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The dimension-free estimate for the truncated maximal operator

  • Xudong Nie and Panwang Wang EMAIL logo
Published/Copyright: November 25, 2022

Abstract

We mainly study the dimension-free L p -inequality of the truncated maximal operator

M n a f ( x ) = sup t > 0 1 B a 1 B a 1 f ( x t y ) d y ,

where B a 1 = { x : a x 1 } . When 0 a < 1 , we prove that M n a L p ( R n ) C ( p ) f L p ( R n ) for p > n / ( n 1 ) . When a = 1 , we prove that M n 1 L p ( R n ) C ( p ) f L p ( R n ) for p 2 .

MSC 2010: 42B20; 42B25

1 Introduction

Let f S ( R n ) be a rapidly decreasing function defined on R n . For 0 a < 1 , define the truncated maximal operator

M n a f ( x ) = sup t > 0 1 B a 1 B a 1 f ( x t y ) d y ,

where B a 1 { x : a x 1 } and B a 1 denote the volume of B a 1 . Conveniently, we denote the unite sphere S n 1 by B 1 1 . Define

M n 1 f ( x ) = sup t > 0 1 B 1 1 B 1 1 f ( x t y ) d σ ( y ) ,

where d σ ( y ) denotes the usual measure of the unite sphere and B 1 1 denotes its total mass. Obviously, M n 0 is the Hardy-Littlewood maximal operator and M n 1 is the sphere maximal operator. We mainly study the dimension-free L p -boundedness of the truncated maximal operators M n a for 0 a 1 . Stein first studied the sphere maximal operator M n 1 . In [1], he pointed out that if p > n / ( n 1 ) , then

M n 1 f L p ( R n ) C ( p , n ) f L p ( R n ) ,

where C ( p , n ) denotes a constant depending on p and n . The case for n = 2 was proved by Bourgain [2]. Later many authors tried to generalize the spherical maximal function to other hyper-surface. In [3], Sogge and Stein pointed out that if the Gaussian curvature of S does not vanish of infinite order at each point of S , then there exists a 2 < P 0 ( S ) < such that the corresponding surface maximal operator is strongly L p -bounded for p > p 0 ( S ) . Moreover, when the surface has at least one non-vanishing principal curvature everywhere in R n , then the maximal operator maps L p to L p for p > 2 [4]. More related works can be seen in [5,6, 7,8,9, 10,11,12, 13,14] and the references therein.

When a = 0 , M n a is the classical Hardy-Littlewood maximal operator. According to the result of [1], Stein [15] obtained that there exists a constant C ( p ) independent of n such that

(1) M n 0 f L p ( R n ) C ( p ) f L p ( R n )

for p > 1 . Analogously, many authors turned to focus on generalizing the dimension-free estimate for the maximal function to the general case. Bourgain [16] studied the maximal operator over central symmetric convex sets and obtained a similar result as (1) for p = 2 . Later, Bourgain [17] and Carbery [18] generalized this result for all p > 3 / 2 in different ways independently. For some special convex set such as q -balls, 1 q < , Müller [19] extended the L p bound to every p > 1 . Recently, Bourgain [20] showed that the strong type constant can be bounded by a constant, which is independent of the dimension for the Hardy-Littlewood maximal operator over cubes for all p > 1 . In this article, we will study the dimension-free estimate of the truncated maximal operator M n a , generalizing the results of Hardy-Littlewood maximal operators and sphere maximal operators proved in [1].

Theorem 1.1

Let f S ( R n ) . If 0 a < 1 , then there exists a constant C ( p ) independent of n and a such that

M n a f L p ( R n ) ( 1 a ) 1 C ( p ) f L p ( R n ) ,

for p > 1 . When p > n / ( n 1 ) ,

M n a f L p ( R n ) C ( p ) f L p ( R n ) .

If a = 1 , then

(2) M n 1 f L p ( R n ) C ( p ) f L p ( R n ) ,

for p 2 .

2 The proof of main theorem for the case a = 1

By interpolation theorem, we only need to prove the case p = 2 . This result follows from the general L 2 -estimate on convolution maximal operators obtained by Bourgain [16].

Lemma 2.1

Let K S ( R n ) be a tempered distribution. Suppose K ^ L ( R n ) and is differentiable. Define the following quantities:

α j = sup 2 j ξ 2 j + 1 K ^ ( ξ ) and β j = sup 2 j ξ 2 j + 1 K ^ ( ξ ) , ξ .

for j Z . Then,

sup t > 0 f K t L 2 ( R n ) C Γ ( K ) f L 2 ( R n ) ,

where

Γ ( K ) = j Z α j 1 / 2 ( α j + β j ) 1 / 2 .

Let M = 1 B n 1 d σ ( y ) and m ( ξ ) is the Fourier transform of M , where d σ ( y ) is the usual measure of unite sphere. Then,

m ( ξ ) = Γ n 2 π 1 2 Γ n 1 2 1 1 e 2 π i s ξ ( 1 s 2 ) n 3 2 d s ,

and

M n 1 f ( x ) = sup t > 0 R n f M t ( x ) .

Let P t ( t > 0 ) be the Poisson-semigroup on R n satisfying P t ^ ( ξ ) = e t ξ . To derive (2), we take K ^ ( ξ ) = m ( ξ ) e n 1 2 ξ . Stein [15] showed that there exists a constant C p independent of dimension n , such that

sup t > 0 P t f L p ( R n ) C p f L p ( R n )

for all p > 1 . So it is sufficient to prove that

(3) sup t > 0 K t f L 2 ( R n ) C f L 2 ( R n ) .

