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BY 4.0 license Open Access Published by De Gruyter Open Access October 5, 2022

A note on commutators of strongly singular Calderón-Zygmund operators

  • Pu Zhang EMAIL logo and Xiaomeng Zhu
From the journal Open Mathematics

Abstract

In this article, the authors consider the commutators of strongly singular Calderón-Zygmund operator with Lipschitz functions. A sufficient condition is given for the boundedness of the commutators from Lebesgue spaces L p ( R n ) to certain Campanato spaces C p , β ( R n ) .

MSC 2010: 42B20; 42B35; 47B47

1 Introduction and result

Let T be the classical singular integral operator, and the commutator T b generated by T and a locally integrable function b is given by

T b f = b T ( f ) T ( b f ) .

A well-known result by Coifman et al. [1] states that T b is bounded on L p ( R n ) for 1 < p < when b BMO ( R n ) . They also gave some characterization of BMO ( R n ) in virtue of the L p boundedness of the aforementioned commutator (see also [2,3]).

In 1978, Janson [2] studied the boundedness of the commutator T b when b Λ ˙ γ ( R n ) , the homogeneous Lipschitz space of order 0 < γ < 1 , which is the space of all functions b , such that

(1.1) b Λ ˙ γ ( R n ) = sup x , y R n x y b ( x ) b ( y ) x y γ < .

Janson proved that T b is bounded from L p ( R n ) to L q ( R n ) for 1 < p < q < if and only if b Λ ˙ γ ( R n ) with γ = n ( 1 / p 1 / q ) . In 1995, Paluszyński [4] made a further study of the problem and proved that T b is bounded from L p ( R n ) to some Triebel-Lizorkin spaces F ˙ p γ , ( R n ) if and only if b Λ ˙ γ ( R n ) , for 1 < p < and 0 < γ < 1 .

In 2015, Zhang et al. [5] gave another kind of interesting results for T b when b belongs to Lipschitz spaces. They proved that T b is bounded from L p ( R n ) to C p , β ( R n ) if and only if b Λ ˙ γ ( R n ) , for 1 < p < , n / p β < 0 and 0 < γ = β + n / p < 1 , where C p , β ( R n ) is Campanato space (see Definition 1.2).

On the other hand, motivated by the study of multiplier operator with symbol given by e i ξ α ξ β away from the origin ( 0 < α < 1 , β > 0 ) , Alvarez and Milman [6] introduced the following strongly singular Calderón-Zygmund operator.

Definition 1.1

[6] Let T : S S be a bounded linear operator. T is called a strongly singular Calderón-Zygmund operator if the following conditions are fulfilled.

  1. T can be extended to a continuous operator from L 2 into itself.

  2. There exists a continuous function K ( x , y ) on { ( x , y ) : x y } such that

    K ( x , y ) K ( x , z ) + K ( y , x ) K ( z , x ) C y z δ x z n + δ / α ,

    if 2 y z α x z for some 0 < δ 1 and 0 < α < 1 , and,

    T f , g = K ( x , y ) f ( y ) g ( x ) d y d x ,

    for f , g S with disjoint supports.

  3. For some ( 1 α ) n / 2 η < n / 2 , both T and its conjugate operator T can be extended to continuous operators from L q ( R n ) into L 2 ( R n ) , where 1 / q = 1 / 2 + η / n .

In 1986, Alvarez and Milman studied the boundedness of strongly singular Calderón-Zygmund operator on Lebesgue spaces and Hardy spaces in [6,7]. Later on, there are many authors discussed the mapping properties of strongly singular Calderón-Zygmund operators in various spaces. See, for instance, [8,9, 10,11]. We would like to note that, as stated in [6,7], the strongly singular Calderón-Zygmund operators include pseudo-differential operator with a symbol in the Hörmander class S α , δ η , where 0 < δ α < 1 , ( 1 α ) n / 2 η < n / 2 .

Now, we define the commutator generated by strongly singular Calderón-Zygmund operator T and a locally integrable function b as follows:

T b f ( x ) = b ( x ) T ( f ) ( x ) T ( b f ) ( x ) .

The main result of Alvarez et al. in [8] yields the boundedness of T b on L p ( R n ) , 1 < p < , when b BMO ( R n ) . Afterward, the mapping properties of T b , when b belongs to BMO space or Lipschitz space, on Lebesgue spaces, Morrey spaces, Herz type spaces, and Hardy spaces have been studied by several authors. See [10,11,12, 13,14,15] for example.

