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J. Korean Math. Soc. 44 (2007), No. 4, pp. 809–822

ENDPOINT ESTIMATES FOR MAXIMAL COMMUTATORS IN NON-HOMOGENEOUS SPACES

Guoen Hu, Yan Meng, and Dachun Yang

Reprinted from the

Journal of the Korean Mathematical Society Vol. 44, No. 4, July 2007

c

°2007 The Korean Mathematical Society

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ENDPOINT ESTIMATES FOR MAXIMAL COMMUTATORS IN NON-HOMOGENEOUS SPACES

Guoen Hu, Yan Meng, and Dachun Yang

Abstract. Certain weak type endpoint estimates are established for maximal commutators generated by Calder´ on-Zygmund operators and Osc

expLr

(µ) functions for r ≥ 1 under the condition that the under- lying measure only satisfies some growth condition, where the kernels of Calder´ on-Zgymund operators only satisfy the standard size condition and some H¨ ormander type regularity condition, and Osc

exp Lr

(µ) are the spaces of Orlicz type satisfying that Osc

exp Lr

(µ) = RBMO(µ) if r = 1 and Osc

exp Lr

(µ) ⊂ RBMO(µ) if r > 1.

1. Introduction

It is well known that the doubling condition of the underlying measure is a key assumption in the analysis on spaces of homogeneous type. We recall that µ is said to satisfy the doubling condition if there is a constant C > 0 such that µ (B(x, 2r)) ≤ Cµ (B(x, r)) for all x ∈ R d and r > 0, where B(x, r) = {y ∈ R d : |y − x| < r}. However, during the last several years, many classical results have been proved still valid if the underlying measure µ is a positive Radon measure on R d , which only satisfies the following growth condition that there exist constants C 0 > 0 and n ∈ (0, d] such that for all x ∈ R d and r > 0,

(1.1) µ (B(x, r)) ≤ C 0 r n ;

see [5, 6, 7, 10, 11, 12]. The Euclidean space R d equipped with a Radon measure that only satisfies (1.1) is called a non-homogeneous space since µ may not be doubling. The motivation for developing the analysis on non-homogeneous spaces and some examples of non-doubling measures can be found in [14]. We only point out that the analysis on non-homogeneous spaces played an essential role in solving the long-standing Painlev´e’s problem by Tolsa in [13].

Received January 11, 2006.

2000 Mathematics Subject Classification. Primary 47B47; Secondary 42B20, 43A99.

Key words and phrases. Calder´ on-Zygmund operator, Osc

expLr

(µ), maximal commuta- tor, endpoint estimate.

The third author was supported by Program for New Century Excellent Talents in Uni- versity (NCET-04-0142) of China.

c

°2007 The Korean Mathematical Society

809

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The purpose of this paper is to establish some weak type endpoint esti- mates for the maximal commutators associated to Calder´on-Zygmund opera- tors, whose kernels satisfy the standard size condition and some weaker regu- larity condition, with Osc expL

r

(µ) functions, where r ≥ 1. Before stating our results, we first recall some necessary notation and definitions.

Throughout this paper, by a cube Q ⊂ R d , we mean a closed cube whose sides are parallel to the axes and centered at some point of supp(µ), and we denote its side length by l(Q) and its center by x Q . Let α and β be positive constants such that α > 1 and β > α n . For a cube Q, we say that Q is (α, β)- doubling if µ(αQ) ≤ βµ(Q), where αQ denotes the cube concentric with Q and having side length αl(Q). In what follows, for definiteness, if α and β are not specified, by a doubling cube we mean a (2, 2 d+1 )-doubling cube. Especially, for any given cube Q, we denote by e Q the smallest doubling cube in the family {2 k Q} k≥0 . For two cubes Q 1 ⊂ Q 2 , set

K Q

1

, Q

2

= 1 +

N

Q1, Q2

X

k=1

µ(2 k Q 1 )

£ l(2 k Q 1 ) ¤ n ,

where N Q

1

, Q

2

is the first positive integer k such that l(2 k Q 1 ) ≥ l(Q 2 ); see [9]

for some basic properties of K Q

1

, Q

2

.

Definition. For r ≥ 1, a locally integrable function f is said to belong to the space Osc exp L

r

(µ) if there is a constant C 1 > 0 such that

(i) for any Q,

° °

°f − m Q e (f )

° °

° exp L

r

, Q

= inf

½

λ > 0 : 1 µ(2Q)

Z

Q

exp ³ |f − m Q e (f )|

λ

´ r dµ ≤ 2

¾

≤ C 1 ,

(ii) for any two doubling cubes Q 1 ⊂ Q 2 , |m Q

1

(f ) − m Q

2

(f )| ≤ C 1 K Q

1

, Q

2

, where m Q e (f ) is the mean value of f on e Q, namely, m Q e (f ) = µ( e 1 Q) R

Q e f (x) dµ(x).

