Home Some estimates for commutators of Littlewood-Paley g-functions
Article Open Access

Some estimates for commutators of Littlewood-Paley g-functions

  • Guanghui Lu EMAIL logo
Published/Copyright: August 27, 2021

Abstract

The aim of this paper is to establish the boundedness of commutator [ b , g ˙ r ] generated by Littlewood-Paley g -functions g ˙ r and b RBMO ( μ ) on non-homogeneous metric measure space. Under assumption that λ satisfies ε -weak reverse doubling condition, the author proves that [ b , g ˙ r ] is bounded from Lebesgue spaces L p ( μ ) into Lebesgue spaces L p ( μ ) for p ( 1 , ) and also bounded from spaces L 1 ( μ ) into spaces L 1 , ( μ ) . Furthermore, the boundedness of [ b , g ˙ r ] on Morrey space M q p ( μ ) and on generalized Morrey L p , ϕ ( μ ) is obtained.

MSC 2010: 42B25; 42B35; 30L99

1 Introduction

Although the metric measure spaces equipped with the polynomial growth conditions (see [1,2,3, 4,5]) and spaces of homogeneous type in the sense of Coifman and Weiss [6,7] are two important classes of function spaces in harmonic analysis, there exist no relations between the non-doubling measure spaces and spaces of homogeneous type. To solve this problem, Hytönen [8] first introduced the non-homogeneous metric measure spaces satisfying the so-called geometrically doubling and upper doubling conditions. From then on, many papers focus on the properties of function spaces and operators over non-homogeneous metric measure spaces. For example, Cao and Zhou [9] obtained the definition of Morrey space on non-homogeneous metric measure space and also proved that Hardy-Littlewood maximal operator, Calderón-Zygmund operator and fractional integral are bounded on Morrey space. Fu and Zhao [10] proved that generalized homogeneous Littlewood-Paley g -function is bounded from atomic Hardy space H atb 1 ( μ ) into space L 1 ( μ ) and also bounded from space RBMO ( μ ) into space RBLO ( μ ) . For more development of harmonic analysis on non-homogeneous metric measure space the readers can see [11,12,13, 14,15,16, 17,18,19] and references therein.

Let ( X , d , μ ) be a non-homogeneous metric measure space in the sense of Hytönen [8]. In this setting, the author proves that the commutator [ b , g ˙ r ] generated by b RBMO ( μ ) and generalized homogeneous Littlewood-Paley g -function g ˙ r is bounded on Lebesgue spaces L p ( μ ) for p ( 1 , ) and also bounded from spaces L 1 ( μ ) into spaces L 1 , ( μ ) . Furthermore, the boundedness of [ b , g ˙ r ] on Morrey space M q p ( μ ) and on generalized Morrey space L p , ϕ ( μ ) is also established in this paper. In 2016, Fu and Zhao obtained the boundedness of g ˙ r on atomic Hardy space H atb 1 ( μ ) and on space RBMO ( μ ) (see [10]). In 2021, Lu and Tao [11] proved that the g ˙ r is bounded on Lipschitz space Lip β ( μ ) and on generalized Morrey space L p , ϕ ( μ ) .

Before stating the main results of this paper, we first recall some necessary notions. The following definitions of geometrically doubling and upper doubling conditions are from [8].

Definition 1.1

A metric space ( X , d ) is said to be geometrically doubling if there exists some N 0 N such that, for any ball B ( x , r ) X with x X and r ( 0 , ) , there exists a finite ball covering { B ( x i , r / 2 ) } i of B ( x , r ) such that the cardinality of this covering is at most N 0 .

Remark 1.2

Let ( X , d ) be a metric measure. Hytönen [8] showed that the geometrically doubling ( X , d ) is equivalent to the following statement: for any ε ( 0 , 1 ) and any ball B ( x , r ) X with x X and r ( 0 , ) , there exists a finite ball covering { B ( x i , ε r ) } i of B ( x , r ) such that the cardinality of this covering is at most ε n 0 , where n 0 log 2 N 0 .

Definition 1.3

A metric measure space ( X , d , μ ) is said to be upper doubling if μ is a Borel measure on X and there exist a dominating function λ : X × ( 0 , ) ( 0 , ) and constant C ( λ ) > 0 , depending on λ , such that, for each x X , r λ ( x , r ) is non-decreasing and for all x X and r ( 0 , ) ,

(1.1) μ ( B ( x , r ) ) λ ( x , r ) C ( λ ) λ ( x , r / 2 ) .

Moreover, Hytönen et al. [12] showed that there exists another dominating function λ ˜ such that λ ˜ λ , C ( λ ˜ ) C ( λ ) and, for all x , y X with d ( x , y ) r ,

(1.2) λ ˜ ( x , r ) C ( λ ) λ ˜ ( y , r ) .

Here and in what follows, we always assume that λ satisfies (1.2).

Although the doubling measure condition is not assumed uniformly for all balls on ( X , d , μ ) , Hytönen [8] showed that there exist many balls satisfying the ( α , β ) -doubling condition, i.e., let α , β ( 1 , ) , a ball B X is said to be ( α , β ) -doubling if μ ( α B ) β μ ( B ) . Throughout this paper, for any α ( 1 , ) and ball B , the smallest ( α , β α ) -doubling ball of the form α j B with j N is denoted by B ˜ α , where

β α α 3 ( max { n , ν } ) + 3 0 n + 3 0 ν .

We always denote by B ˜ the smallest ( 6 , β 6 ) -doubling ball of the form B ˜ 6 in this paper.

We now recall the definition of coefficient K B , S introduced in [8], which is very close to the quantity K Q , R introduced by Tolsa [3], that is, for any two balls B S , define

(1.3) K B , S 1 + ( 2 S ) B 1 λ ( c ( B ) , d ( x , c ( B ) ) ) d μ ( x ) ,

where c ( B ) represents the center of ball B . For more properties of the K B , S , we can see [12, Lemma 2.1].

