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BOUNDEDNESS OF MULTILINEAR OPERATORS ON TRIEBEL-LIZORKIN SPACES
LIU LANZHE Received 20 January 2003
The purpose of this paper is to study the boundedness in the context of Triebel-Lizorkin spaces for some multilinear operators related to certain convolution operators. The opera- tors include Littlewood-Paley operator, Marcinkiewicz integral, and Bochner-Riesz operator.
2000 Mathematics Subject Classification: 42B20, 42B25.
1. Introduction. LetTbe a Calderon-Zygmund operator. A well-known result of Coif- man et al. [6] states that the commutator [b, T ]=T (bf )−bT f (whereb∈BMO) is bounded onLp(Rn)for 1< p <∞; Chanillo [1] proves a similar result whenT is re- placed by the fractional integral operator. In [7, 9], Janson and Paluszy´nski extend these results to the Triebel-Lizorkin spaces and the caseb∈Lipβ(where Lipβis the homogeneous Lipschitz space). The main purpose of this paper is to discuss the bound- edness of some multilinear operators related to certain convolution operators in the context of Triebel-Lizorkin spaces. In fact, we will establish the boundedness on the Triebel-Lizorkin spaces for some multilinear operators related to certain convolution operator only under certain conditions on the size of the operators. As applications, we obtain the boundedness of the multilinear operators related to the Marcinkiewicz inte- gral, Littlewood-Paley operator, and Bochner-Riesz operator in the context of Triebel- Lizorkin spaces.
2. Preliminaries. Throughout this paper, M(f ) will denote the Hardy-Littlewood maximal function off,Mpf=(M(fp))1/p forp >0, andQwill denote a cube ofRn with sides parallel to the axes. For a cubeQ, letfQ= |Q|−1
Qf (x)dxand f#(x)= supx∈Q|Q|−1
Q|f (y)−fQ|dy. For β >0 and p >1, let ˙Fpβ,∞ be the homogeneous Triebel-Lizorkin space. The Lipschitz space ˙∧βis the space of functionsfsuch that
f∧˙β= sup
x,h∈Rn h≠0
∆[β]h +1f (x)
|h|β <∞, (2.1)
where∆khdenotes thekth difference operator (see [9]).
The operators considered in this paper are following several sublinear operators.
Letmbe a positive integer and letAbe a function onRn. We denote Rm+1(A;x, y)=A(x)−
|α|≤m
1
α!DαA(y)(x−y)α. (2.2)
Definition2.1. Letε >0 and letψbe a fixed function which satisfies the following properties:
(1) |ψ(x)| ≤C(1+|x|)−(n+1),
(2) |ψ(x+y)−ψ(x)| ≤C|y|ε(1+|x|)−(n+1+ε)when 2|y|<|x|. The multilinear Littlewood-Paley operator is defined by
gAψ(f )(x)= ∞
0
FtA(f )(x)2dt t
1/2
, (2.3)
where
FtA(f )(x)=
Rnψt(x−y)Rm+1(A;x, y)
|x−y|m f (y)dy (2.4) andψt(x)=t−nψ(x/t)fort >0. DenoteFt(f )=ψt∗f. Also define
gψ(f )(x)=∞ 0
Ft(f )(x)2dt t
1/2
(2.5) which is the Littlewood-Paleygfunction (see [10]).
LetH be the spaceH= {h:h =(∞
0 |h(t)|2dt/t)1/2<∞}. Then, for each fixed x∈Rn,FtA(f )(x)may be viewed as a mapping from[0,+∞)toH, and it is clear that
gψ(f )(x)=Ft(f )(x), gψA(f )(x)=FtA(f )(x). (2.6) Definition2.2. Let 0< γ≤1 and letΩ be homogeneous of degree zero onRn such that
Sn−1Ω(x)dσ (x)=0. Assume thatΩ∈Lipγ(Sn−1), that is, there exists a constantM >0 such that for anyx, y∈Sn−1,|Ω(x)−Ω(y)| ≤M|x−y|γ. The multi- linear Marcinkiewicz integral operator is defined by
µAΩ(f )(x)= ∞
0
FtA(f )(x)2dt t3
1/2
, (2.7)
where
FtA(f )(x)=
|x−y|≤t
Ω(x−y)
|x−y|n−1
Rm+1(A;x, y)
|x−y|m f (y)dy. (2.8) Denote
Ft(f )(x)=
|x−y|≤t
Ω(x−y)
|x−y|n−1f (y)dy. (2.9) Also define
µΩ(f )(x)= ∞
0
Ft(f )(x)2dt t3
1/2
(2.10) which is the Marcinkiewicz integral (see [11]).
