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Research article

Multilinear strongly singular integral operators with generalized kernels and applications

  • Received: 12 March 2021 Accepted: 17 September 2021 Published: 23 September 2021
  • MSC : 42B25, 42B35

  • 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××LBMO and BMO××BMOBMO 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××LBMO and BMO××BMOBMO 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 mN+. For some ε>0 and 0<α1, it satisfies

    |K(x,y1,,ym)K(x,y1,,ym)|C|xx|ε(|xy1|++|xym|)mn+ε/α, (1.1)

    whenever |xx|α12max1jm|xyj|.

    T is an m-linear operator with the kernel K given by the integral representation

    T(f1,,fm)(x)=RnRnK(x,y1,,ym)mj=1fj(yj)dy1dym, (1.2)

    where fjCc(Rn)(j=1,,m) and xmj=1suppfj.

    For some 1r1,,rm< with 1/r=1/r1++1/rm, T is bounded from Lr1××Lrm to Lr,, and for some 1l1,,lm< with 1/l=1/l1++1/lm, T is bounded from Ll1××Llm to Lq,, where 0<l/qα. 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××LBMO, BMO××BMOBMO and LMO××LMOLMO 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+supr11|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<α1 and p0>1, such that for any k1,,khN+, h{1,,m},

    (Ii1Ii2Iih|K(x,y1,,ym)K(x,y1,,ym)|p0dyi1dyi2dyih)1p0
    C|xx|εt[n(mhp0)+εα]hi=12ki[n(mh1p0)+εhα], (1.3)

    where Iis={yis:2ks|xx|t|yisx|2ks+1|xx|t}, s=1,,h, and t=1 when |xx|1, t=α when |xx|<1.

    Remark 1.1. It is easy to see that the condition (1.1) implies the condition (1.3) as follows:

    (Ii1Ii2Iih|K(x,y1,,ym)K(x,y1,,ym)|p0dyi1dyi2dyih)1p0(Ii1Ii2Iih(C|xx|ε(|xy1|++|xym|)mn+ε/α)hp0hdyi1dyi2dyih)1p0C|xx|ε(Ii1(1|xyi1|mn+ε/α)p0hdyi1)1p0(Iih(1|xyih|mn+ε/α)p0hdyih)1p0C|xx|εt[n(mhp0)+εα]hi=12ki[n(mh1p0)+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 1r1,,rm< with 1/r=1/r1++1/rm, T is bounded from Lr1××Lrm to Lr,, and for some 1l1,,lm< with 1/l=1/l1++1/lm, T is bounded from Ll1××Llm to Lq,, where 0<l/qα.

    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)=supBx1|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)=supBx1|B|B|f(y)fB|dysupBxinfaC1|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 Ms(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)1pdx)p1<,

    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)dyCw(x),a.e.xQ.

    Denote by A=p1Ap.

    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

    fLp()(Rn)=inf{λ>0:Rn(|f(x)|λ)p(x)dx1}.

    Denote by P(Rn) the set of all measurable functions p():Rn[1,) such that

    1<p:=essinfxRnp(x)andp+:=esssupxRnp(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××LBMO and BMO××BMOBMO 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 p0max{r1,,rm,l1,,lm}, 1/p0+1/p0=1, where p0, rj and lj are given by Definition 1.2, j=1,,m. For any p0<p1,,pm< with 1/p=1/p1++1/pm, (w1,,wm)(Ap1/p0,,Apm/p0) and w=mj=1wp/pjj, there is

    T(f)Lp(w)Cmj=1fjLpj(wj).

    Theorem 2.2. Suppose T is an m-linear strongly singular integral operator with generalized kernel and p0max{r1,,rm,l1,,lm}, 1/p0+1/p0=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 p0min1jmqj0, then

    T(f)Lp()(Rn)Cmj=1fjLpj()(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, p0max{r1,,rm,l1,,lm}, 1/p0+1/p0=1. Then

    T(f)BMOCmj=1fj.

    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, p0max{r1,,rm,l1,,lm}, 1/p0+1/p0=1, and T(f1,,fj1,1,fj+1,,fm)=0(j=1,,m). Then

    T(f)BMOCmj=1fjBMO.

    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/pfLp(Q)C|Q|1/rfLr,(Q).

