \tilde{f}_{1}^{1}+\tilde{f}_{1}^{2}+\tilde{f}_{1}^{3}, |
f_{2} = (f_{2})_{16\tilde{B}}+(f_{2}-(f_{2})_{16\tilde{B}})\chi_{16\tilde{B}}+(f_{2}-(f_{2})_{16\tilde{B}})\chi_{(16\tilde{B})^{c}} : = \tilde{f}_{2}^{1}+\tilde{f}_{2}^{2}+\tilde{f}_{2}^{3}. |
It follows from the hypothesis of the theorem that
T(f_{1}, f_{2}) = T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{2})+T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{3})+T(\tilde{f}_{1}^{3}, \tilde{f}_{2}^{2}) +T(\tilde{f}_{1}^{3}, \tilde{f}_{2}^{3}). |
Choose a \tilde{z}_{0} \in 3B\setminus2B and take a \tilde{d}_{0} = T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{3})(\tilde{z}_{0})+T(\tilde{f}_{1}^{3}, \tilde{f}_{2}^{2})(\tilde{z}_{0}) +T(\tilde{f}_{1}^{3}, \tilde{f}_{2}^{3})(\tilde{z}_{0}) , then
\begin{eqnarray*} &&\dfrac{1}{|B|}\int_{B}|T(f_{1}, f_{2})(x)-\tilde{d}_{0}|dx\\ &&\leq \dfrac{1}{|B|}\int_{B}|T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{2})(x)|dx +\dfrac{1}{|B|}\int_{B}|T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{3})(x)-T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{3})(\tilde{z}_{0} )|dx\\ &&\quad+\dfrac{1}{|B|}\int_{B}|T(\tilde{f}_{1}^{3}, \tilde{f}_{2}^{2})(x)-T(\tilde{f}_{1}^{3}, \tilde{f}_{2}^{2})(\tilde{z}_{0} )|dx +\dfrac{1}{|B|}\int_{B}|T(\tilde{f}_{1}^{3}, \tilde{f}_{2}^{3})(x)-T(\tilde{f}_{1}^{3}, \tilde{f}_{2}^{3})(\tilde{z}_{0} )|dx\\ &&: = \sum\limits_{j = 1}^{4}\tilde{L}_{j}. \end{eqnarray*} |
Notice that 1 < q < \infty and 0 < l/q\leq \alpha , where l is given as in Definition 1.2. By Lemma 3.1, we have
\begin{eqnarray*} \tilde{L}_{1}&\leq& |B|^{-1}\|T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{2})\|_{L^{1}(B)}\\ &\leq& C|B|^{-1/q}\|T(\tilde{f}_{1}^{2}, \tilde{f}_{2}^{2})\|_{L^{q, \infty}(B)}\\ &\leq& C|B|^{-1/q}|\tilde{B}|^{1/l}\biggl(\dfrac{1}{|16\tilde{B}|}\int_{16\tilde{B}}|f_{1}(y_{1})-(f_{1})_{16\tilde{B}}|^{l_{1}}dy_{1}\biggr)^{\frac{1}{l_{1}}}\biggl(\dfrac{1}{|16\tilde{B}|}\int_{16\tilde{B}}|f_{2}(y_{2})-(f_{2})_{16\tilde{B}}|^{l_{2}}dy_{2}\biggr)^{\frac{1}{l_{2}}}\\ &\leq& C r_{B}^{n({\frac{\alpha}{l}}-{\frac{1}{q}})}\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}\\ &\leq& C\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}. \end{eqnarray*} |
For x\in B and y_{2}\in (16\tilde{B})^{c} , there is 2|x-\tilde{z}_{0}|^{\alpha}\leq|y_{2}-\tilde{z}_{0}| , r_{B}\leq |x-\tilde{z}_{0}|\leq 4r_{B} and |x-\tilde{z}_{0}| < 1 . By Hölder's inequality, Lemma 3.10 and the condition (1.3) of the kernel, we have