The minimal constant C 1 satisfying (i) and (ii) is defined to be the Osc exp L

r

(µ) norm of f and denoted by kf k Osc

exp Lr

(µ) .

The space Osc exp L

r

(µ) is an analogy of the classical Osc exp L

r

(R d ) space which was introduced by P´erez and Trujillo-Gonz´alez in [8]. Obviously, for any r 2 > r 1 > 1, Osc exp L

r2

(µ) ⊂ Osc exp L

r1

(µ) ⊂ RBMO(µ). Moreover, from the John-Nirenberg inequality established by Tolsa in [9], it follows that Osc expL

1

(µ) is just the space RBMO(µ) of Tolsa in [9].

Let K ∈ L 1 loc (R d × R d \ {(x, y) : x = y}) and there exists a constant C > 0 such that for all x, y ∈ R d with x 6= y,

(1.2) |K(x, y)| ≤ C|x − y| −n ,

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and for all y, y 0 ∈ R d , (1.3)

Z

|x−y|≥2|y−y

0

|

{|K(x, y) − K(x, y 0 )|

+|K(y, x) − K(y 0 , x)|} dµ(x) ≤ C.

For any ² > 0, define the truncated operators T ² by (1.4) T ² (f )(x) =

Z

|x−y|>²

K(x, y)f (y) dµ(y), and the maximal Calder´on-Zygmund operator T by

(1.5) T (f )(x) = sup

²>0 |T ² (f )(x)| .

It is well known that if the operators T ² are bounded on L 2 (µ) uniformly for

² > 0, then there is an operator T which is the weak limit as ² → 0 of some subsequence of the uniformly bounded operators T ² . The operator T is also bounded on L 2 (µ) and satisfies that for f ∈ L 2 (µ) with suppf 6= R d , and almost all x ∈ R d \ supp f ,

T (f )(x) = Z

R

d

K(x, y)f (y) dµ(y).

For m ∈ N and b 1 , b 2 , . . . , b m ∈ RBMO(µ), define the multilinear commutator T ~b by

T ~b f (x) = [b m , [b m−1 , . . . , [b 1 , T ] · · ·]] (f )(x), where ~b = (b 1 , b 2 , . . . , b m ) and [b 1 , T ] is defined by

(1.6) [b 1 , T ](f )(x) = b 1 (x)T (f )(x) − T (b 1 f )(x).

For the case of m = 1, we denote T ~b simply by T b . When the kernel K satisfies the size condition (1.2) and the standard regularity condition: there exist two constants α ∈ (0, 1] and C > 0 such that for all x, y, y 0 ∈ R d with

|x − y| ≥ 2|y − y 0 | and x 6= y,

(1.7) |K(x, y) − K(x, y 0 )| + |K(y, x) − K(y 0 , x)| ≤ C |y − y 0 | α

|x − y| n+α , Tolsa [9] proved that if the operators T ² are bounded on L 2 (µ) uniformly for ² >

0, then T b is bounded on L p (µ) for any p ∈ (1, ∞). In [1], we generalized this result of Tolsa and proved that if K satisfies (1.2) and (1.7) and the operators T ² are bounded on L 2 (µ) uniformly for ² > 0, then for any m ∈ N, T ~b is also bounded on L p (µ) with p ∈ (1, ∞), and satisfies a weak type endpoint estimate, namely, there exists a constant C > 0 such that for all λ > 0 and all bounded functions f with compact support,

µ ³n

x ∈ R d : |T ~b (f )(x)| > λ

≤ Cϕ 1/r

³ Y m

i=1

kb i k Osc

exp Lri

(µ)

´ Z

R

d

ϕ 1/r

³ |f(x)|

λ

´

dµ(x),

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where C > 0 is a constant, 1/r = P m

i=1 1/r i and ϕ σ (t) = t log σ (2 + t) for σ, t > 0.

We now define the maximal commutator associated with the operator T ~b . For m ∈ N and b 1 , b 2 , . . . , b m ∈ RBMO(µ), the maximal commutator T ~b is defined by

(1.8) T ~b (f )(x) = sup

²>0

¯ ¯

¯T ²,~b (f )(x)

¯ ¯

¯

= sup

²>0

¯ ¯

¯ ¯

¯ Z

|x−y|>²

Y m i=1

[b i (x) − b i (y)]K(x, y)f (y)dµ(y)

¯ ¯

¯ ¯

¯ . Repeating the proof of Lemma 4.1 in [4], we can prove that if K satisfies (1.2) and the following H¨ormander-type condition

(1.9) sup

y, y

0

∈R

d

, r≥|y−y

0

|

X l=1

l m Z

2

l

r<|x−y|≤2

l+1

r

n

|K(x, y) − K(x, y 0 )|

+|K(y, x) − K(y 0 , x)| o

dµ(x) < ∞,

and if the operators T ² are bounded on L 2 (µ) uniformly on ² > 0, then for b i ∈ RBMO(µ) with i = 1, 2, . . . , m, the operator T ~b is bounded on L p (µ) for any p ∈ (1, ∞). It was also proved in [3] that if K satisfies (1.2) and (1.7), and if the operators T ² are bounded on L 2 (µ) uniformly for ² > 0, then for m = 1, the maximal commutator T ~b satisfies the weak type endpoint estimate, namely, there exists a constant C > 0 such that for all λ > 0 and all bounded functions f with compact support,

µ

³n

x ∈ R d : |T ~b (f )(x)| > λ

≤ Cϕ 1/r

³

kb 1 k Osc

exp Lr

(µ)

´ Z

R

d

ϕ 1/r

³ |f(x)|

λ

´ dµ(x).