To use Lemma 2.1, we will study the asymptotic properties of K ( ) . Suppose n 3 , we give three estimates about m ( ξ ) .

Firstly, when ξ is large enough, we have

(4) m ( ξ ) = Γ n 2 π 1 2 Γ n 1 2 1 2 π ξ 1 1 e 2 π i s ξ d d s ( 1 s 2 ) n 3 2 d s Γ n 2 π 1 2 Γ n 1 2 1 2 π ξ 1 1 d d s ( 1 s 2 ) n 3 2 d s C n 1 2 ξ 1 .

When ξ is small enough, we obtain

(5) m ( ξ ) 1 = Γ n 2 π 1 2 Γ n 1 2 1 1 ( e 2 π i s ξ 1 ) ( 1 s 2 ) n 3 2 d s Γ n 2 π 1 2 Γ n 1 2 2 π ξ 1 1 s ( 1 s 2 ) n 3 2 d s C n 1 2 ξ .

Finally, we obtain

(6) m ( ξ ) , ξ = Γ n 2 π 1 2 Γ n 1 2 1 1 e 2 π i s ξ ( 2 π i s ξ ) ( 1 s 2 ) n 3 2 d s = Γ n 2 π 1 2 Γ n 1 2 1 1 e 2 π i s ξ d d s s ( 1 s 2 ) n 3 2 d s C n 1 2 0 1 d d s s ( 1 s 2 ) n 3 2 d s C .

It is easy to know that

e n 1 2 ξ 1 n 1 2 ξ ,

e n 1 2 ξ n 1 2 ξ 1 ,

and

e n 1 2 ξ , ξ C .

Combining these two inequalities with (4)–(6), we have

K ^ ( ξ ) C n 1 2 ξ 1 ,

K ^ ( ξ ) C n 1 2 ξ ,

and

< K ^ ( ξ ) , ξ > C .

According to three inequalities mentioned earlier and Lemma 2.1, we obtain

sup t > 0 f K t L 2 ( R n ) C f L 2 ( R n ) .

3 The proof of main theorem for the case 0 < a < 1

For 0 a < 1 , we have

(7) M n a f ( x ) = sup t > 0 1 B a 1 B a 1 f ( x t y ) d y B 0 1 B a 1 sup t > 0 1 B 0 1 B 0 1 f ( x t y ) d y 1 1 a M n 0 ( f ) ( x ) .

It follows from (1) and (7) that

M a f L p ( R n ) 1 1 a C ( p ) f L p ( R n ) .

The general case has been proved. It remains to consider the special case p > n / ( n 1 ) . We introduce the following operator:

M n , m a f ( x ) = sup t > 0 a y 1 f ( x t y ) y m d y a y 1 y m d y .

Noting that

(8) a y 1 f ( x t y ) y m d y a y 1 y m d y = a 1 S n 1 f ( x t ρ θ ) ρ m + n 1 d θ d ρ a 1 S n 1 ρ n + m 1 d θ d ρ .

It implies

M n , m a f ( x ) M n 1 ( f ) ( x ) .

From this, it follows that

(9) M n , m a f L p ( R n ) C ( p , n ) f L p ( R n ) .

For τ O ( n ) , define

M k , τ a f ( x ) = sup t > 0 a y 1 1 f ( x t τ ( y 1 , 0 ) ) y 1 n k d y 1 a y 1 1 y 1 n k d y 1 ,

where ( y 1 , 0 ) R k × R n k . Then

M k , τ a f ( x ) = sup t > 0 a y 1 1 f τ ( τ 1 x t ( y 1 , 0 ) ) y 1 n k d y 1 a y 1 1 y 1 n k d y 1 = M n , k a f τ ( τ 1 x ) ,

where f τ ( ) = f ( τ ) . Hence,

(10) M k , τ a f L p ( R n ) A ( p , k ) f L p ( R n ) .

Since

1 B a 1 B a 1 f ( x t y ) d y = a y 1 f ( x t y ) d y a y 1 d y = O ( n ) a y 1 1 f ( x t τ ( y 1 , 0 ) ) y 1 n k d y 1 d τ O ( n ) a y 1 1 y 1 n k d y 1 d τ ,

we obtain

(11) M n a f ( x ) O ( n ) M k , τ a ( f ) ( x ) d τ ,

where d τ is the normalized Harr measure on the orthogonal group O ( n ) .

It follows from (10) and (11) that

(12) M n a f L p ( R n ) A ( p , k ) f L p ( R n ) .

Since n > p / ( p 1 ) , we take k to be the smallest integer greater than p / ( p 1 ) . Our theorem follows from (12).

  1. Funding information: The research was supported by the Hebei Province introduced overseas student support projects (Grant No. C20190365).

  2. Author contributions: All authors contributed equally and significantly in writing this paper. All authors read and approved the final manuscript.

  3. Conflict of interest: The authors state no conflict of interests.

  4. Data availability statement: Not applicable

  5. Code availability: Not applicable

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Received: 2022-01-15
Revised: 2022-10-09
Accepted: 2022-11-08
Published Online: 2022-11-25

© 2022 the author(s), published by De Gruyter

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

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