In this article, we will continue the study of the commutator of strongly singular Calderón-Zygmund operator when the symbol b belongs to Lipschitz space. The aim is to extend some of the results in [5] to a strongly singular Calderón-Zygmund operator.

As usual, let B = B ( x 0 , r ) denote the ball centered at x 0 with radius r . For a > 0 , a B stands for the ball concentric with B having a times its radius, that is, a B = B ( x 0 , a r ) . Denote by B the Lebesgue measure of B and by χ B its characteristic function. For f L loc 1 ( R n ) , we write

f B = 1 B B f ( x ) d x .

Definition 1.2

Let 1 p < , n / p β < 1 , the Campanato space C p , β ( R n ) is given by

C p , β ( R n ) = { f L loc p ( R n ) , f C p , β ( R n ) < } ,

where

f C p , β ( R n ) sup B 1 B β / n 1 B B f ( x ) f B p d x 1 / p ,

and the supremum is taken over all balls B in R n .

Our result can be stated as follows.

Theorem 1.1

Let T be a strongly singular Calderón-Zygmund operator, and, α , η , and δ be as in Definition 1.1. Suppose that n ( 1 α ) + 2 η 2 η < p < , n / p β < 0 , and 0 < γ = β + n / p < 1 . If b Λ ˙ γ ( R n ) , then T b is bounded from L p ( R n ) to C p , β ( R n ) , that is, there exists a constant C > 0 such that for all f L p ( R n ) ,

T b ( f ) C p , β ( R n ) C b Λ ˙ γ ( R n ) f L p ( R n ) .

Remark 1.1

Theorem 1.1 gives a new kind of boundedness for commutator T b when b belongs to certain Lipschitz spaces, compared with the ( L p , L q ) -boundedness and the ( M p , β , M q , β + γ ) -boundedness of T b , when n ( 1 α ) + 2 η 2 η < p < q < and 0 < γ = n 1 p 1 q < 1 , obtained in [12, Corollary 1] and [10, Theorem 2.2], respectively.

2 Proof of Theorem 1.1

To prove Theorem 1.1, we need some known results. The first one is due to DeVore and Sharpley [16] and Janson et al. [17] (see also Paluszyński [4], Lemma 1.5).

Lemma 2.1

Let 0 < γ < 1 and b Λ ˙ γ ( R n ) , then for all 1 p < ,

b Λ ˙ γ ( R n ) sup B 1 B γ / n 1 B B b ( x ) b B p d x 1 / p sup B 1 B γ / n b b B L ( B ) .

The next result is easy to check by using (1.1). See also DeVore and Sharpley [16], page 14.

Lemma 2.2

[16] Let 0 < γ < 1 , b Λ ˙ γ ( R n ) , and B and B be balls in R n . If B B , then

b B b B C b Λ ˙ γ ( R n ) B γ / n .

Now we recall the boundedness of strongly singular Calderón-Zygmund operator T on Lebesgue spaces. Let us observe that T is bounded from L to BMO ([6], Theorem 2.1), from L 1 to L 1 , ([7], Theorem 4.1), and from H 1 to L 1 ([12], Lemma 2), and note the assumption (3) in Definition 1.1, and by interpolation between these estimates, we achieve the following L p -boundedness of T . We refer to [12] (page 1052) and [11] (pages 42 and 43), for details.

Lemma 2.3

Let T be a strongly singular Calderón-Zygmund operator, and, α , η , and δ be the same as in Definition 1.1.

  1. If 1 < p < , then T is bounded from L p ( R n ) to itself.

  2. If n ( 1 α ) + 2 η 2 η u < , then there is a positive number v satisfying 0 < u / v α , such that T is bounded from L u ( R n ) to L v ( R n ) .

Furthermore, the index v can be chosen as v = u q 2 q u q + 2 u 2 when n ( 1 α ) + 2 η 2 η u 2 and v = u q 2 when 2 u < , where q is given in Definition 1.1 and q is its conjugate index.

Now, let us prove Theorem 1.1.

Proof of Theorem 1.1

For any f L p ( R n ) , it suffices to prove

(2.1) 1 B β / n 1 B B T b f ( y ) ( T b f ) B p d y 1 / p C b Λ ˙ γ ( R n ) f L p ( R n ) ,

for all balls B in R n .

For any ball B = B ( x 0 , r ) centered at x 0 with radius r , we divide the proof into two cases.