In this paper, we will further prove that if K satisfies (1.2) and (1.9), then for any m ∈ N, the maximal commutator T ~b enjoys the same endpoint estimate.

Our result can be stated as follows.

Theorem 1.1. Let m ∈ N, r i ≥ 1 and b i ∈ Osc exp L

ri

(µ) for i = 1, 2, . . . , m, and T b be the same as in (1.8) with the kernel K satisfying (1.2) and (1.9). If the operators T ² are bounded on L 2 (µ) uniformly for ² > 0, then there exists a constant C > 0 such that for all λ > 0 and all bounded functions f with compact support,

(1.10)

µ

³n

x ∈ R d : |T ~b (f )(x)| > λ

≤ Cϕ 1/r

³ Y m

i=1

kb i k Osc

exp Lri

(µ)

´ Z

R

d

ϕ 1/r

³ |f(x)|

λ

´ dµ(x).

Throughout this paper, for any index p ∈ [1, ∞], we denote by p 0 its conju-

gate index, namely, 1/p + 1/p 0 = 1. For f ∼ g, we mean that the ratio f /g is

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bounded and bounded away from zero by constants independent of the relevant variables in f and g. Similar is f . g. Constants with subscripts, such as C 0 , are positive constants independent of the main parameters involved but whose values may not be the same at each occurrence.

2. Proof of Theorem 1.1

We begin with a generalization of the H¨older inequality. For r > 0, a cube Q and an appropriate function f , define

kf k L(logL)

r

, Q = inf n

λ > 0 : 1 µ(2Q)

Z

Q

|f (x)|

λ log r µ

2 + |f (x)|

λ

dµ(x) ≤ 1 o

, and

kf k expL

r

, Q = inf n

λ > 0 : 1 µ(2Q)

Z

Q

exp

µ |f (x)|

λ

r

dµ(x) ≤ 2 o . Then for any cube Q,

(2.1) 1

µ(2Q) Z

Q

¯ ¯

¯ Y m i=1

b i (x)f (x)

¯ ¯

¯ dµ(x) ≤ C Y m i=1

kb i k exp L

ri

, Q kf k L(log L)

1/r

, Q , where r i ≥ 1 and 1/r = P m

i=1 1/r i ; see Lemma 3.2 in [8] and the related references there.

Lemma 2.1. Let m ∈ N, r i ≥ 1 and b i ∈ Osc exp L

ri

(µ) for i = 1, 2, . . . , m, and M ~b be defined by

(2.2) M ~b (f )(x) = sup

r>0

1 r n

Z

|y−x|≤r

Y m i=1

|b i (x) − b i (y)||f (y)| dµ(y).

Then there exists a constant C > 0 such that for all λ > 0 and all bounded functions f with compact support,

µ ¡©

x ∈ R d : M ~b (f )(x) > λ ª¢

≤ Cϕ 1/r

³ Y m

i=1

kb i k Osc

exp Lri

(µ)

´ Z

R

d

ϕ 1/r

µ |f (x)|

λ

dµ(x), where r and ϕ 1/r are the same as in Theorem 1.1.

For the special case m = 1, Lemma 2.1 was proved in [3]. For m ≥ 2, Lemma 2.1 can be proved in a similar way. We omit the details for brevity.

Proof of Theorem 1.1. By the homogeneity, we may assume that for i = 1, . . . , m, kb i k Osc

exp Lri

(µ) = 1. We carry out the argument by induction on m.

Step I. m = 1. In this case, we denote T ~b simply by T b . For each fixed bounded function f with compact support and each λ > 0 (with λ >

2 d+1 kf k L

1

(µ) /kµk if kµk < ∞; note that if kµk < ∞ and λ ≤ 2 d+1 kf k L

1

(µ) /kµk,

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then the inequality (1.10) is trivial), applying the Calder´on-Zygmund decom- position to f at level λ (see [9]), we can obtain a sequence of cubes {Q j } j∈N

with bounded overlaps (that is, P

j χ Q

j

(x) . 1) such that (a) 2

d+1

λ < µ(2Q 1

j

)

R

Q

j

|f (x)| dµ(x);

(b) µ(2ηQ 1

j

)

R

ηQ

j

|f (x)| dµ(x) ≤ 2

d+1

λ for any η > 2;

(c) |f (x)| ≤ λ µ-a. e. on R d \ ∪ j Q j ;

(d) for each fixed j, let R j be the smallest (6, 6 n+1 )-doubling cube of the form 6 k Q j , k ≥ 1. Set w j = χ Q

j

/ P

k χ Q

k

. Then there is a function θ j

with supp θ j ⊂ R j and satisfying Z

R

d

θ j (x) dµ(x) = Z

Q

j

f (x)w j (x) dµ(x), kθ j k L

(µ) µ(R j ) . Z

Q

j

|f (x)| dµ(x), and P

j j (x)| . λ.