LetHbe the spaceH= {h:h =(∞
0 |h(t)|2dt/t3)1/2<∞}. Then, it is clear that µΩ(f )(x)=Ft(f )(x), µΩA(f )(x)=FtA(f )(x). (2.11)
Definition2.3. LetBδt(f )(ξ)ˆ =(1−t2|ξ|2)δ+f (ξ). Denoteˆ Bδ,tA (f )(x)=
RnBδt(x−y)Rm+1(A;x, y)
|x−y|m f (y)dy, (2.12) whereBδt(z)=t−nBδ(z/t)fort >0. The maximal multilinear Bochner-Riesz operator is defined by
Bδ,∗A (f )(x)=sup
t>0
Bδ,tA (f )(x). (2.13)
Also define
Bδ∗(f )(x)=sup
t>0
Bδt(f )(x) (2.14)
which is the Bochner-Riesz operator (see [7,8]).
LetHbe the spaceH= {h:h =supt>0|h(t)|<∞}, then it is clear that
Bδ∗(f )(x)=Btδ(f )(x), Bδ,∗A (f )(x)=BAδ,t(f )(x). (2.15) More generally, we consider the following multilinear operators related to certain convolution operators.
Definition2.4. LetK(x, t)be defined onRn×[0,+∞). Denote that Ktf (x)=
RnK(x−y, t)f (y)dy, KtAf (x)=
Rn
Rm+1(A;x, y)
|x−y|m K(x−y, t)f (y)dy.
(2.16)
Let H be the normed space H= {h:h<∞}. For each fixedx ∈Rn, Ktf (x) and KAt(f )(x)are viewed as a mapping from[0,+∞)toH. Then, the multilinear operators related toKtis defined by
TAf (x)=KtA(f )(x); (2.17) also defineT f (x)= Ktf (x).
It is clear that Definitions2.1,2.2, and2.3are the particular examples ofDefinition 2.4. Note that whenm=0,TAis just the commutator ofKtandA. It is well known that multilinear operators are of great interest in harmonic analysis and have been widely studied by many authors (see [2,3,4,5]). The main purpose of this paper is to consider the continuity of the multilinear operators on Triebel-Lizorkin spaces. We will prove the following theorems inSection 3.
Theorem2.5. LetgψAbe the multilinear Littlewood-Paley operator as inDefinition 2.1 and let0< β <min(1, ε),1< p <∞, andDαA∈∧˙βfor|α| =m. Then
(a) gψAis bounded fromLp(Rn)toF˙pβ,∞(Rn),
(b) gψAis bounded fromLp(Rn)toLq(Rn)for1/p−1/q=β/nand1/p > β/n.
Theorem2.6. LetµΩAbe the multilinear Marcinkiewicz integral operator as inDefini- tion 2.2and let0< γ≤1,0< β <min(1/2, γ),1< p <∞, andDαA∈∧˙βfor|α| =m.
Then
(a) µΩAis bounded fromLp(Rn)toF˙pβ,∞(Rn),
(b) µΩAis bounded fromLp(Rn)toLq(Rn)for1/p−1/q=β/nand1/p > β/n.
Theorem 2.7. Let BAδ,∗ be the maximal multilinear Bochner-Riesz operator as in Definition 2.3 and let δ > (n−1)/2, 0< β <min(1, δ−(n−1)/2), 1< p <∞, and DαA∈∧˙βfor|α| =m. Then
(a) Bδ,∗A is bounded fromLp(Rn)toF˙pβ,∞(Rn);
(b) Bδ,∗A is bounded fromLp(Rn)toLq(Rn)for1/p−1/q=β/nand1/p > β/n.
3. Main theorem and proof. First, we will establish the following theorem.
Theorem3.1. Let0< β <1,1< p <∞, andDαA∈∧˙βfor|α| =m. LetKt,T, and TA be the same as inDefinition 2.4. IfT is bounded onLq(Rn)forq∈(1,+∞)andTA
satisfies the size condition
KtA(f )(x)−KtA(f )
x0 ≤C
|α|=m
DαA˙
∧β|Q|β/nM(f )(x) (3.1)
for any cubeQwithsuppf⊂(2Q)candx∈Q, then (a) TAis bounded fromLp(Rn)toF˙pβ,∞(Rn),
(b) TAis bounded fromLp(Rn)toLq(Rn)for1/p−1/q=β/nand1/p > β/n.