The following regularized bounded mean oscillation (RBMO) space was from [8].

Definition 1.4

Let ρ > 1 . A function f L loc 1 ( μ ) is said to be in the space RBMO ( μ ) if there exist a positive constant C and, for any ball B , a number f B such that

(1.4) 1 μ ( ρ B ) B f ( y ) f B d μ ( y ) C

and, for any two balls B and S such that B S ,

(1.5) f B f S C K B , S .

The infimum of the positive constants C satisfying both (1.4) and (1.5) is defined to be the RBMO ( μ ) norm of f and denoted by f RBMO ( μ ) . Moreover, Hytönen [8] also showed that the space RBMO ( μ ) is independent of the choice of the constant ρ ( 1 , ) .

In 2015, Tan and Li [13] gave an approximation of the identity S { S k } k Z associated with ( 2 , 2 ( C λ + 1 ) ) -doubling balls { Q x , k } x supp ( μ ) , k Z on ( X , d , μ ) , which are integral operators associated with kernels S k ( x , y ) on X × X satisfying the following conditions:

  1. S k ( x , y ) = S k ( y , x ) for all x , y supp ( μ ) .

  2. For any k Z and x supp ( μ ) , S k 1 ( x ) = 1 = S k 1 ( x ) , where S k is the adjoint operator of S k .

  3. For each k Z and x supp ( μ ) , supp ( S k ( x , ) ) Q x , k 1 .

  4. For all x , y X and k Z , if x y or Q x , k { x } , then there exists a non-negative constant C such that

    0 S k ( x , y ) C λ ( x , r ( Q x , k ) + r ( Q y , k ) + d ( x , y ) ) .

  5. For all x , x ˜ , y X and k Z , if x , x ˜ Q x 0 , k for some x 0 supp ( μ ) and x x ˜ , then there exists a positive constant C such that

    S k ( x , y ) S k ( x ˜ , y ) d ( x , x ˜ ) r ( Q x 0 , k ) ε C λ ( x , r ( Q x , k ) + r ( Q y , k ) + d ( x , y ) ) ,

    where ε ( 0 , ) and Q x , k represents a fixed doubling ball center as x of generation k .

Moreover, Tan and Li [13] showed that the aforementioned results through (A-1) to (A-5) are still correct if the ( 2 , 2 ( C λ + 1 ) ) -doubling balls are replaced by ( 6 , β 6 ) -doubling balls.

We now recall the definition of generalized homogeneous Littlewood-Paley g -function introduced in [10].

Definition 1.5

Let k Z , r [ 2 , ) , D k ( x , y ) S k ( x , y ) S k 1 ( x , y ) for all x , y X , and D k be the corresponding integral operator associated with the kernel D k ( x , y ) . Then, the generalized homogeneous Littlewood-Paley g -function g ˙ r is defined by

(1.6) g ˙ r ( f ) ( x ) k Z D k ( x , ) f ( x ) r 1 r , for any x X .

Given a function b RBMO ( μ ) , the commutator [ b , g ˙ r ] , which is generated by b and g ˙ r as in (1.6), is defined by

(1.7) [ b , g ˙ r ] ( x ) k Z D k ( x , ) ( b ( x ) b ( ) ) f ( x ) r 1 r ,

where x X and f L b ( μ ) being the space of all L ( μ ) functions with bounded support.

The following definition of generalized Morrey space is from [14].

Definition 1.6

Let k > 1 and 1 < p < . Suppose that ϕ is an increasing function on ( 0 , ) . Then, the generalized Morrey space L p , ϕ ( μ ) is defined by

L p , ϕ ( μ ) { f L loc p ( μ ) : f L p , ϕ ( μ ) < } ,

where

(1.8) f L p , ϕ ( μ ) = sup B [ ϕ ( μ ( k B ) ) ] 1 p B f ( x ) p d μ ( x ) 1 p .

Remark 1.7

  1. From [14], Lu and Tao showed that the norm f M q p ( μ ) is independent of the choice of parameter k for k > 1 .

  2. If we take ϕ ( t ) = t 1 q p with t > 0 and 1 < q p < , then L p , ϕ ( μ ) defined as in (1.8) is just the Morrey space M q p ( μ ) , which was introduced by Cao and Zhou [9], that is, let k > 1 and 1 < q p < , then Morrey space M q p ( μ ) is defined by

    M q p ( μ ) = { f L loc q ( μ ) : f M q p ( μ ) < } ,

    where

    (1.9) f M q p ( μ ) sup B [ μ ( k B ) ] 1 p 1 q B f ( y ) q d μ ( y ) 1 q .

We now recall the following ε -weak reverse doubling condition introduced in [16].

Definition 1.8

Let ε ( 0 , ) . A dominating function λ is said to satisfy the ε -weak reverse doubling condition if, for all r ( 0 , 2 diam ( X ) ) and a ( 1 , 2 diam ( X ) / r ) , there exists a number C ( a ) [ 1 , ) , depending only on a and X , such that, for all x X ,

λ ( x , a r ) C ( a ) λ ( x , r )

and, moreover,

(1.10) k = 1 1 [ C ( a k ) ] ε < .

The main theorems of this paper are stated as follows:

Theorem 1.9

Let b RBMO ( μ ) and r [ 2 , ) . Suppose that λ satisfies the ε -weak reverse doubling condition defined as in Definition 1.8. Then, there exists a constant C > 0 such that, for all f L p ( μ ) with p ( 1 , ) ,

[ b , g ˙ r ] ( f ) L p ( μ ) C b RBMO ( μ ) f L p ( μ ) .

Theorem 1.10

Let b RBMO ( μ ) and r [ 2 , ) . Suppose that λ satisfies the ε -weak reverse doubling condition defined as in Definition 1.8. Then, there exists a constant C > 0 such that, for all f L 1 ( μ ) ,

[ b , g ˙ r ] ( f ) L 1 , ( μ ) C b RBMO ( μ ) f L 1 ( μ ) .