Set g(x) = f (x)χ R

d

\∪

j

Q

j

(x) + P

j θ j (x) and h(x) = f (x) − g(x) = X

j

{f (x)w j (x) − θ j (x)} = X

j

h j (x).

Obviously,

T b (f )(x) ≤ T b (g)(x) + T b (h)(x).

Note that kgk L

(µ) . λ, and kgk L

1

(µ) . kf k L

1

(µ) . The L 2 (µ)-boundedness of T b tells us that

(2.3) µ ¡©

x ∈ R d : T b (g)(x) > λ ª¢

. λ −2 Z

R

d

|g(x)| 2 dµ(x) . λ −1

Z

R

d

|f (x)| dµ(x).

Taking into account the fact that (2.4) µ (∪ j 2Q j ) . λ −1

Z

R

d

|f (x)| dµ(x),

we see that the proof of Theorem 1.1 can be reduced to proving that (2.5) µ ¡©

x ∈ R d \ ∪ j 2Q j : T b (h)(x) > λ ª¢

. Z

R

d

ϕ 1/r

³ |f(x)|

λ

´ dµ(x).

To this end, by the vanishing moment conditions of h j for j ∈ N, we can write T b (h)(x)χ R

d

\ j 2Q j (x)

= sup

²>0

¯ ¯

¯ ¯

¯ ¯ X

j

Z

R

d

½

K ² (x, y) [b(x) − b(y)]

−K ² (x, x Q

j

) h

b(x) − m Q e

j

(b) i ¾

h j (y) dµ(y)

¯ ¯

¯ ¯ χ R

d

\ j 2Q j (x)

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X

j

¯ ¯

¯b(x) − m Q f

j

(b)

¯ ¯

¯

× sup

²>0

¯ ¯

¯ ¯ Z

R

d

£ K ² (x, y) − K ² (x, x Q

j

) ¤

h j (y) dµ(y)

¯ ¯

¯ ¯ χ R

d

\ j 2Q j (x) + T ³ X

j

h

b − m Q f

j

(b) i

h j

´ (x)

= E(x) + F(x),

where T is defined by (1.5), and K ² for ² > 0 is defined by K ² (x, y) = K(x, y)χ {|x−y|>²} (x, y).

Theorem 1.1 in [2] tells us that if T ² are bounded on L 2 (µ) uniformly on ² > 0, and K satisfies (1.2) and (1.3), then T is bounded from L 1 (µ) to weak L 1 (µ).

Thus, µ ¡©

x ∈ R d : |F(x)| > λ ª¢

. λ −1 X

j

Z

R

d

¯ ¯

¯b(x) − m Q f

j

(b)

¯ ¯

¯ |f (x)w j (x)| dµ(x)

+ λ −1 X

j

Z

R

d

¯ ¯

¯b(x) − m Q f

j

(b)

¯ ¯

¯ |θ j (x)| dµ(x)

= G + H.

Note that R j is also (2, 2 n+1 )-doubling and R j = f R j . A trivial computation gives us that K Q f

j

, R

j

. 1. Thus,

H . λ −1 X

j

j k L

(µ)

(Z

R

j

¯ ¯b(x) − m R

j

(b) ¯

¯ dµ(x)

+µ(R j )

¯ ¯

¯m R

j

(b) − m Q f

j

(b)

¯ ¯

¯ o

. λ −1 X

j

j k L

(µ) µ(R j )

. λ −1 Z

R

d

|f (x)| dµ(x).

On the other hand, by the generalization of H¨older inequality (2.1), we obtain G . λ −1 X

j

µ(2Q j )kf k L(log L)

1/r

, Q

j

kb − m Q f

j

(b)k expL

r

, Q

j

. λ −1 X

j

µ(2Q j ) inf

t>0

(

t + t µ(2Q j )

Z

Q

j

|f (x)|

t log 1/r

³

2 + |f (x)|

t

´ dµ(x)

)

. Z

R

d

|f (x)|

λ log 1/r ³

2 + |f (x)|

λ

´

dµ(x).