To prove the theorem, we need the following lemmas.
Lemma3.2(see [9]). For0< β <1and1< p <∞, fF˙pβ,∞≈
sup
Q
1
|Q|1+β/n
Q
f (x)−fQdx Lp
≈ sup
·∈Qinf
c
1
|Q|1+β/n
Q
f (x)−cdx Lp.
(3.2)
Lemma3.3(see [9]). For0< β <1and1≤p≤ ∞, f˙∧β≈sup
Q
1
|Q|1+β/n
Q
f (x)−fQdx
≈sup
Q
1
|Q|β/n 1
|Q|
Q
f (x)−fQpdx 1/p
.
(3.3)
Lemma3.4(see [1]). For1≤r <∞andδ >0, let Mδ,r(f )(x)=sup
x∈Q
1
|Q|1−δr /n
Q
f (y)pdy 1/p
. (3.4)
Suppose thatr < p < δ/nand1/q=1/p−δ/n. ThenMδ,r(f )Lq≤CfLp.
Lemma3.5(see [9]). LetQ1⊂Q2. Then
fQ1−fQ2≤Cf∧˙βQ2β/n. (3.5) Lemma3.6(see [4]). LetAbe a function onRn andDαA∈Lq(Rn)for|α| =mand someq > n. Then
Rm(A;x, y)≤C|x−y|m
|α|=m
1 Q(x, y)˜
Q(x,y)˜
DαA(z)qdz 1/q
, (3.6)
whereQ(x, y)˜ is the cube centered atxand having side length5√
n|x−y|. Proof ofTheorem3.1. (a) Fix a cubeQ=Q(x0, l)and ˜x∈Q. Let ˜Q=5√
nQand A(x)˜ =A(x)−
|α|=m(1/α!)(DαA)Q˜xα, then Rm(A;x, y)=Rm(A;˜x, y) and DαA˜= DαA−(DαA)Q˜ for|α| =m. Forf1=f χQ˜andf2=f χRn\Q˜,
KtA(f )(x)=
Rn
Rm+1A;˜x, y
|x−y|m K(x−y, t)f (y)dy
=
Rn
Rm+1A;˜x, y
|x−y|m K(x−y, t)f (y)dy +
Rn
RmA;˜x, y
|x−y|m K(x−y, t)f1(y)dy
−
|α|=m
1 α!
Rn
K(x−y, t)(x−y)α
|x−y|m DαA(y)f˜ 1(y)dy,
(3.7)
then
TA(f )(x)−TA˜
f2 x0 =KtA(f )(x)−KtA˜ f2 x0
≤ Kt
RmA;˜x,·
|x−·|m f1
(x)
+
|α|=m
1 α!
Kt
(x−·)α
|x−·|mDαAf˜ 1
(x)
+KtA˜
f2 (x)−KtA˜ f2 x0
=A(x)+B(x)+C(x).
(3.8)
Thus, 1
|Q|1+β/n
Q
TAf (x)−TA˜(f ) x0 dx
≤ 1
|Q|1+β/n
Q
A(x)dx+ 1
|Q|1+β/n
Q
B(x)dx+ 1
|Q|1+β/n
Q
C(x)dx :=I+II+III.
(3.9)
Now, we estimate I, II, and III, respectively. First, forx∈Qandy∈Q, using Lemmas˜ 3.3and3.6, we get
Rm
A;˜x, y ≤C|x−y|m
|α|=m
sup
x∈Q˜
DαA(x)−
DαA Q˜
≤C|x−y|m|Q|β/n
|α|=m
DαA˙∧
β. (3.10)
Thus, by Holder’s inequality and theLr boundedness ofT for 1< r < p, we obtain I≤C
|α|=m
DαA∧˙
β
1
|Q|
Q
T
f1 (x)dx
≤C
|α|=m
DαA∧˙
βT
f1 Lr|Q|−1/r
≤C
|α|=m
DαA∧˙
βf1Lr|Q|−1/r
≤C
|α|=m
DαA∧˙
βMr(f )(x).˜
(3.11)
Secondly, for 1< r < q, using the inequality (see [9]) DαA−
DαA Q˜f χQ˜Lr ≤C|Q|1/r+β/nDαA∧˙
βMr(f )(x), (3.12) and similar to the proof of I, we obtain
II≤ C
|Q|1+β/n
|α|=m
T DαA−
DαA Q˜ f χQ˜ Lr|Q|1−1/r
≤C|Q|−β/n−1/r
|α|=m
DαA−
DαA Q˜ f χQ˜Lr
≤C
|α|=m
DαA˙
∧βMr(f )(x).˜
(3.13)
For III, using the size condition ofTA, we have III≤C
|α|=m
DαA˙
∧βM(f )(˜x). (3.14)
Putting these estimates together, taking the supremum over allQsuch that ˜x∈Q, and using theLpboundedness ofMr forr < p, we obtain
TA(f )˙
Fpβ,∞≤C
|α|=m
DαA∧˙
βfLp. (3.15)
This completes the proof of (a).