\begin{eqnarray*} \tilde{L}_{2} &\leq &\dfrac{1}{|B|}\int_{B} \sum^{\infty}_{k = 1}\int_{16\tilde{B}}\Big(\int_{2^k|x-\tilde{z}_{0}|^\alpha\leq|y_{2}-\tilde{z}_{0}|\leq2^{k+1}|x-\tilde{z}_{0}|^\alpha} |K(x, y_{1}, y_{2})-K(\tilde{z}_{0}, y_{1}, y_{2})|^{p_0}dy_{2}\Big)^{\frac{1}{p_0}}\\ &&\times\Big(\int_{2^{k+4}\tilde{B}}|f_{2}(y_{2})-(f_{2})_{16\tilde{B}}|^{p_0'}dy_{2}\Big)^{\frac{1}{p_0'}}|f_{1}(y_{1})-(f_{1})_{16\tilde{B}}|dy_{1}dx\\&\leq &C\dfrac{1}{|B|}\int_{B} \sum^{\infty}_{k = 1}|\tilde{B}| 2^{-k(n(2-{\frac{1}{p_0}})+\frac{\varepsilon}{\alpha})}|x-\tilde{z}_{0}|^{\varepsilon-{\alpha}(n(2-{\frac{1}{p_0}})+\frac{\varepsilon}{\alpha})}dx(2^{k+4}r_B^\alpha)^{\frac{n}{p_0'}}\Big(1+\ln\dfrac{2^{k+4}r_B^\alpha}{16r_B^\alpha}\Big)\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}\\ &\leq &C\sum^{\infty}_{k = 1}k2^{-k(n+\frac{\varepsilon}{\alpha})}\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}\\ &\leq& C\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}. \end{eqnarray*} |
Similarly we can also get that
\tilde{L}_{3}\leq C\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}. |
For x\in B and y_{1}, y_{2}\in (16\tilde{B})^{c} , there are 2|x-\tilde{z}_{0}|^{\alpha}\leq|y_{1}-\tilde{z}_{0}| , 2|x-\tilde{z}_{0}|^{\alpha}\leq|y_{2}-\tilde{z}_{0}| , r_{B}\leq |x-\tilde{z}_{0}|\leq 4r_{B} and |x-\tilde{z}_{0}| < 1 . By Hölder's inequality, Lemma 3.10 and the condition (1.3) of the kernel, we have
\begin{eqnarray*} \tilde{L}_{4} &\leq &\dfrac{1}{|B|}\int_{B} \sum^{\infty}_{k_1 = 1} \sum^{\infty}_{k_2 = 1}\Big(\int_{2^{k_1}|x-\tilde{z}_{0}|^\alpha\leq|y_{1}-\tilde{z}_{0}|\leq2^{k_1+1}|x-\tilde{z}_{0}|^\alpha}\int_{2^{k_2}|x-\tilde{z}_{0}|^\alpha\leq|y_{2}-\tilde{z}_{0}|\leq2^{k_2+1}|x-\tilde{z}_{0}|^\alpha}\\ &&|K(x, y_{1}, y_{2})-K(\tilde{z}_{0}, y_{1}, y_{2})|^{p_0}dy_{2}dy_{1}\Big)^{\frac{1}{p_0}}\Big(\int_{2^{k+4}\tilde{B}}|f_{1}(y_{1})-(f_{1})_{16\tilde{B}}|^{p_0'}dy_{1}\Big)^{\frac{1}{p_0'}}\\ &&\times\Big(\int_{2^{k+4}\tilde{B}}|f_{2}(y_{2})-(f_{2})_{16\tilde{B}}|^{p_0'}dy_{2}\Big)^{\frac{1}{p_0'}}dx\\ &\leq&C\dfrac{1}{|B|}\int_{B}\sum^{\infty}_{k_1 = 1}\sum^{\infty}_{k_2 = 1} \prod^{2}_{i = 1}2^{-k_{i}(n(1-{\frac{1}{p_0}})+\frac{\varepsilon}{2\alpha})}|x-\tilde{z}_{0}|^{\varepsilon-\alpha(n(2-{\frac{2}{p_0}})+\frac{\varepsilon}{\alpha})}dx\prod^{2}_{i = 1}\Big((2^{k_i+4}r_B^\alpha)^{\frac{n}{p_0}}(1+\ln\dfrac{2^{k_i+4}r_B^\alpha}{16r_B^\alpha})\Big)\\ &&\times\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}\\ &\leq&C\sum^{\infty}_{k_1 = 1}\sum^{\infty}_{k_2 = 1}\prod^{2}_{i = 1} k_i2^\frac{-k_i\varepsilon}{2\alpha}\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}\\ &\leq& C\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}. \end{eqnarray*} |
Thus, according to the estimates in both cases, there is
\|T(f_{1}, f_{2})\|_{BMO}\sim \sup\limits_{B} \inf\limits_{a\in \mathbb{C}}\dfrac{1}{|B|}\int_{B}|T(f_{1}, f_{2})(x)-a|dx\leq C\|f_{1}\|_{BMO}\|f_{2}\|_{BMO}, |