Case 1. The case when r > 1 . Denote by B = 8 B = B ( x 0 , 8 r ) the ball with the same center as B and 8 times the radius. Let f 1 = f χ B and f 2 = f f 1 . For any real number c , by Minkowski’s inequality and Hölder’s inequality, we have

1 B β / n 1 B B T b f ( y ) ( T b f ) B p d y 1 / p 1 B β / n 1 B B T b f ( y ) c p d y 1 / p + 1 B β / n 1 B B ( T b f ) B c p d y 1 / p 1 B β / n 1 B B T b f ( y ) c p d y 1 / p + 1 B β / n ( T b f ) B c 1 B β / n 1 B B T b f ( y ) c p d y 1 / p + 1 B β / n 1 B B T b f ( z ) c d z 1 B β / n 1 B B T b f ( y ) c p d y 1 / p + 1 B β / n 1 B B T b f ( z ) c p d z 1 / p 2 B β / n 1 B B T b f ( y ) c p d y 1 / p .

Let c = ( T ( ( b b B ) f 2 ) ) B and notice that T b f = T b b B f , one has

(2.2) 1 B β / n 1 B B T b f ( y ) ( T b f ) B p d y 1 / p 2 B β / n 1 B B T b b B f ( y ) + ( T ( ( b b B ) f 2 ) ) B p d y 1 / p 2 B β / n 1 B B ( b ( y ) b B ) T f ( y ) p d y 1 / p + 2 B β / n 1 B B T ( ( b b B ) f 1 ) ( y ) p d y 1 / p + 2 B β / n 1 B B T ( ( b b B ) f 2 ) ( y ) ( T ( ( b b B ) f 2 ) ) B p d y 1 / p I 1 + I 2 + I 3 .

For I 1 , note that 1 < p < and 0 < γ = β + n / p < 1 , it follows from Lemmas 2.1 and 2.3 that

I 1 = 2 B γ / n B ( b ( y ) b B ) T f ( y ) p d y 1 / p 2 B γ / n b b B L ( B ) B T f ( y ) p d y 1 / p

C b Λ ˙ γ ( R n ) T f L p ( R n ) C b Λ ˙ γ ( R n ) f L p ( R n ) .

Next we estimate I 2 . Again we note that 1 < p < and 0 < γ = β + n / p < 1 . By Lemmas 2.1, 2.2, and 2.3, we deduce

I 2 2 B γ / n T ( ( b b B ) f 1 ) L p ( R n ) C B γ / n ( b b B ) f 1 L p ( R n ) C B γ / n { ( b b B ) f L p ( B ) + ( b B b B ) f L p ( B ) } C B γ / n { b b B L ( B ) + b B b B } f L p ( R n ) C B γ / n { C B γ / n b Λ ˙ γ ( R n ) + C b Λ ˙ γ ( R n ) B γ / n } f L p ( R n ) C b Λ ˙ γ ( R n ) f L p ( R n ) .

Now, let us consider I 3 . Since for any w , y B = B ( x 0 , r ) and any z ( B ) c one has 2 y w α < z w , it follows from Definition 1.1 that

(2.3) T ( ( b b B ) f 2 ) ( y ) T ( ( b b B ) f 2 ) ( w ) R n K ( y , z ) K ( w , z ) ( b ( z ) b B ) f 2 ( z ) d z = ( B ) c K ( y , z ) K ( w , z ) b ( z ) b B f ( z ) d z C ( B ) c y w δ z w n + δ / α b ( z ) b B f ( z ) d z C k = 1 2 k B \ 2 k 1 B y w δ z w n + δ / α b ( z ) b B f ( z ) d z C r δ δ / α k = 1 2 k δ / α 2 k B 2 k B b ( z ) b B f ( z ) d z .

Observe that the last term of (2.3) is always independent of w and y , for any w , y B . Then we can write

(2.4) I 3 = 2 B β / n 1 B B T ( ( b b B ) f 2 ) ( y ) ( T ( ( b b B ) f 2 ) ) B p d y 1 / p 2 B β / n 1 B B 1 B B T ( ( b b B ) f 2 ) ( y ) T ( ( b b B ) f 2 ) ( w ) d w p d y 1 / p 2 B β / n 1 B B 1 B B C r δ δ / α k = 1 2 k δ / α 2 k B 2 k B b ( z ) b B f ( z ) d z d w p d y 1 / p C r δ ( 1 1 / α ) B β / n k = 1 2 k δ / α 2 k B 2 k B b ( z ) b B f ( z ) d z C r δ ( 1 1 / α ) B β / n k = 1 2 k δ / α 2 k B 2 k B b ( z ) b 2 k B f ( z ) d z + C r δ ( 1 1 / α ) B β / n k = 1 2 k δ / α 2 k B 2 k B b 2 k B b B f ( z ) d z I 3 , 1 + I 3 , 2 .