(b) By the same argument as in the proof of (a), we have 1
|Q|
Q
TA(f )(x)−TA˜
f2 x0 dx≤C
|α|=m
DαA∧˙
β
Mβ,r(f )+Mβ,1(f ) , (3.16)
thus,
TA(f ) #≤C
|α|=m
DαA∧˙
β
Mβ,r(f )+Mβ,1(f ) . (3.17)
Now, usingLemma 3.4, we obtain TA(f )Lq≤CTA(f ) #Lq
≤C
|α|=m
DαA˙∧
βMβ,r(f )Lq+Mβ,1(f )Lq ≤CfLp. (3.18) This completes the proof of (b) and the theorem.
To prove Theorems2.5,2.6, and2.7, it suffices to verify thatgψA,µAΩ, andBδ,A∗satisfy the size condition in theTheorem 3.1.
Suppose suppf⊂Q˜candx∈Q=Q(x0, l). Note that|x0−y| ≈ |x−y|fory∈Q˜c. ForgψA, we write
FtA˜(f )(x)−FtA˜(f ) x0
=
Rn\Q˜
ψt(x−y)
|x−y|m −ψt
x0−y x0−ym
Rm
A;˜x, y f (y)dy
+
Rn\Q˜
ψt
x0−y f (y) x0−ym
Rm
A;x, y˜ −Rm
A;˜x0, y dy
−
|α|=m
1 α!
Rn\Q˜
ψt(x−y)(x−y)α
|x−y|m −ψt
x0−y x0−y α x0−ym
×DαA(y)f (y)dy˜
=I1+I2+I3.
(3.19)
By the condition ofψ, we obtain I1≤C
Rn\Q˜
x−x0 x0−ym+1Rm
A;˜x, y f (y)
× ∞
0
t dt
t+x0−y 2(n+1) 1/2
dy +C
Rn\Q˜
x−x0ε x0−ymRm
A;˜x, y f (y)
× ∞
0
t dt
t+x0−y 2(n+1+ε) 1/2
dy
≤C
Rn\Q˜
x−x0
x0−ym+n+1+ x−x0ε x0−ym+n+ε
Rm
A;˜x, y f (y)dy
≤C
|α|=m
DαA˙
∧β|Q|β/n
× ∞ k=0
2k+1Q\2˜ k+1Q˜
x−x0
x0−yn+1+ x−x0ε x0−yn+ε
f (y)dy
≤C
|α|=m
DαA∧˙
β|Q|β/n ∞ k=1
2−k+2−kε 1 2kQ˜
2kQ˜
f (y)dy
≤C
|α|=m
DαA∧˙
β|Q|β/n ∞ k=1
2−k+2−kε M(f )(x)
≤C
|α|=m
DαA∧˙
β|Q|β/nM(f )(x).
(3.20) For I2, by the formula (see [4])
RmA;˜x, y −RmA;˜x0, y =
|η|<m
1
η!Rm−|η|
DηA;x, x˜ 0 (x−y)η (3.21)
andLemma 3.6, we get Rm
A;x, y˜ −Rm
A;˜x0, y ≤C
|α|=m
DαA˙∧
β|Q|β/nx−x0x0−ym−1. (3.22) Thus, similar to the proof of I1,
I2≤C
Rn\Q˜
Rm
A;˜x, y −Rm
A;˜x0, y
x0−ym+n f (y)dy
≤C
|α|=m
DαA∧˙
β|Q|β/n ∞ k=0
2k+1Q\2˜ kQ˜
x−x0
x0−yn+1f (y)dy
≤C
|α|=m
DαA∧˙
β|Q|β/nM(f )(x).