(9)

It remains to estimate E(x). Note that for y ∈ R j and x ∈ R d \ 2R j ,

|x − x Q

j

| ∼ |x − y|. A straightforward computation indicates sup

²>0

Z

R

d

¯ ¯K ² (x, y) − K ² (x, x Q

j

) ¯

¯ |h j (y)| dµ(y)

Z

R

d

¯ ¯K(x, y) − K(x, x Q

j

) ¯

¯ |h j (y)| dµ(y)

+ sup

²>0

Z

R

d

n

|K(x, y)|χ {|x−y|>²}∩{|x−x

Qj

|≤²} (x, y) +|K(x, x Q

j

)|χ {|x−y|≤²}∩{|x−x

Qj

|>²} (x, y)

o

|h j (y)| dµ(y) .

Z

R

d

¯ ¯K(x, y) − K(x, x Q

j

) ¯

¯ |h j (y)| dµ(y) + M (h j )(x), where M is the Hardy-Littlewood maximal operator defined by

M h(x) = sup

Q3x

1 [l(Q)] n

Z

Q

|h(y)| dµ(y).

Therefore, E(x) . X

j

¯ ¯

¯b(x) − m Q f

j

(b)

¯ ¯

¯ Z

R

d

¯ ¯K(x, y) − K(x, x Q

j

) ¯

¯ |h j (y)| dµ(y)χ R

d

\2R

j

(x)

+ M ~b ³ X

j

|h j | ´

(x) + M ³ X

j

¯ ¯b − m Q f

j

(b) ¯

¯|h j | ´ (x)

+ X

j

¯ ¯

¯b(x) − m Q f

j

(b)

¯ ¯

¯ T (h j )(x)χ 2R

j

\2Q

j

(x)

+ X

j

¯ ¯

¯b(x) − m Q f

j

(b)

¯ ¯

¯ sup

²>0

Z

R

d

¯ ¯K ² (x, x Q

j

)h j (y) ¯

¯ dµ(y)χ 2R

j

\2Q

j

(x)

= E 1 (x) + E 2 (x) + E 3 (x) + E 4 (x) + E 5 (x).

An application of Lemma 2.1 gives us that µ ¡©

x ∈ R d : E 2 (x) > λ ª¢

. Z

R

d

ϕ 1/r ³ P

j |f ω j (x)|

λ

´ dµ(x)

+ Z

R

d

ϕ 1/r

³ P j j (x)|

λ

´ dµ(x)

= I + J.

Obviously,

I . Z

R

d

ϕ 1/r ³ |f(x)|

λ

´ dµ(x).

Recall that P

j j (x)| . λ. It then follows that J . λ −1 X

j

j k L

(µ) µ(R j ) . λ −1 Z

R

d

|f (x)| dµ(x),

(10)

and so

µ ¡©

x ∈ R d : E 2 (x) > λ ª¢

. Z

R

d

ϕ 1/r ³ |f(x)|

λ

´ dµ(x).

Since the Hardy-Littlewood maximal operator M is bounded from L 1 (µ) to weak L 1 (µ), similar to the estimate for F(x), it follows that

µ ¡©

x ∈ R d : E 3 (x) > λ ª¢

. Z

R

d

ϕ 1/r

³ |f(x)|

λ

´ dµ(x).

To estimate E 4 (x), observing that 1 ≤ k ≤ N 2Q

j

, 2R

j

, K Q f

j

, ^ 2

k+1

Q

j

. K Q

j

, R

j

. 1, we can easily obtain that

µ ¡©

x ∈ R d : E 4 (x) > λ ª¢

. 1 λ

X

j

N

2Qj , 2Rj

X

k=1

Z

2

k+1

Q

j

\2

k

Q

j

× Z

R

d

|b(x) − m Q f

j

(b)|

|x − y| n {|f (y)w j (y)| + |θ j (y)|} dµ(y)dµ(x) . 1

λ X

j

N

2Qj , 2Rj

X

k=1

µ(2 k+2 Q j ) l(2 k Q j ) n K Q f

j

, ^ 2

k+1

Q

j

× (Z

Q

j

|f (y)| dµ(y) + kθ j k L

(µ) µ(R j ) )

. 1 λ

X

j

Z

Q

j

|f (y)| dµ(y), and similarly,

µ ¡©

x ∈ R d : E 5 (x) > λ ª¢

. 1 λ

X

j

Z

Q

j

|f (y)| dµ(y).