Theorem 1.11

Let b RBMO ( μ ) , r [ 2 , ) and 1 < q p < . Suppose that λ satisfies the weak reverse doubling condition defined as in Definition 1.8. Then, there exists a constant C > 0 such that, for all f M q p ( μ ) ,

[ b , g ˙ r ] ( f ) M q p ( μ ) C b RBMO ( μ ) f M q p ( μ ) .

Theorem 1.12

Let b RBMO ( μ ) , r [ 2 , ) and p ( 1 , ) . Suppose that ϕ : ( 0 , ) ( 0 , ) is an increasing function and the mapping s ϕ ( s ) s is almost decreasing, namely, there is a constant C > 0 such that, the following inequality

(1.11) ϕ ( w ) w C ϕ ( s ) s

holds for s w . Then, there exists a positive constant C such that, for all f L p , ϕ ( μ ) ,

[ b , g ˙ r ] ( f ) L p , ϕ ( μ ) C b RBMO ( μ ) f L p , ϕ ( μ ) .

Finally, we make some conventions on notation. Throughout the paper, C represents a positive constant, which is independent of the main parameters. For any subset E of X , we use χ E to denote its characteristic function. Given any q ( 1 , ) , let q q / ( q 1 ) denote its conjugate index. For any ball B , c ( B ) and r ( B ) represent the center and radius of ball B , respectively. Furthermore, m B ( f ) denotes the mean value of function f over ball B , that is, m B ( f ) = 1 μ ( B ) B f ( y ) d μ ( y ) .

2 Preliminaries

To prove the main theorems of this paper, we should recall some necessary results in this section (see [10,14,16,17]).

Lemma 2.1

Let ( X , d , μ ) be a non-homogeneous metric measure space satisfying the weak reverse doubling condition, r [ 2 , ) and p ( 1 , ) . Then, there exists a constant C > 0 such that, for all f L p ( μ ) ,

(2.1) g ˙ r ( f ) L p ( μ ) C f L p ( μ ) .

Corollary 2.2

If f RBMO ( μ ) , then there exists a constant C > 0 such that, for any ball B , τ ( 1 , ) and s [ 1 , ) ,

(2.2) 1 μ ( τ B ) B f ( y ) f B s d μ ( y ) 1 s C f RBMO ( μ ) .

Lemma 2.3

  1. Let p ( 1 , ) , t ( 1 , p ) and ρ [ 5 , ) . The following maximal operators, respectively, defined for all f L loc 1 ( μ ) and x X ,

    (2.3) M t , ρ f ( x ) sup B x 1 μ ( ρ B ) B f ( y ) t d μ ( y ) 1 t

    and

    N f ( x ) sup B x B doubling 1 μ ( B ) B f ( y ) d μ ( y )

    are bounded on L p ( μ ) and also bounded from L 1 ( μ ) into L 1 , ( μ ) .

  2. For all f L loc 1 ( μ ) , it holds true that f ( x ) N f ( x ) for μ -a.e x X .

Lemma 2.4

Let f L loc 1 ( μ ) satisfy X f ( x ) d μ ( x ) = 0 when μ μ ( x ) < . Assume that, for some p , q satisfying 1 < q p < , inf { 1 , N f } M q p ( μ ) . Then, there exists a constant C > 0 ,

(2.4) N f M q p ( μ ) C M f M q p ( μ ) ,

where the sharp maximal operator M is defined by, for all f L loc 1 ( μ ) and x X ,

(2.5) M f ( x ) sup B x 1 μ ( 6 B ) B f ( y ) m B ˜ ( f ) d μ ( y ) + sup x B S B , S ( 6 , β 6 ) - doubling m B ( f ) m S ( f ) K B , S .

Lemma 2.5

Let ρ > 1 , 1 < t < p < and ϕ : ( 0 , ) ( 0 , ) be an increasing function. Suppose that M t , ρ is defined as in (2.3) and the mapping s ϕ ( s ) s satisfies the condition (1.11). Then, there exists a positive constant C > 0 such that, for all f L p , ϕ ( μ ) ,

M t , ρ f L p , ϕ ( μ ) C f L p , ϕ ( μ ) .

3 Proof of Theorems 1.9–1.12

Proof of Theorem 1.9

For any r [ 2 , ) , p ( 1 , ) , f L p ( μ ) and x X , we first claim that

(3.1) M ( [ b , g ˙ r ] ( f ) ) ( x ) C b RBMO ( μ ) { M r 2 , 6 ( f ) ( x ) + M r , 6 ( f ) ( x ) + M r , 6 ( g ˙ r ( f ) ) ( x ) } .

Once (3.1) is proved, by applying Lemma 2.3 and Theorem 4.2 in [15], we have

[ b , g ˙ r ] ( f ) L p ( μ ) N ( [ b , g ˙ r ] ( f ) ) L p ( μ ) C M ( [ b , g ˙ r ] ( f ) ) L p ( μ ) C b RBMO ( μ ) { M r , 6 ( g ˙ r ( f ) ) L p ( μ ) + M r 2 , 6 ( f ) L p ( μ ) + M r , 6 ( f ) L p ( μ ) } C b RBMO ( μ ) f L p ( μ ) ,

which is just the desired conclusion.

To show (3.1), by the definition of sharp maximal function M , there exists a family of numbers { b B } B such that, for all x and B with B x ,

(3.2) 1 μ ( 6 B ) B g ˙ r , b ( f ) ( x ) h B d μ ( x ) C b RBMO ( μ ) { M r 2 , 6 ( f ) ( x ) + M r , 6 ( f ) ( x ) + M r , 6 ( g ˙ r ( f ) ) ( x ) }

and, for all balls B , S satisfying B S and B x ,

(3.3) h B h S C K B , S b RBMO ( μ ) { M r , 6 ( g ˙ r ( f ) ) ( x ) + M r 2 , 6 ( f ) ( x ) + M r , 6 ( f ) ( x ) } ,

where

h B m B ( g ˙ r ( ( b b B ) f χ X 6 B ) ) and h S m S ( g ˙ r ( ( b b S ) f χ X 6 S ) ) .