    Lemma 3.2. Let T be an m-linear strongly singular integral operator with generalized kernel and p0max{r1,,rm,l1,,lm}, 1/p0+1/p0=1, where p0, rj and lj are given by Definition 1.2, j=1,,m. If 0<δ<1/m, then

    Mδ(T(f))(x)Cmj=1Mp0(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: rB14.

    Write

    f1=f1χ32B+f1χ(32B)c:=f11+f21,f2=f2χ32B+f2χ(32B)c:=f12+f22.

    Choose a z06B5B 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/δC(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:=4j=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

    I1C|B|1/δT(f11,f12)Lδ(B)C|B|1/rT(f11,f12)Lr,(B)C(1|32B|32B|f1(y1)|r1dy1)1r1(1|32B|32B|f2(y2)|r2dy2)1r2CMr1(f1)(x)Mr2(f2)(x)CMp0(f1)(x)Mp0(f2)(x).

    For zB and y1(32B)c, there are 2|zz0||y1z0|, 4rB|zz0|7rB and |zz0|1. By Hölder's inequality and the condition (1.3) of the kernel, we have

    I2C1|B|B|T(f21,f12)(z)T(f21,f12)(z0)|dzC1|B|Bk=12k|zz0||y1z0|2k+1|zz0|32B|K(z,y1,y2)K(z0,y1,y2)||f1(y1)||f2(y2)|dy2dy1dzC1|B|Bk=1(32B(2k|zz0||y1z0|2k+1|zz0||K(z,y1,y2)K(z0,y1,y2)|p0dy1)1p0×(2k|zz0||y1z0|2k+1|zz0||f1(y1)|p0dy1)1p0|f2(y2)|dy2)dzC1|B|Bk=1|B|2k(n(21p0)+εα)|zz0|ε(n(21p0)+εα)(2k+1|zz0|)np0dzMp0(f1)(x)M(f2)(x)Ck=12k(n+εα)B|zz0|nεα+εdzMp0(f1)(x)Mp0(f2)(x)Ck=12k(n+εα)rεεαBMp0(f1)(x)Mp0(f2)(x)CMp0(f1)(x)Mp0(f2)(x).

    Similarly we can also get that

    I3CMp0(f1)(x)Mp0(f2)(x).

    For zB and y1,y2(32B)c, there are 2|zz0||y1z0|, 2|zz0||y2z0|, 4rB|zz0|7rB and |zz0|1. By Hölder's inequality and the condition (1.3) of the kernel, we have

    I4C1|B|B|T(f21,f22)(z)T(f21,f22)(z0)|dzC1|B|Bk1=1k2=12k1|zz0||y1z0|2k1+1|zz0|2k2|zz0||y2z0|2k2+1|zz0||K(z,y1,y2)K(z0,y1,y2)|×|f1(y1)||f2(y2)|dy2dy1dzC1|B|Bk1=1k2=1(2k1|zz0||y1z0|2k1+1|zz0|2k2|zz0||y2z0|2k2+1|zz0||K(z,y1,y2)K(z0,y1,y2)|p0dy2dy1)1p0(2k1|zz0||y1z0|2k1+1|zz0||f1(y1)|p0dy1)1p0(2k2|zz0||y2z0|2k2+1|zz0||f2(y2)|p0dy2)1p0dzC1|B|Bk1=1k2=12i=12ki(n(11p0)+ε2α)|zz0|ε(n(22p0)+εα)2i=1(2ki+1|zz0|)np0dzMp0(f1)(x)×Mp0(f2)(x)C1|B|k1=1k2=12i=12kiε2αB|zz0|εεαdzMp0(f1)(x)Mp0(f2)(x)Ck1=1k2=12i=12kiε2αrεεαBMp0(f1)(x)Mp0(f2)(x)CMp0(f1)(x)Mp0(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 ˜z03B2B 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/δC(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:=4j=1˜Ij.

    Notice that 0<δ<q< and 0<l/qα, where l and q are given as in Definition 1.2. By Lemma 3.1, we have

    ˜I1C|B|1/δT(˜f11,˜f12)Lδ(B)C|B|1/qT(˜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)1l2Crn(αl1q)BMl1(f1)(x)Ml2(f2)(x)CMp0(f1)(x)Mp0(f2)(x).