which completes the proof of the theorem.
Compared with the multilinear strongly singular Calderón-Zygmund operator in [15], the kernel function of the multilinear strongly singular integral operator with generalized kernel in the present article satisfies the weaker smoothness condition. Our results further generalize the corresponding results in [15].
We thank the referees for their time and comments. This work was supported by the National Natural Science Foundation of China (No. 12071052).
The authors declare that there is no conflict of interests regarding the publication of this article.
[1] |
R. R. Coifman, Y. Meyer, On commutators of singular integrals and bilinear singular integrals, T. Am. Math. Soc., 212 (1975), 315–331. doi: 10.1090/S0002-9947-1975-0380244-8
![]() |
[2] | R. R. Coifman, Y. Meyer, Au delà des Opérateurs pseudo-différentiels, Astèrisque, 57 (1978), 1–199. |
[3] |
R. R. Coifman, Y. Meyer, Commutateurs d'intégrales singulières et opérateurs multilinaires, Ann. Ins. Fourier (Grenoble), 28 (1978), 177–202. doi: 10.5802/aif.708
![]() |
[4] |
T. A. Bui, X. T. Duong, Weighted norm inequalities for multilinear operators and applications to multilinear Fourier multipliers, Bull. Sci. Math., 137 (2013), 63–75. doi: 10.1016/j.bulsci.2012.04.001
![]() |
[5] |
L. Grafakos, R. Torres, Multilinear Calderón-Zygmund theory, Adv. Math., 165 (2002), 124–164. doi: 10.1006/aima.2001.2028
![]() |
[6] |
L. Grafakos, R. Torres, Maximal operator and weighted norm inequalities for multilinear singular integrals, Indiana Univ. Math. J., 51 (2002), 1261–1276. doi: 10.1512/iumj.2002.51.2114
![]() |
[7] |
J. Hart, Bilinear square functions and vector-valued Calderón-Zygmund operators, J. Fourier Anal. Appl., 18 (2012), 1291–1313. doi: 10.1007/s00041-012-9238-1
![]() |
[8] |
J. Hart, A new proof of the bilinear T(1) theorem, Proc. Am. Math. Soc., 142 (2014), 3169–3181. doi: 10.1090/S0002-9939-2014-12054-5
![]() |
[9] |
A. K. Lerner, S. Ombrosi, C. Pérez, R. H. Torres, R. Trujillo-González, New maximal functions and multiple weights for the multilinear Calderón-Zygmund theory, Adv. Math., 220 (2009), 1222–1264. doi: 10.1016/j.aim.2008.10.014
![]() |
[10] |
K. Li, W. Sun, Weak and strong type weighted estimates for multilinear Calderón-Zygmund operators, Adv. Math., 254 (2014), 736–771. doi: 10.1016/j.aim.2013.12.027
![]() |
[11] |
D. Maldonado, V. Naibo, Weighted norm inequalities for paraproducts and bilinear pseudodifferential operators with mild regularity, J. Fourier Anal. Appl., 15 (2009), 218–261. doi: 10.1007/s00041-008-9029-x
![]() |
[12] |