To prove (3.2), for a fixed ball B and x with x B , write

[ b , g ˙ r ] ( f ) ( x ) C b ( x ) b B k Z D k f ( x ) r 1 r + C k Z D k ( b ( ) b B ) f 1 ( x ) r 1 r + C k Z D k ( b ( ) b B ) f 2 ( x ) r 1 r C { b ( x ) b B g ˙ r ( f ) ( x ) + g ˙ r ( ( b ( ) b B ) f 1 ) ( x ) + g ˙ r ( ( b ( ) b B ) f 2 ) ( x ) } ,

where f 1 f χ 6 B and f 2 f f 1 .

By applying Hölder inequality, (2.1) and (2.2), we obtain that

(3.4) 1 μ ( 6 B ) B b ( x ) b B g ˙ r ( f ) ( x ) d μ ( x ) 1 μ ( 6 B ) B g ˙ r ( f ) ( x ) r d μ ( x ) 1 r 1 μ ( 6 B ) B b ( x ) b B r d μ ( x ) 1 r C b RBMO ( μ ) M r , 6 ( g ˙ r ( f ) ) ( x ) .

To estimate g ˙ r ( ( b ( ) b B ) f 1 ) , take s r . From Hölder inequality, (2.1) and (2.2), it follows that

(3.5) 1 μ ( 6 B ) B g ˙ r ( ( b ( ) b B ) f 1 ) ( x ) d μ ( x ) 1 [ μ ( 6 B ) ] 1 s B g ˙ r ( ( b ( ) b B ) f 1 ) ( x ) s d μ ( x ) 1 s C [ μ ( 6 B ) ] 1 s ( b ( ) b B ) f 1 L s ( μ ) C 1 μ ( 6 B ) 6 B b ( y ) b B s s d μ ( y ) 1 s s 1 μ ( 6 B ) 6 B f ( y ) s s d μ ( y ) 1 s s C b RBMO ( μ ) M r , 6 ( f ) ( x ) .

Together with the aforementioned estimates, to get (3.2), we still need to estimate the difference g ˙ r ( ( b ( ) b B ) f 2 ) h B . For all y 1 , y 2 B , write

g ˙ r ( ( b ( ) b B ) f 2 ) ( y 1 ) h B 1 μ ( B ) B k Z X D k ( y 1 , z ) ( b ( z ) b B ) f 2 ( z ) d μ ( z ) r 1 r k Z X D k ( y 2 , z ) ( b ( z ) b B ) f 2 ( z ) d μ ( z ) r 1 r d μ ( y 2 ) 1 μ ( B ) B k Z X ( D k ( y 1 , z ) D k ( y 2 , z ) ) ( b ( z ) b B ) f 2 ( z ) d μ ( z ) r 1 r d μ ( y 2 ) ,

therefore, we only consider

k Z X ( D k ( y 1 , z ) D k ( y 2 , z ) ) ( b ( z ) b B ) f 2 ( z ) d μ ( z ) r 1 r .

From Fubini-Tonelli theorem, Hölder inequality, (1.1), (1.6) and (2.2), it follows that

(3.6) k Z X ( D k ( y 1 , z ) D k ( y 2 , z ) ) ( b ( z ) b B ) f 2 ( z ) d μ ( z ) r 1 r X 6 B k Z D k ( y 1 , z ) D k ( y 2 , z ) r b ( z ) b B r f ( z ) r d μ ( z ) 1 r C i = H B y 1 3 Q y 1 , i Q y 1 , i + 1 d ( y 1 , y 2 ) r ( Q y 1 , i ) r ε b ( z ) b B r f ( z ) r [ λ ( y 1 , d ( y 1 , z ) ) ] r d μ ( z ) 1 r + C Q y 1 , H B y 1 2 6 B b ( z ) b B r f ( z ) r [ λ ( y 1 , d ( y 1 , z ) ) ] r d μ ( z ) 1 r C i = 3 Q y 1 , H B y 1 i Q y 1 , H B y 1 i + 1 r ( B ) r ( Q y 1 , H B y 1 i + 3 ) r ε b ( z ) b B r f ( z ) r [ λ ( y 1 , d ( y 1 , z ) ) ] r d μ ( z ) 1 r + C Q y 1 , H B y 1 2 6 B b ( z ) b B r f ( z ) r [ λ ( y 1 , d ( y 1 , z ) ) ] r d μ ( z ) 1 r C i = 3 r ( B ) r ( Q y 1 , H B y 1 i + 3 ) r ε 1 [ λ ( y 1 , r ( Q y 1 , H B y 1 i + 1 ) ) ] r Q y 1 , H B y 1 i b ( z ) b B r f ( z ) r d μ ( z ) 1 r + C λ ( y 1 , r ( 6 B ) ) Q y 1 , H B y 1 2 b ( z ) b B r f ( z ) r d μ ( z ) 1 r

C i = 3 r ( B ) r ( Q y 1 , H B y 1 i + 3 ) r ε 1 [ λ ( y 1 , r ( Q y 1 , H B y 1 i + 1 ) ) ] r × Q y 1 , H B y 1 i b ( z ) b Q y 1 , H B y 1 i r f ( z ) r d μ ( z ) + b B b Q y 1 , H B y 1 i r Q y 1 , H B y 1 i f ( z ) r d μ ( z ) 1 r + C λ ( y 1 , r ( 6 B ) ) b Q y 1 , H B y 1 2 b B r Q y 1 , H B y 1 2 f ( z ) r d μ ( z ) + Q y 1 , H B y 1 2 b ( z ) b Q y 1 , H B y 1 2 r f ( z ) r d μ ( z ) 1 r C i = 3 1 1 0 ( r ( i 3 ) ε ) 1 [ λ ( y 1 , r ( Q y 1 , H B y 1 i + 1 ) ) ] r b RBMO ( μ ) r [ μ ( 6 Q y 1 , H B y 1 i ) ] M r 2 , 6 r ( f ) ( x ) + i r b RBMO ( μ ) r [ μ ( 6 Q y 1 , H B y 1 i ) ] M r , 6 r ( f ) ( x ) 1 r + C λ ( y 1 , r ( 6 B ) ) { b RBMO ( μ ) r [ μ ( 6 Q y 1 , H B y 1 2 ) ] M r , 6 r ( f ) ( x ) + b RBMO ( μ ) r [ μ ( 6 Q y 1 , H B y 1 i ) ] M r 2 , 6 r ( f ) ( x ) } 1 r C b RBMO ( μ ) { M r 2 , 6 ( f ) ( x ) + M r , 6 ( f ) ( x ) } ,