    For zB and y1(16˜B)c, there are |z˜z0|α(4rB)α12|y1˜z0|, rB|z˜z0|4rB and |z˜z0|<1. By Hölder's inequality and the condition (1.3) of the kernel, we have

    ˜I2C1|B|B|T(˜f21,˜f12)(z)T(˜f21,˜f12)(˜z0)|dzC1|B|Bk=12k|z˜z0|α|y1˜z0|2k+1|z˜z0|α16˜B|K(z,y1,y2)K(˜z0,y1,y2)||f1(y1)||f2(y2)|dy2dy1dzC1|B|Bk=116˜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)|p0dy1)1p0|f2(y2)|dy2dzC1|B|Bk=1|˜B|2k(n(21p0)+εα)|z˜z0|εα(n(21p0)+εα)(2k+1|z˜z0|α)np0dzMp0(f1)(x)M(f2)(x)C1|B|k=1|˜B|2k(n+εα)B|z˜z0|αndzMp0(f1)(x)Mp0(f2)(x)CMp0(f1)(x)Mp0(f2)(x).

    Similarly we can also get that

    ˜I3CMp0(f1)(x)Mp0(f2)(x).

    For zB 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

    ˜I4C1|B|B|T(˜f21,˜f22)(z)T(˜f21,˜f22)(˜z0)|dzC1|B|Bk1=1k2=1(2k1|z˜z0|α|y1˜z0|2k1+1|z˜z0|α2k2|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)|p0dy1)1p0×(2k2|z˜z0|α|y2˜z0|2k2+1|z˜z0|α|f2(y2)|p0dy2)1p0dzC1|B|Bk1=1k2=12i=12ki(n(11p0)+ε2α)|z˜z0|εα(n(22p0)+εα)2i=1(2ki+1|z˜z0|α)np0dz×Mp0(f1)(x)Mp0(f2)(x)Ck1=1k2=12i=12kiε2αMp0(f1)(x)Mp0(f2)(x)CMp0(f1)(x)Mp0(f2)(x).

    Thus, according to the estimates in both cases, there is

    Mδ(T(f1,f2))(x)supBxinfaC(1|B|B||T(f1,f2)(z)|δa|dz)1/δCMp0(f1)(x)Mp0(f2)(x),

    which completes the proof of the lemma.

    Lemma 3.3. [9] Let 0<p,δ< and wA. Then there exists a constant C>0 depending only on the A constant of w such that

    Rn[Mδ(f)(x)]pw(x)dxCRn[Mδ(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 1p1,,pm<, and for 0<θ1,,θm<1 such that θ1++θm=1, we have wθ11wθmmAmax{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 wA1,

    Rn|f(x)|~p0w(x)dxC0Rn|g(x)|~p0w(x)dx.

    Let p()P(Rn) with ~p0p. If (p()~p0)B(Rn), then there exists a constant C>0 such that for all (f,g)F, fLp()(Rn)CgLp()(Rn).

    Lemma 3.7. [25] Let p(),p1(),,pm()P(Rn) with 1/p(x)=1/p1(x)++1/pm(x). Then for any fjLpj()(Rn), j=1,,m, there has

    mj=1fjLp()(Rn)2m1mj=1fjLpj()(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()~p0B(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 Cc(Rn) is dense in Lp()(Rn).

    Lemma 3.10. [26] Let f be a function in BMO. Suppose 1p<, xRn, and r1,r2>0. Then

    (1|B(x,r1)|B(x,r1)|f(y)fB(x,r2)|pdy)1/pC(1+|lnr1r2|)fBMO,

    where C>0 is independent of f, x, r1 and r2.

    Proof of Theorem 2.1. From the fact that wjApj/p0 and pj>p0 (j=1,,m), it follows that the Hardy-Littlewood maximal operator M is bounded on Lpj/p0(wj). By Lemma 3.4, we obtain wAmax{p1/p0,,pm/p0}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)CMδ(T(f))Lp(w)Cmj=1Mp0(fj)Lp(w)Cmj=1Mp0(fj)Lpj(wj)=Cmj=1M(|fj|p0)1/p0Lpj/p0(wj)Cmj=1|fj|p01/p0Lpj/p0(wj)=Cmj=1fjLpj(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 wA1, by Lemma 3.2 and Lemma 3.3, we can get that

    Rn|T(f)(x)|~p0w(x)dxRn[Mδ(T(f))(x)]~p0w(x)dxCRn[Mδ(T(f))(x)]~p0w(x)dxCRn[mj=1Mp0(fj)(x)]~p0w(x)dxCRn[mj=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.



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