For E 1 (x), another application of the generalized H¨older inequality (2.1) yields Z

R

d

\2R

j

¯ ¯

¯b(x) − m Q f

j

(b)

¯ ¯

¯ ¯

¯K(x, y) − K(x, x Q

j

) ¯

¯ dµ(x)

X k=1

¯ ¯

¯m 2 ^

k+1

R

j

(b) − m Q f

j

(b)

¯ ¯

¯ Z

2

k+1

R

j

\2

k

R

j

¯ ¯K(x, y) − K(x, x Q

j

) ¯

¯ dµ(x)

+ X k=1

Z

2

k+1

R

j

\2

k

R

j

¯ ¯

¯b(x) − m 2

k+1

^ R

j

(b)

¯ ¯

¯ ¯

¯K(x, y) − K(x, x Q

j

) ¯

¯ dµ(x)

. X k=1

K Q f

j

, ^ 2

k+1

R

j

Z

2

k+1

R

j

\2

k

R

j

¯ ¯K(x, y) − K(x, x Q

j

) ¯

¯ dµ(x)

(11)

+ X k=1

µ ¡ 2 k+2 R j

¢ ° °

°b − m 2 ^

k+1

R

j

(b)

° °

° exp L

r

(µ), 2

k+1

R

j

× °

° ©

K(·, y) − K(·, x Q

j

) ª

χ 2

k+1

R

j

\2

k

R

j

(·) °

° L(log L)

1/r

(µ), 2

k+1

R

j

. Let

λ k = £ µ ¡

2 k+2 R j

¢¤ −1 ³ k

Z

2

k+1

R

j

\2

k

R

j

¯ ¯K(x, y) − K(x, x Q

j

) ¯

¯ dµ(x) + 2 −k ´ . By (1.2), we then have that for y ∈ R j ,

1 µ(2 k+2 R j )

Z

2

k+1

R

j

\2

k

R

j

|K(x, y) − K(x, x Q

j

)|

λ k

× log 1/r

³

2 + |K(x, y) − K(x, x Q

j

)|

λ k

´ dµ(x)

. 1

µ(2 k+2 R j ) Z

2

k+1

R

j

\2

k

R

j

|K(x, y) − K(x, x Q

j

)|

λ k

× log 1/r

³

2 + 1

λ k |x − y| n + 1 λ k |x − x Q

j

| n

´ dµ(x)

. k

µ(2 k+2 R j ) Z

2

k+1

R

j

\2

k

R

j

|K(x, y) − K(x, x Q

j

)|

λ k

dµ(x) . 1.

Thus,

° ° ©

K(·, y) − K(·, x Q

j

) ª

χ 2

k+1

R

j

\2

k

R

j

(·) °

° L(log L)

1/r

(µ), 2

k+1

R

j

. λ k . This via (1.9) tells us that

Z

R

d

\2R

j

¯ ¯

¯b(x) − m Q f

j

(b)

¯ ¯

¯ ¯

¯K(x, y) − K(x, x Q

j

) ¯

¯ dµ(x)

. X k=1

à k

Z

2

k+1

R

j

\2

k

R

j

¯ ¯K(x, y) − K(x, x Q

j

) ¯

¯ dµ(x) + 2 −k

!

. 1.

Therefore, µ ¡©

x ∈ R d : E 1 (x) > λ ª¢

. 1 λ

X

j

Z

R

j

Z

R

d

\2R

j

¯ ¯

¯b(x) − m Q f

j

(b)

¯ ¯

¯

× ¯

¯K(x, y) − K(x, x Q

j

) ¯

¯ |h j (y)| dµ(x) dµ(y) . 1

λ X

j

Z

R

j

|h j (y)| dµ(y)

. 1 λ

Z

R

d

|f (y)| dµ(y),

(12)

which along with the estimates for E 2 (x), E 3 (x), E 4 (x) and E 5 (x) gives the desired estimate for E(x). Combining the estimates for E(x) and F(x) yields the estimate (2.5) and then completes the proof of m = 1.

Step II. m ≥ 2. In this case, we need more notation. For 0 ≤ i ≤ m, we de- note by C i m the family of all finite subsets σ = {σ(1), . . . , σ(i)} of {1, 2, . . . , m}

with i different elements. For σ ∈ C i m , the complementary sequence σ 0 is given by σ 0 = {1, 2, . . . , m}\σ. If σ = ∅, we set σ 0 = {1, . . . , m}. For any i−tuple r = (r 1 , r 2 , . . . , r i ), we write 1/r σ = 1/r σ(1) + · · · + 1/r σ(i) and 1/r σ

0

= 1/r − 1/r σ , where 1/r = 1/r 1 + · · · + 1/r m . Let ~b = (b 1 , b 2 . . . , b m ) be a finite family of locally integrable functions. For σ ∈ C i m , we set ~b σ = (b σ(1) , . . . , b σ(i) ) and the product b σ = b σ(1) · · · b σ(i) . For σ = ∅, we define b σ = 1. With this notation, we write

k~b σ k Osc

exp Lrσ

(µ) = kb σ(1) k Osc

exp Lrσ(1)

(µ) · · · kb σ(i) k Osc

exp Lrσ(i)

(µ) . For i ∈ {1, . . . , m} and σ ∈ C i m , we set

[b(y) − b(z)] σ = £

b σ(1) (y) − b σ(1) (z) ¤

· · · £

b σ(i) (y) − b σ(i) (z) ¤ and

h

m Q e (b) − b(y) i

σ = h

m Q e (b σ(1) ) − b σ(1) (y) i

· · · h

m Q e (b σ(i) ) − b σ(i) (y) i ,

where Q is any cube in R d and y, z ∈ R d . For any σ ∈ C i m , define

T ~b

σ

(f )(x) =

¯ ¯

¯ sup

²>0

Z

R

d

K ² (x, y) Y i j=1

£ b σ(j) (x) − b σ(j) (y) ¤

f (y) dµ(y)

¯ ¯

¯.