where H B y 1 represents the largest integer k satisfying B B y 1 , k for any ball B and y 1 B supp ( μ ) . Moreover, we also need some known facts proved in [10].

X 6 B = i = 3 ( Q y 2 , H B y 1 i Q y 2 , H B y 1 i + 1 ) ( Q y 2 , H B y 1 i + 1 6 B )

and, for all y 1 , y 2 B and z X Q y 2 , H B y 1 2 ,

k Z D k ( y 1 , z ) D k ( y 2 , z ) r C d ( y 1 , y 2 ) r ( Q y 1 , H B y 1 i + 3 ) r ε 1 [ λ ( y 1 , d ( y 1 , z ) ) ] r .

Combining the estimates for (3.4), (3.5) and (3.6), we get (3.2).

Now, we show the condition (3.3). Consider two balls B , S X satisfying B S and x B , and let N N B , S + 1 . Write

h B h S m B ( g ˙ r ( ( b b S ) f χ 6 N B 6 B ) ) + m S ( g ˙ r ( ( b b S ) f χ 6 N B 6 S ) ) + m B ( g ˙ r ( ( b b S ) f χ X 6 N B ) ) m S ( g ˙ r ( ( b b S ) f χ X 6 N B ) ) + m B ( g ˙ r ( ( b S b B ) f χ X 6 B ) ) E 1 + E 2 + E 3 + E 4 .

With an argument similar to that used in the estimate of (3.6), it is easy to see that

E 3 C b RBMO ( μ ) { M r 2 , 6 ( f ) ( x ) + M r , 6 ( f ) ( x ) } .

For y B , by applying Fubini-Tonelli Theorem, Minkowski inequality, Hölder inequality and (2.2), we can deduce that

E 1 1 μ ( B ) B g ˙ r ( ( b b S ) f χ 6 N B 6 B ) ( y ) d μ ( y ) 1 μ ( B ) B 6 N B 6 B k Z D ( y , z ) r b ( z ) b S r f ( z ) r d μ ( z ) 1 r d μ ( y )

1 μ ( B ) 6 N B 6 B B k Z D ( y , z ) r 1 r d μ ( y ) b ( z ) b S f ( z ) d μ ( z ) C j = 1 N 1 6 j + 1 B 6 j B b ( z ) b S λ ( c ( B ) , d ( c ( B ) , z ) ) f ( z ) d μ ( z ) C j = 1 N 1 1 λ ( c ( B ) , 6 j r B ) 6 j + 1 B b ( z ) b 6 j + 1 B f ( z ) d μ ( z ) + b 6 j + 1 B b S 6 j + 1 B f ( z ) d μ ( z ) C K B , S b RBMO ( μ ) M r , 6 ( f ) ( x ) j = 1 N 1 μ ( 6 j + 1 B ) λ ( c ( B ) , 6 j r ( B ) ) C K B , S b RBMO ( μ ) M r , 6 ( f ) ( x ) .

Similarly, it follows that E 2 C K B , S b RBMO ( μ ) M r , 6 ( f ) ( x ) .

Now, let us estimate E 4 . For any y B , from (1.5), Fubini-Tonelli Theorem, Minkowski inequality and Hölder inequality, we have

1 μ ( B ) B g ˙ r ( ( b B b S ) f χ X 6 B ) ( y ) d μ ( y ) C K B , S b RBMO ( μ ) 1 μ ( B ) B g ˙ r ( f χ X 6 B ) ( y ) d μ ( y ) + B g ˙ r ( f χ 6 B ) ( y ) d μ ( y ) C K B , S b RBMO ( μ ) { M r , 6 ( g ˙ ( f ) ) ( x ) + M r , 6 ( f ) ( x ) } .

Proof of Theorem 1.10

By applying Lemma 2.3 and (3.1), it is obvious to see that

[ b , g ˙ r ] ( f ) L 1 , ( μ ) N ( [ b , g ˙ r ] ( f ) ) L 1 , ( μ ) C M ( [ b , g ˙ r ] ( f ) ) L 1 , ( μ ) C b RBMO ( μ ) { M r , 6 ( g ˙ r ( f ) ) L 1 , ( μ ) + M r 2 , 6 ( f ) L 1 , ( μ ) + M r , 6 ( f ) L 1 , ( μ ) } C b RBMO ( μ ) f L 1 ( μ ) ,

which is the desired result.□

Proof of Theorem 1.11

By applying (2.4), (3.1) and Theorem 14 (see [9]), we have

[ b , g ˙ r ] ( f ) M q p ( μ ) N ( [ b , g ˙ r ] ( f ) ) M q p ( μ ) C M ( [ b , g ˙ r ] ( f ) ) M q p ( μ ) C b RBMO ( μ ) { M r , 6 ( g ˙ r ( f ) ) M q p ( μ ) + M r 2 , 6 ( f ) M q p ( μ ) + M r , 6 ( f ) M q p ( μ ) } C b RBMO ( μ ) f M q p ( μ ) .