(3.23)
For I3, byLemma 3.5, we get DαA(y)−
DαA Q˜≤DαA˙
∧βx0−yβ. (3.24) Thus, similar to the proof of I1, we obtain
I3≤C
|α|=m
Rn\Q˜
x−x0
x0−yn+1+ x−x0ε x0−yn+ε
f (y)DαA(y)˜ dy
≤C
|α|=m
DαA˙
∧β|Q|β/n ∞ k=1
2k(β−1)+2k(β−ε) M(f )(x)
≤C
|α|=m
DαA˙∧
β|Q|β/nM(f )(x).
(3.25)
So,
FtA˜(f )(x)−FtA˜(f )
x0 ≤C
|α|=m
DαA∧˙
β|Q|β/nM(f )(x). (3.26)
ForµAΩ, we write FtA˜(f )(x)−FtA˜(f )
x0
≤
∞
0
|x−y|≤t
Ω(x−y)Rm
A;˜x, y
|x−y|m+n−1 f (y)dy
−
|x0−y|≤t
Ω
x0−y Rm
A;˜x0, y
x0−ym+n−1 f (y)dy
2dt t3
1/2
+C
|α|=m
∞
0
|x−y|≤t
Ω(x−y)(x−y)α
|x−y|m+n−1
−
|x0−y|≤t
Ω
x0−y x0−y α x0−ym+n−1
×DαA(y)f (y)dy˜
2dt t3
1/2
≤
∞
0
|x−y|≤t,|x0−y|>t
Ω(x−y)Rm
A;˜x, y
|x−y|m+n−1 f (y)dy 2
dt t3
1/2
+
∞
0
|x−y|>t,|x0−y|≤t
Ω
x0−y Rm
A;x˜ 0, y
x0−ym+n−1 f (y)dy 2
dt t3
1/2
+
∞
0
|x−y|≤t,|x0−y|≤t
Ω(x−y)Rm
A;˜x, y
|x−y|m+n−1 −Ω
x0−y Rm
A;˜x0, y x0−ym+n−1
×f (y)dy 2
dt t3
1/2
+C
|α|=m
∞
0
|x−y|≤t
Ω(x−y)(x−y)α
|x−y|m+n−1
−
|x0−y|≤t
Ω
x0−y x0−y α x0−ym+n−1
×DαA(y)f (y)dy˜
2dt t3
1/2
:=J1+J2+J3+J4.
(3.27)
Thus
J1≤C
Rn\Q˜
f (y)Rm
A;˜x, y
|x−y|m+n−1
|x−y|≤t<|x0−y|
dt t3
1/2
dy
≤C
Rn\Q˜
f (y)Rm
A;˜x, y
|x−y|m+n−1
x0−x1/2
|x−y|3/2 dy
≤C
|α|=m
DαA˙
∧β|Q|β/n∞
k=1
2−k/22kQ˜−1
2kQ˜
f (y)dy
≤C
|α|=m
DαA∧˙
β|Q|β/nM(f )(x).
(3.28)
Similarly, we haveJ2≤C
|α|=mDαA∧˙β|Q|β/nM(f )(x).
ForJ3, by the inequality (see [11])
Ω(x−y)
|x−y|m+n−1− Ω x0−y x0−ym+n−1
≤C x−x0
x0−ym+n+ x−x0γ x0−ym+n−1+γ
, (3.29)
we obtain
J3≤C
|α|=m
DαA∧˙
β|Q|β/n
Rn\Q˜
x−x0
x0−yn+ x−x0γ x0−yn−1+γ
×
|x0−y|≤t,|x−y|≤t
dt t3
1/2
f (y)dy
≤C
|α|=m
DαA∧˙
β|Q|β/n ∞ k=1
2−k+2−γk M(f )(x)
≤C
|α|=m
DαA˙
∧β|Q|β/nM(f )(x).
(3.30)
ForJ4, similar to the proof ofJ1,J2, andJ3, we obtain
J4≤C
|α|=m
Rn\Q˜
x−x0
x0−yn+1+ x−x01/2
x0−yn+1/2+ x−x0γ x0−yn+γ
×DαA(y)˜ f (y)dy
≤C
|α|=m
DαA˙
∧β|Q|β/n
× ∞ k=1
2k(β−1)+2k(β−1/2)+2k(β−γ) 1 2kQ˜
2kQ˜
f (y)dy
≤C
|α|=m
DαA∧˙
β|Q|β/nM(f )(x).