When σ = {1, . . . , m}, we denote T ~b

σ

simply by T ~b .

Now let m ≥ 2 be an integer. We assume that (1.10) holds for any 1 ≤ i ≤ m − 1 and any subset σ ∈ C i m . For any fixed f and λ > 2 d+1 kf k L

1

(µ) /kµk, let Q j , R j , θ j , w j , g, h and h j be the same as in Step I. By an argument similar to the estimates for (2.3) and (2.4), it suffices to verify that

(2.6) µ ³n

x ∈ R d \ ∪ j 2Q j : |T ~b h(x)| > λ

. Z

R

d

ϕ 1/r ³ |f(x)|

λ

´ dµ(x).

With the aid of the formula that for y, z ∈ R d , Y m

i=1

h

m Q e (b i ) − b i (z) i

= X m i=0

X

σ∈C

im

[b(y) − b(z)] σ

0

h

m Q e (b) − b(y) i

σ

(13)

and the vanishing moment conditions satisfied by h j for j ∈ N, it is easy to see that

T ~b h(x) = sup

²>0

¯ ¯

¯ ¯

¯ ¯ X

j

Z

R

d

(

K ² (x, y) Y m i=1

[b i (x) − b i (y)]

−K ² (x, x Q

j

) Y m i=1

h

b i (x) − m Q e

j

(b i ) i )

h j (y) dµ(y)

¯ ¯

¯ ¯

¯

≤ sup

²>0

X

j

Y m i=1

¯ ¯

¯b i (x) − m Q e

j

(b i )

¯ ¯

¯

× Z

R

d

¯ ¯K ² (x, y) − K ² (x, x Q

j

) ¯

¯ |h j (y)| dµ(y)

+ T ³ X

j

Y m i=1

h

b i − m Q e

j

(b i ) i h j

´ (x)

+

m−1 X

i=1

X

σ∈C

im

T ~b

σ0

³ X

j

h

b − m Q f

j

(b) i

σ h j

´ (x)

= T ~b ∗, I (h)(x) + T ~b ∗, II (h)(x) +

m−1 X

i=1

X

σ∈C

mi

T ~b ∗, III

σ0

(h)(x).

Similar to the estimate for E(x) in Step I, we have µ

³n

x ∈ R d \ ∪ j 2Q j : T ~b ∗, I (h)(x) > λ

. Z

R

d

ϕ 1/r

µ |f (x)|

λ

dµ(x).

On the other hand, the same argument as that for F(x) in Step I leads to that µ

³n

x ∈ R d \ ∪ j 2Q j : T ~b ∗, II (h)(x) > λ

. Z

R

d

ϕ 1/r

µ |f (x)|

λ

dµ(x).

For each fixed i with 1 ≤ i ≤ m − 1, our induction hypothesis now states that µ

³n

x ∈ R d : T ~b ∗, III

σ0

(h)(x) > λ

. X

j

Z

R

d

ϕ 1/r

σ0

³ ¯ ¯

¯ h

b(x) − m Q f

j

(b) i

σ

¯ ¯

¯ |w j (x)f (x)|

λ

´ dµ(x)

+ Z

R

d

ϕ 1/r

σ0

³ X

j

¯ ¯

¯ h

b(x) − m Q f

j

(b) i

σ

¯ ¯

¯ j (x)|

λ

´ dµ(x)

= M σ + N σ . Applying the inequality

ϕ 1/r

σ0

(t 0 t 1 · · · t i ) . ϕ 1/r (t 0 ) + exp t r 1

σ(1)

+ · · · + exp t r i

σ(i)

, t 0 , t 1 , . . . , t i > 0

(14)

(see Lemma 2.2 in [8]), and the fact (a) in the Calder´on-Zygmund decomposi- tion, we then deduce that

M σ . X

j

Z

R

d

ϕ 1/r ³

k~b σ k Osc

exp Lrσ

(µ) Q

j

(x)f (x)|

λ

´ dµ(x)

+ X

j

X i l=1

Z

R

d

exp ³ |b σ(l) (x) − m Q f

j

(b σ(l) )|

kb σ(l) k Osc

exp Lrσ(l)

(µ) χ Q

j

(x)

´ r

σ(l)

dµ(x)

. Z

R

d

|f (x)|

λ log 1/r ³

2 + |f (x)|

λ

´

dµ(x) + X

j

µ(2Q j )

. Z

R

d

|f (x)|

λ log 1/r

³

2 + |f (x)|

λ

´ dµ(x).