Proof of Theorem 1.12

From Remark 1.7 (1), we assume k = 6 in (1.8). By applying Definition 1.6, Lemma 2.3 (2), Theorem 4.2 in [15] and (3.1), we can deduce that

[ b , g ˙ r ] ( f ) L p , ϕ ( μ ) sup B C [ ϕ ( μ ( 6 B ) ) ] 1 p N ( [ b , g ˙ r ] ( f ) ) L p ( μ , B ) sup B C [ ϕ ( μ ( 6 B ) ) ] 1 p M ( [ b , g ˙ r ] ( f ) ) L p ( μ , B ) C b RBMO ( μ ) { M r , 6 ( g ˙ r ( f ) ) L p , ϕ ( μ ) + M r 2 , 6 ( f ) L p , ϕ ( μ ) + M r , 6 ( f ) L p , ϕ ( μ ) } C b RBMO ( μ ) f L p , ϕ ( μ ) .

  1. Funding information: This research was supported by the Scientific Startup Foundation for Doctors of Northwest Normal University (0002020203), Young Teachers’ Scientific Research Ability Promotion Project of Northwest Normal University (NWNU-LKQN2020-07) and Innovation Fund Project for Higher Education of Gansu Province (2020A-010).

  2. Conflict of interest: Author states no conflict of interest.

References

[1] Y. Sawano , Generalized Morrey spaces for non-doubling measures, Nonlinear Differ. Equ. Appl. 15 (2008), no. 4–5, 413–425, https://doi.org/10.1007/s00030-008-6032-5. Search in Google Scholar

[2] Y. Sawano and H. Tanaka , Morrey spaces for non-doubling measures, Acta Math. Sin. (Engl. Ser.) 21 (2005), no. 6, 1535–1544, https://doi.org/10.1007/s10114-005-0660-z. Search in Google Scholar

[3] X. Tolsa , Littlewood-Paley theory and the T(1) theorem with non-doubling measures, Adv. Math. 164 (2001), no. 1, 57–116, https://doi.org/10.1006/aima.2001.2011. Search in Google Scholar

[4] X. Tolsa , BMO, H1 , and Calderón-Zygmund operators for non-doubling measures, Math. Ann. 319 (2001), no. 1, 89–149, https://doi.org/10.1007/PL00004432. Search in Google Scholar

[5] G. Lu and J. Zhou , Estimates for fractional type Marcinkiewicz integrals with non-doubling measures, J. Inequal. Appl. 2014 (2014), 285, https://doi.org/10.1186/1029-242X-2014-285. Search in Google Scholar

[6] R. R. Coifman and G. Weiss , Analyse Harmonique Non-commutative sur Certains Espaces Homogènes, Springer-Verlag, Berlin-New York, 1971. 10.1007/BFb0058946Search in Google Scholar

[7] R. R. Coifman and G. Weiss , Extensions of Hardy spaces and their use in analysis, Bull. Amer. Math. Soc. 83 (1977), no. 4, 569–645, https://doi.org/10.1090/S0002-9904-1977-14325-5. Search in Google Scholar

[8] T. Hytönen , A framework for non-homogeneous analysis on metric spaces, and the RBMO space of Tolsa, Publ. Mat. 54 (2010), no. 2, 485–504, https://doi.org/10.5565/PUBLMAT_54210_10. Search in Google Scholar

[9] Y. Cao and J. Zhou , Morrey spaces for nonhomogeneous metric measure spaces, Abstr. Appl. Anal. 2013 (2013), 196459, https://doi.org/10.1155/2013/196459. Search in Google Scholar

[10] X. Fu and J. Zhao , Endpoint estimates of generalized homogeneous Littlewood-Paley g -functions over non-homogeneous metric measure spaces, Acta Math. Sin. (Engl. Ser.) 32 (2016), no. 9, 1035–1074, https://doi.org/10.1007/s10114-016-5059-5. Search in Google Scholar

[11] G. Lu and S. Tao , Generalized homogeneous Littlewood-Paley g -function on some function spaces, Bull. Malay. Math. Sci. Soc. 44 (2021), no. 1, 17–34, https://doi.org/10.1007/s40840-020-00934-7. Search in Google Scholar

[12] T. Hytönen , D. Yang , and D. Yang , The Hardy space H1 on non-homogeneous metric measure spaces, Math. Proc. Cambridge Philos. Soc. 153 (2012), no. 1, 9–31, https://doi.org/10.1017/S0305004111000776. Search in Google Scholar

[13] C. Tan and J. Li , Littlewood-Paley theory on metric spaces with non-doubling measures and its applications, Sci. China Math. 58 (2015), no. 5, 983–1004, https://doi.org/10.1007/s11425-014-4950-8. Search in Google Scholar

[14] G. Lu and S. Tao , Generalized Morrey spaces over non-homogeneous metric measure spaces, J. Aust. Math. Soc. 103 (2017), no. 2, 268–278, https://doi.org/10.1017/S1446788716000483. Search in Google Scholar

[15] T. A. Bui and X. T. Duong , Hardy spaces, regularized BMO spaces and the boundedness of Calderón-Zygmund operators on non-homogeneous spaces, J. Geom. Anal. 23 (2013), no. 2, 895–932, https://doi.org/10.1007/s12220-011-9268-y. Search in Google Scholar

[16] X. Fu , D. Yang , and W. Yuan , Generalized fractional integral and their commutators over non-homogeneous metric measure spaces, Taiwanese J. Math. 18 (2014), no. 2, 509–557, https://doi.org/10.11650/tjm.18.2014.3651. Search in Google Scholar

[17] G.-H. Lu , Commutator of bilinear θ -type Calderón-Zygmund operator on Morrey space over non-homogeneous metric measure spaces, Anal. Math. 46 (2020), no. 1, 97–118, https://doi.org/10.1007/s10476-020-0020-3. Search in Google Scholar

[18] G. Lu and S. Tao , Commutators of Littlewood-Paley gκ∗ -functions on non-homogeneous metric measure spaces, Open Math. 15 (2017), no. 1, 1283–1299, https://doi.org/10.1515/math-2017-0110. Search in Google Scholar