Applying Hölder’s inequality, Lemma 2.1, and noting that 0 < γ = β + n / p < 1 , we obtain

I 3 , 1 C r δ ( 1 1 / α ) B β / n k = 1 2 k δ / α 2 k B 2 k B b ( z ) b 2 k B p d z 1 / p 2 k B f ( z ) p d z 1 / p C r δ ( 1 1 / α ) B β / n k = 1 2 k δ / α 2 k B 2 k B γ / n + 1 / p b Λ ˙ γ ( R n ) f L p ( R n ) C b Λ ˙ γ ( R n ) f L p ( R n ) r δ ( 1 1 / α ) B β / n k = 1 2 k δ / α 2 k B β / n C b Λ ˙ γ ( R n ) f L p ( R n ) r δ ( 1 1 / α ) k = 1 2 k ( β δ / α ) C b Λ ˙ γ ( R n ) f L p ( R n ) ,

where in the last step we made use of the fact that r δ ( 1 1 / α ) 1 since r > 1 and δ ( 1 1 / α ) < 0 and the fact that the series k = 1 2 k ( β δ / α ) is convergent since β δ / α < 0 .

For I 3 , 2 , noting that 0 < γ = β + n / p < 1 and applying Lemma 2.2 and Hölder’s inequality, we have

I 3 , 2 = C r δ ( 1 1 / α ) B β / n k = 1 2 k δ / α 2 k B 2 k B b 2 k B b B f ( z ) d z C r δ ( 1 1 / α ) B β / n k = 1 2 k δ / α 2 k B b Λ ˙ γ ( R n ) 2 k B γ / n 2 k B f ( z ) d z C b Λ ˙ γ ( R n ) r δ ( 1 1 / α ) B β / n k = 1 2 k δ / α 2 k B 2 k B γ / n 2 k B f ( z ) p d z 1 / p 2 k B 1 1 / p C b Λ ˙ γ ( R n ) f L p ( R n ) r δ ( 1 1 / α ) B β / n k = 1 2 k δ / α 2 k B β / n C b Λ ˙ γ ( R n ) f L p ( R n ) r δ ( 1 1 / α ) k = 1 2 k ( β δ / α ) C b Λ ˙ γ ( R n ) f L p ( R n ) ,

where in the last step we also made use of the fact that r δ ( 1 1 / α ) 1 and k = 1 2 k ( β δ / α ) is convergent. This, together with the estimates for I 3 , 1 , yields

I 3 C b Λ ˙ γ ( R n ) f L p ( R n ) .

Combining the estimates for I 1 , I 2 , and I 3 leads to (2.1) for the case r > 1 .

Case 2. The case 0 < r 1 . Set B ˜ = B ( x 0 , r α ) and denote B ˜ = 8 B ˜ = B ( x 0 , 8 r α ) . Let f 3 = f χ B ˜ and f 4 = f f 3 . For the same reason as that in (2.2), we deduce that

1 B β / n 1 B B T b f ( y ) ( T b f ) B p d y 1 / p 2 B β / n + 1 / p B ( b ( y ) b B ) T f ( y ) p d y 1 / p + 2 B β / n + 1 / p B T ( ( b b B ) f 3 ) ( y ) p d y 1 / p + 2 B β / n + 1 / p B T ( ( b b B ) f 4 ) ( y ) ( T ( ( b b B ) f 4 ) ) B p d y 1 / p J 1 + J 2 + J 3 .

Similar to I 1 , we have

J 1 = 2 B γ / n B ( b ( y ) b B ) T f ( y ) p d y 1 / p C b Λ ˙ γ ( R n ) f L p ( R n ) .

To estimate J 2 , we first observe that, by Lemma 2.3, there is an s satisfying 0 < p / s α such that T is bounded from L p to L s since n ( 1 α ) + 2 η 2 η < p < . This, together with Hölder’s inequality, Lemmas 2.1 and 2.2, gives