To estimate N σ , let r j = λ −1 j |, and Λ ⊂ N be a finite index set. The convexity of ϕ 1/r

σ0

says that

ϕ 1/r

σ0

³ X

j∈Λ

¯ ¯

¯ h

b(x) − m Q f

j

(b) i

σ

¯ ¯

¯ j (x)|

λ

´

X

j∈Λ

³ P r j l∈Λ r l

´

ϕ 1/r

σ0

³ ¯ ¯

¯ h

b(x) − m Q f

j

(b) i

σ

¯ ¯

¯ χ R

j

(x) X

l∈Λ

r l

´

. 1

P

l∈Λ r l

ϕ 1/r

σ0

³ X

l∈Λ

r l

´ X

j∈Λ

r j ϕ 1/r

σ0

³¯

¯ £

b(x) − m Q f

j

(b) ¤

σ

¯ ¯χ R

j

(x) ´

. log 1/r

σ0

³ 2 + X

l∈Λ

r l

´ X

j∈Λ

r j ϕ 1/r

σ0

³¯ ¯ £

b(x) − m Q f

j

(b) ¤

σ

¯ ¯χ R

j

(x)

´

. X

j∈Λ

r j ϕ 1/r

σ0

³¯

¯ £

b(x) − m Q f

j

(b) ¤

σ

¯ ¯χ R

j

(x) ´ . This in turn leads to that

N σ . λ −1 X

j

j k L

(µ) Z

R

j

ϕ 1/r

σ0

³¯ ¯

¯ h

b(x) − m Q f

j

(b) i

σ

¯ ¯

¯

´ dµ(x)

. λ −1 X

j

j k L

(µ) µ(R j )

. λ −1 Z

R

d

|f (x)| dµ(x).

Therefore, for 1 ≤ i ≤ m − 1 and σ ∈ C i m , we have µ ³n

x ∈ R d : T ~b ∗, III

σ0

(h)(x) > λ

. Z

R

d

ϕ 1/r

µ |f (x)|

λ

dµ(x),

which completes the proof of (2.6), and hence the proof of Theorem 1.1. ¤

Acknowledgements. The authors would like to express their sincere thanks

to the referee for his careful reading and useful suggestions.

(15)

References

[1] G. Hu, Y. Meng, and D. Yang, Multilinear commutators of singular integrals with non doubling measures, Integral Equations Operator Theory 51 (2005), no. 2, 235–255.

[2] , Estimates for maximal singular integral operators in non-homogeneous spaces, Proc. Roy. Soc. Edinburgh Sect. A 136 (2006), no. 2, 351–364.

[3] , Endpoint estimate for maximal commutators with non-doubling measures, Acta Math. Sci. Ser. B Engl. Ed. 26 (2006), no. 2, 271–280.

[4] , Boundedness of some maximal commutators in Hardy-type spaces with non- doubling measures, Acta Math. Sin. (Engl. Ser.) 23 (2007), no. 6, 1129–1148.

[5] F. Nazarov, S. Treil, and A. Volberg, Accretive system T b-theorems on nonhomogeneous spaces, Duke Math. J. 113 (2002), no. 2, 259–312.

[6] , T b-theorem on nonhomogeneous spaces, Acta Math. 190 (2003), 151–239.

[7] J. Orobitg and C. P´erez, A

p

weights for nondoubling measures in R

n

and applications, Trans. Amer. Math. Soc. 354 (2002), no. 5, 2013–2033.

[8] C. P´erez and R. Trujillo-Gonz´ alez, Sharp weighted estimates for multilinear commuta- tors, J. London Math. Soc. 65 (2002), no. 3, 672–692.

[9] X. Tolsa, BMO, H

1

, and Calderon-Zygmund operators for non doubling measures, Math. Ann. 319 (2001), no. 1, 89–149.

[10] , A T (1) theorem for non-doubling measures with atoms, Proc. London Math.

Soc. (3) 82 (2001), no. 1, 195–228.

[11] , Littlewood-Paley theory and the T (1) theorem with non-doubling measures, Adv. Math. 164 (2001), no. 1, 57–116.

[12] , The space H

1

for nondoubling measures in terms of a grand maximal operator, Trans. Amer. Math. Soc. 355 (2003), no. 1, 315–348.

[13] , Painlev´e’s problem and the semiadditivity of analytic capacity, Acta Math. 190 (2003), 105–149.

[14] J. Verdera, The fall of the doubling condition in Calder´ on-Zygmund theory, Publ. Mat.

Vol. Extra (2002), 275–292.

Guoen Hu

Department of Applied Mathematics University of Information Engineering Zhengzhou 450002, P. R. China

E-mail address: [email protected] Yan Meng

School of Information Renmin University of China Beijing 100872, P. R. China E-mail address: [email protected] Dachun Yang

School of Mathematical Sciences

Beijing Normal University

Beijing 100875, P. R. China

E-mail address: [email protected]

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