[19] Y. Zhao , H. Lin , and Y. Meng , Endpoint estimates for multilinear fractional integral operators on metric measure spaces, Ann. Funct. Anal. 10 (2019), no. 3, 337–349, https://doi.org/10.1215/20088752-2018-0033. Search in Google Scholar

Received: 2020-03-07
Revised: 2021-03-01
Accepted: 2021-05-30
Published Online: 2021-08-27

© 2021 Guanghui Lu, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

Articles in the same Issue

  1. Regular Articles
  2. Sharp conditions for the convergence of greedy expansions with prescribed coefficients
  3. Range-kernel weak orthogonality of some elementary operators
  4. Stability analysis for Selkov-Schnakenberg reaction-diffusion system
  5. On non-normal cyclic subgroups of prime order or order 4 of finite groups
  6. Some results on semigroups of transformations with restricted range
  7. Quasi-ideal Ehresmann transversals: The spined product structure
  8. On the regulator problem for linear systems over rings and algebras
  9. Solvability of the abstract evolution equations in Ls-spaces with critical temporal weights
  10. Resolving resolution dimensions in triangulated categories
  11. Entire functions that share two pairs of small functions
  12. On stochastic inverse problem of construction of stable program motion
  13. Pentagonal quasigroups, their translatability and parastrophes
  14. Counting certain quadratic partitions of zero modulo a prime number
  15. Global attractors for a class of semilinear degenerate parabolic equations
  16. A new implicit symmetric method of sixth algebraic order with vanished phase-lag and its first derivative for solving Schrödinger's equation
  17. On sub-class sizes of mutually permutable products
  18. Asymptotic solution of the Cauchy problem for the singularly perturbed partial integro-differential equation with rapidly oscillating coefficients and with rapidly oscillating heterogeneity
  19. Existence and asymptotical behavior of solutions for a quasilinear Choquard equation with singularity
  20. On kernels by rainbow paths in arc-coloured digraphs
  21. Fully degenerate Bell polynomials associated with degenerate Poisson random variables
  22. Multiple solutions and ground state solutions for a class of generalized Kadomtsev-Petviashvili equation
  23. A note on maximal operators related to Laplace-Bessel differential operators on variable exponent Lebesgue spaces
  24. Weak and strong estimates for linear and multilinear fractional Hausdorff operators on the Heisenberg group
  25. Partial sums and inclusion relations for analytic functions involving (p, q)-differential operator
  26. Hodge-Deligne polynomials of character varieties of free abelian groups
  27. Diophantine approximation with one prime, two squares of primes and one kth power of a prime
  28. The equivalent parameter conditions for constructing multiple integral half-discrete Hilbert-type inequalities with a class of nonhomogeneous kernels and their applications
  29. Boundedness of vector-valued sublinear operators on weighted Herz-Morrey spaces with variable exponents
  30. On some new quantum midpoint-type inequalities for twice quantum differentiable convex functions
  31. Quantum Ostrowski-type inequalities for twice quantum differentiable functions in quantum calculus
  32. Asymptotic measure-expansiveness for generic diffeomorphisms
  33. Infinitesimals via Cauchy sequences: Refining the classical equivalence
  34. The (1, 2)-step competition graph of a hypertournament
  35. Properties of multiplication operators on the space of functions of bounded φ-variation
  36. Disproving a conjecture of Thornton on Bohemian matrices
  37. Some estimates for the commutators of multilinear maximal function on Morrey-type space
  38. Inviscid, zero Froude number limit of the viscous shallow water system
  39. Inequalities between height and deviation of polynomials
  40. New criteria-based ℋ-tensors for identifying the positive definiteness of multivariate homogeneous forms
  41. Determinantal inequalities of Hua-Marcus-Zhang type for quaternion matrices
  42. On a new generalization of some Hilbert-type inequalities
  43. On split quaternion equivalents for Quaternaccis, shortly Split Quaternaccis
  44. On split regular BiHom-Poisson color algebras
  45. Asymptotic stability of the time-changed stochastic delay differential equations with Markovian switching
  46. The mixed metric dimension of flower snarks and wheels
  47. Oscillatory bifurcation problems for ODEs with logarithmic nonlinearity
  48. The B-topology on S-doubly quasicontinuous posets
  49. Hyers-Ulam stability of isometries on bounded domains
  50. Inhomogeneous conformable abstract Cauchy problem
  51. Path homology theory of edge-colored graphs
  52. Refinements of quantum Hermite-Hadamard-type inequalities
  53. Symmetric graphs of valency seven and their basic normal quotient graphs
  54. Mean oscillation and boundedness of multilinear operator related to multiplier operator
  55. Numerical methods for time-fractional convection-diffusion problems with high-order accuracy
  56. Several explicit formulas for (degenerate) Narumi and Cauchy polynomials and numbers
  57. Finite groups whose intersection power graphs are toroidal and projective-planar
  58. On primitive solutions of the Diophantine equation x2 + y2 = M
  59. A note on polyexponential and unipoly Bernoulli polynomials of the second kind
  60. On the type 2 poly-Bernoulli polynomials associated with umbral calculus
  61. Some estimates for commutators of Littlewood-Paley g-functions
  62. Construction of a family of non-stationary combined ternary subdivision schemes reproducing exponential polynomials
  63. On the evolutionary bifurcation curves for the one-dimensional prescribed mean curvature equation with logistic type
  64. On intersections of two non-incident subgroups of finite p-groups
  65. Global existence and boundedness in a two-species chemotaxis system with nonlinear diffusion
  66. Finite groups with 4p2q elements of maximal order
  67. Positive solutions of a discrete nonlinear third-order three-point eigenvalue problem with sign-changing Green's function
  68. Power moments of automorphic L-functions related to Maass forms for SL3(ℤ)
  69. Entire solutions for several general quadratic trinomial differential difference equations
  70. Strong consistency of regression function estimator with martingale difference errors
  71. Fractional Hermite-Hadamard-type inequalities for interval-valued co-ordinated convex functions