K. Moen, Weighted inequalities for multilinear fractional integral operators, Collect. Math., 60 (2009), 213–238. doi: 10.1007/BF03191210
![]() |
[13] |
C. Pérez, R. H. Torres, Sharp maximal function estimates for multilinear singular integrals, Contemp. Math., 320 (2003), 323–331. doi: 10.1090/conm/320/05615
![]() |
[14] |
C. Pérez, R. H. Torres, Minimal regularity conditions for the end-point estimate of bilinear Calderón-Zygmund operators, Proc. Am. Math. Soc. Ser. B, 1 (2014), 1–13. doi: 10.1090/S2330-1511-2014-00009-2
![]() |
[15] |
Y. Lin, Multilinear theory of strongly singular Calderón-Zygmund operators and applications, Nonlinear Anal., 192 (2020), 111699. doi: 10.1016/j.na.2019.111699
![]() |
[16] |
Y. Lin, G. Z. Lu, S. Z. Lu, Sharp maximal estimates for multilinear commutators of multilinear strongly singular Calderón-Zygmund operators and applications, Forum Math., 31 (2019), 1–18. doi: 10.1515/forum-2018-0008
![]() |
[17] | Y. Lin, Y. Y. Han, Sharp maximal and weighted estimates for multilinear iterated commutators of multilinear strongly singular Calderón-Zygmund operators, Chinese J. Contemp. Math., 40 (2019), 399–416. |
[18] | S. Spanne, Some function spaces defined using the mean oscillation over cubes, Ann. Sc. Norm. Super. Pisa., 19 (1965), 593–608. |
[19] | Y. Lin, H. H. Yan, Multilinear strongly singular Calderón-Zygmund operators and commutators on Morrey type spaces, Jordan J. Math. Stat., 14 (2021), 351–375. |
[20] | Á. Bényi, L. Chaffee, V. Naibo, Strongly singular bilinear Calderón-Zygmund operators and a class of bilinear pseudodifferential operators, J. Math. Soc. Jpn., 71 (2019), 569–587. |
[21] | J. Garcia-Cuerva, J. L. Rubio de Francia, Weighted norm inequalities and related topics, North-Holland Math Studies, Vol. 116, Amsterdam: North-Holland Publishing Co., 1985. |
[22] |
L. Grafakos, J. M. Martell, Extrapolation of weighted norm inequalities for multivariable operators and applications, J. Geom. Anal., 14 (2004), 19–46. doi: 10.1007/BF02921864
![]() |
[23] |
L. Diening, Maximal function on Musielak-Orlicz spaces and generlaized Lebesgue spaces, Bull. Sci. Math., 129 (2005), 657–700. doi: 10.1016/j.bulsci.2003.10.003
![]() |
[24] | L. Diening, P. Harjulehto, P. Hästö, M. R{\rm{\dot u}}žička, Lebesgue and sobolev spaces with variable exponents, In: Lecture notes in mathematics, Berlin: Springer, 2011. |
[25] |
G. Z. Lu, P. Zhang, Multilinear Calderón-Zygmund operator with kernels of Dini's type and applications, Nonlinear Anal., 107 (2014), 92–117. doi: 10.1016/j.na.2014.05.005
![]() |
[26] | Y. Lin, S. Z. Lu, Strongly singular Calderón-Zygmund operators and their commutators, Jordan J. Math. Stat., 1 (2008), 31–49. |
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