J 2 = 2 B β / n + 1 / p B T ( ( b b B ) f 3 ) ( y ) p d y 1 / p 2 B β / n + 1 / s T ( ( b b B ) f 3 ) L s ( R n ) C B β / n + 1 / s ( b b B ) f 3 L p ( R n ) C B β / n + 1 / s { ( b b B ˜ ) f L p ( B ˜ ) + ( b B ˜ b B ) f L p ( B ˜ ) } C B β / n + 1 / s { b b B ˜ L ( B ˜ ) + b B ˜ b B } f L p ( R n ) C B β / n + 1 / s B ˜ γ / n b Λ ˙ γ ( R n ) f L p ( R n ) C r ( α 1 ) β + ( α / p 1 / s ) n b Λ ˙ γ ( R n ) f L p ( R n ) C b Λ ˙ γ ( R n ) f L p ( R n ) ,

where the last two steps follow from the condition 0 < γ = β + n / p < 1 and the fact that r ( α 1 ) β + ( α / p 1 / s ) n 1 since 0 < r 1 and ( α 1 ) β + ( α / p 1 / s ) n > 0 .

Finally, let us consider J 3 . Since 0 < r 1 and 2 y w α < z w for any w , y B = B ( x 0 , r ) and z ( B ˜ ) c , similar to (2.3), we have

T ( ( b b B ) f 4 ) ( y ) T ( ( b b B ) f 4 ) ( w ) R n K ( y , z ) K ( w , z ) ( b ( z ) b B ) f 4 ( z ) d z C ( B ˜ ) c y w δ z w n + δ / α b ( z ) b B f ( z ) d z C k = 1 2 k B ˜ \ 2 k 1 B ˜ y w δ z w n + δ / α b ( z ) b B f ( z ) d z C k = 1 2 k δ / α 2 k B ˜ 2 k B ˜ b ( z ) b B f ( z ) d z .

Reasoning as in (2.4), we can also write

J 3 = 2 B β / n 1 B B T ( ( b b B ) f 4 ) ( y ) ( T ( ( b b B ) f 4 ) ) B p d y 1 / p C B β / n k = 1 2 k δ / α 2 k B ˜ 2 k B ˜ b ( z ) b B f ( z ) d z C B β / n k = 1 2 k δ / α 2 k B ˜ 2 k B ˜ b ( z ) b 2 k B ˜ f ( z ) d z + C B β / n k = 1 2 k δ / α 2 k B ˜ 2 k B ˜ b 2 k B ˜ b B f ( z ) d z J 3 , 1 + J 3 , 2 .

To estimate J 3 , 1 , we first observe the fact that r β ( α 1 ) 1 since 0 < r 1 and β ( α 1 ) > 0 and the series k = 1 2 k ( β δ / α ) is convergent since β δ / α < 0 . Then by Hölder’s inequality and Lemma 2.1 and noticing that 0 < γ = β + n / p < 1 , we obtain

J 3 , 1 = C B β / n k = 1 2 k δ / α 2 k B ˜ 2 k B ˜ b ( z ) b 2 k B ˜ f ( z ) d z C B β / n k = 1 2 k δ / α 2 k B ˜ 2 k B ˜ b ( z ) b 2 k B ˜ p d z 1 / p f L p ( R n ) C B β / n k = 1 2 k δ / α 2 k B ˜ 2 k B ˜ γ / n + 1 / p b Λ ˙ γ ( R n ) f L p ( R n ) C B β / n k = 1 2 k δ / α 2 k B ˜ β / n b Λ ˙ γ ( R n ) f L p ( R n ) C b Λ ˙ γ ( R n ) f L p ( R n ) r β ( α 1 ) k = 1 2 k ( β δ / α ) C b Λ ˙ γ ( R n ) f L p ( R n ) .

For J 3 , 2 , applying Lemma 2.2 and Hölder’s inequality, and observing again the fact that r β ( α 1 ) 1 , the series k = 1 2 k ( β δ / α ) is convergent and 0 < γ = β + n / p < 1 , and we have

J 3 , 2 = C B β / n k = 1 2 k δ / α 2 k B ˜ 2 k B ˜ b 2 k B ˜ b B f ( z ) d z C B β / n k = 1 2 k δ / α 2 k B ˜ 2 k B ˜ γ / n b Λ ˙ γ ( R n ) 2 k B ˜ f ( z ) d z C B β / n k = 1 2 k δ / α 2 k B ˜ 2 k B ˜ γ / n b Λ ˙ γ ( R n ) f L p ( 2 k B ˜ ) 2 k B ˜ 1 / p C B β / n k = 1 2 k δ / α 2 k B ˜ β / n b Λ ˙ γ ( R n ) f L p ( R n ) C b Λ ˙ γ ( R n ) f L p ( R n ) r β ( α 1 ) k = 1 2 k ( β δ / α ) C b Λ ˙ γ ( R n ) f L p ( R n ) .

The estimate for J 3 , 2