(3.31)
ForBAδ,∗, we write
Bδ,tA˜(f )(x)−Bδ,tA˜(f ) x0
=
Rn\Q˜
Btδ(x−y)
|x−y|m −Btδ x0−y x0−ym
Rm
A;˜x, y f (y)dy
+
Rn\Q˜
Btδ x0−y x0−ym
Rm
A;˜x, y −Rm
A;˜x0, y f (y)dy
−
|α|=m
1 α!
Rn\Q˜
Bδt(x−y)(x−y)α
|x−y|m −Btδ
x0−y x0−y α x0−ym
×DαA(y)f (y)dy˜
=L1+L2+L3.
(3.32)
We consider the following two cases.
Case1(0< t≤l). In this case, notice that (see [8]) Bδ(z)≤c
1+|z| −(δ+(n+1)/2). (3.33)
We obtain L1≤Ct−n
Rn\Q˜
f (y)Rm
A;˜x, y x0−ym
1+|x−y|/t −(δ+(n+1)/2)dy
≤C
|α|=m
DαA˙∧
β|Q|β/n(t/l)δ−(n−1)/2
× ∞ k=1
2k((n−1)/2−δ) 1 2kQ˜
2kQ˜
f (y)dy
≤C
|α|=m
DαA˙∧
β|Q|β/nM(f )(x), L2≤Ct−n
Rn\Q˜
f (y)Rm
A;˜x, y −Rm
A;˜x0, y x0−ym
×
1+|x−y|/t −(δ+(n+1)/2)dy
≤C
|α|=m
DαA˙
∧β|Q|β/n(t/l)δ−(n−1)/2
× ∞ k=1
2k((n−1)/2−δ) 1 2kQ˜
2kQ˜
f (y)dy
≤C
|α|=m
DαA˙∧
β|Q|β/nM(f )(x).
(3.34)
ForL3, similar to the proof ofL1, we get L3≤C
|α|=m
DαA∧˙
β|Q|β/n(t/l)δ−(n−1)/2
× ∞ k=1
2k(β−δ+(n−1)/2) 1 2kQ˜
2kQ˜
f (y)dy
≤C
|α|=m
DαA˙
∧β|Q|β/nM(f )(x).
(3.35)
Case2(t > l). In this case, we chooseδ0such thatβ+(n−1)/2< δ0<min(δ, (n+ 1)/2). Notice that (see [8])
(∂/∂z)Bδ(z)≤C
1+|z| −(δ+(n+1)/2). (3.36)
Similar to the proof ofCase 1, we obtain L1≤Ct−n
Rn\Q˜
f (y)Rm
A;˜x, y x0−ym+1
×x0−x1+x0−y/t −(δ0+(n+1)/2)dy +Ct−n−1
Rn\Q˜
f (y)RmA;˜x, y x0−ym
×x0−x1+x0−y/t −(δ0+(n+1)/2)dy
≤C
|α|=m
DαA∧˙
β|Q|β/n(l/t)(n+1)/2−δ0
× ∞ k=1
2k((n−1)/2−δ0) 1 2kQ˜
2kQ˜
f (y)dy
≤C
|α|=m
DαA∧˙
β|Q|β/nM(f )(x), L2≤Ct−n
Rn\Q˜
f (y)RmA;˜x, y −RmA;˜x0, y x0−ym
×
1+x0−y/t −(δ0+(n+1)/2)dy
≤C
|α|=m
DαA˙
∧β|Q|β/n(l/t)(n+1)/2−δ0
× ∞ k=1
2k((n−1)/2−δ0) 1 2kQ˜
2kQ˜
f (y)dy
≤C
|α|=m
DαA∧˙
β|Q|β/nM(f )(x),
L3≤C
|α|=m
DαA∧˙
β|Q|β/n(l/t)(n+1)/2−δ0
× ∞ k=1
2k(β+(n−1)/2−δ0) 1 2kQ˜
2kQ˜
f (y)dy
≤C
|α|=m
DαA˙
∧β|Q|β/nM(f )(x).
(3.37) These yield the desired results.
Acknowledgment. This work was supported by the National Natural Science Foun- dation (NNSF) Grant 10271071.
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30(1981), no. 5, 693–702.
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Liu Lanzhe: Department of Applied Mathematics, Hunan University, Changsha 410082, China E-mail address:[email protected]
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