  72. Montgomery identity and Ostrowski-type inequalities via quantum calculus
  73. Universal inequalities of the poly-drifting Laplacian on smooth metric measure spaces
  74. On reducible non-Weierstrass semigroups
  75. so-metrizable spaces and images of metric spaces
  76. Some new parameterized inequalities for co-ordinated convex functions involving generalized fractional integrals
  77. The concept of cone b-Banach space and fixed point theorems
  78. Complete consistency for the estimator of nonparametric regression model based on m-END errors
  79. A posteriori error estimates based on superconvergence of FEM for fractional evolution equations
  80. Solution of integral equations via coupled fixed point theorems in 𝔉-complete metric spaces
  81. Symmetric pairs and pseudosymmetry of Θ-Yetter-Drinfeld categories for Hom-Hopf algebras
  82. A new characterization of the automorphism groups of Mathieu groups
  83. The role of w-tilting modules in relative Gorenstein (co)homology
  84. Primitive and decomposable elements in homology of ΩΣℂP
  85. The G-sequence shadowing property and G-equicontinuity of the inverse limit spaces under group action
  86. Classification of f-biharmonic submanifolds in Lorentz space forms
  87. Some new results on the weaving of K-g-frames in Hilbert spaces
  88. Matrix representation of a cross product and related curl-based differential operators in all space dimensions
  89. Global optimization and applications to a variational inequality problem
  90. Functional equations related to higher derivations in semiprime rings
  91. A partial order on transformation semigroups with restricted range that preserve double direction equivalence
  92. On multi-step methods for singular fractional q-integro-differential equations
  93. Compact perturbations of operators with property (t)
  94. Entire solutions for several complex partial differential-difference equations of Fermat type in ℂ2
  95. Random attractors for stochastic plate equations with memory in unbounded domains
  96. On the convergence of two-step modulus-based matrix splitting iteration method
  97. On the separation method in stochastic reconstruction problem
  98. Robust estimation for partial functional linear regression models based on FPCA and weighted composite quantile regression
  99. Structure of coincidence isometry groups
  100. Sharp function estimates and boundedness for Toeplitz-type operators associated with general fractional integral operators
  101. Oscillatory hyper-Hilbert transform on Wiener amalgam spaces
  102. Euler-type sums involving multiple harmonic sums and binomial coefficients
  103. Poly-falling factorial sequences and poly-rising factorial sequences
  104. Geometric approximations to transition densities of Jump-type Markov processes
  105. Multiple solutions for a quasilinear Choquard equation with critical nonlinearity
  106. Bifurcations and exact traveling wave solutions for the regularized Schamel equation
  107. Almost factorizable weakly type B semigroups
  108. The finite spectrum of Sturm-Liouville problems with n transmission conditions and quadratic eigenparameter-dependent boundary conditions
  109. Ground state sign-changing solutions for a class of quasilinear Schrödinger equations
  110. Epi-quasi normality
  111. Derivative and higher-order Cauchy integral formula of matrix functions
  112. Commutators of multilinear strongly singular integrals on nonhomogeneous metric measure spaces
  113. Solutions to a multi-phase model of sea ice growth
  114. Existence and simulation of positive solutions for m-point fractional differential equations with derivative terms
  115. Bernstein-Walsh type inequalities for derivatives of algebraic polynomials in quasidisks
  116. Review Article
  117. Semiprimeness of semigroup algebras
  118. Special Issue on Problems, Methods and Applications of Nonlinear Analysis (Part II)
  119. Third-order differential equations with three-point boundary conditions
  120. Fractional calculus, zeta functions and Shannon entropy
  121. Uniqueness of positive solutions for boundary value problems associated with indefinite ϕ-Laplacian-type equations
  122. Synchronization of Caputo fractional neural networks with bounded time variable delays
  123. On quasilinear elliptic problems with finite or infinite potential wells
  124. Deterministic and random approximation by the combination of algebraic polynomials and trigonometric polynomials
  125. On a fractional Schrödinger-Poisson system with strong singularity
  126. Parabolic inequalities in Orlicz spaces with data in L1
  127. Special Issue on Evolution Equations, Theory and Applications (Part II)
  128. Impulsive Caputo-Fabrizio fractional differential equations in b-metric spaces
  129. Existence of a solution of Hilfer fractional hybrid problems via new Krasnoselskii-type fixed point theorems
  130. On a nonlinear system of Riemann-Liouville fractional differential equations with semi-coupled integro-multipoint boundary conditions
  131. Blow-up results of the positive solution for a class of degenerate parabolic equations
  132. Long time decay for 3D Navier-Stokes equations in Fourier-Lei-Lin spaces
  133. On the extinction problem for a p-Laplacian equation with a nonlinear gradient source
  134. General decay rate for a viscoelastic wave equation with distributed delay and Balakrishnan-Taylor damping
  135. On hyponormality on a weighted annulus
  136. Exponential stability of Timoshenko system in thermoelasticity of second sound with a memory and distributed delay term
  137. Convergence results on Picard-Krasnoselskii hybrid iterative process in CAT(0) spaces
  138. Special Issue on Boundary Value Problems and their Applications on Biosciences and Engineering (Part I)
  139. Marangoni convection in layers of water-based nanofluids under the effect of rotation
  140. A transient analysis to the M(τ)/M(τ)/k queue with time-dependent parameters
  141. Existence of random attractors and the upper semicontinuity for small random perturbations of 2D Navier-Stokes equations with linear damping
  142. Degenerate binomial and Poisson random variables associated with degenerate Lah-Bell polynomials
  143. Special Issue on Fractional Problems with Variable-Order or Variable Exponents (Part I)
  144. On the mixed fractional quantum and Hadamard derivatives for impulsive boundary value problems
  145. The Lp dual Minkowski problem about 0 < p < 1 and q > 0
Downloaded on 8.9.2025 from https://www.degruyterbrill.com/document/doi/10.1515/math-2021-0051/html
Scroll to top button