• 検索結果がありません。

MAXIMAL FUNCTIONS

N/A
N/A
Protected

Academic year: 2022

シェア "MAXIMAL FUNCTIONS"

Copied!
17
0
0

読み込み中.... (全文を見る)

全文

(1)

MAXIMAL FUNCTIONS

AHMAD AL-SALMAN

Received 16 January 2006; Revised 12 April 2006; Accepted 13 April 2006

We establishLpestimates for certain class of maximal functions with kernels inLq(Sn1).

As a consequence of suchLp estimates, we obtain theLpboundedness of our maximal functions when their kernels are inL(logL)1/2(Sn1) or in the block spaceB0,q1/2(Sn1), q >1. Several applications of our results are also presented.

Copyright © 2006 Ahmad Al-Salman. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

1. Introduction and statement of results

LetRn,n2, be then-dimensional Euclidean space and let Sn1 be the unit sphere in Rnequipped with the normalized Lebesgue measuredσ. For nonzeroyRn, we will let y= |y|1y. LetΩbe an integrable function on Sn1that is homogeneous of degree zero onRnand satisfies the cancelation property

Sn1Ω(y)dσ(y)=0. (1.1)

Consider the maximal functionᏹΩ, ᏹΩ(f)(x)=sup

hU

Rn f(xy)|y|nh|y|

Ω(y)d y, (1.2) whereUis the class of allhL2(R+,r1dr) withhL2(R+,r1dr)1.

The operator ᏹΩ was introduced by Chen and Lin [7]. They showed that ᏹΩ is bounded on Lp(Rn) for all p >2n/(2n1) provided that ΩᏯ(Sn1). Recently, we have been able to show that theLp(Rn) boundedness ofᏹΩ still holds for all p2 if the conditionΩ(Sn1) is replaced by the more natural and weaker conditionΩ L(logL)1/2(Sn1) [2]. Moreover, we showed that if the conditionΩL(logL)1/2(Sn1) is replaced by any condition in the form ΩL(logL)r(Sn1) for some r <1/2, thenᏹΩ

might fail to be bounded onL2.

Hindawi Publishing Corporation Journal of Inequalities and Applications Volume 2006, Article ID 56272, Pages1–17 DOI10.1155/JIA/2006/56272

(2)

On the other hand, whenΩlies inBs0,1/2(Sn1),s >1, which is a special class of block spaces Bqκ,υ(Sn1) (seeSection 5 for the definition), we were able to show thatᏹΩ is bounded on Lp for all p2 [3]. Moreover, we showed that the condition Ω B0,s1/2(Sn1),s >1 is nearly optimal in the sense that the exponent1/2 cannot be re- placed by any smaller number for theL2 boundedness ofᏹΩto hold. We remark here that block spaces have been introduced by Jiang and Lu to improve previously obtained Lpboundedness results for singular integrals [7]. It should be noted here that the relation between the spacesB0,s1/2(Sn1) andL(logL)1/2(Sn1) is unknown.

However, it is known that Lq(Sn1) is properly contained in L(logL)1/2(Sn1) B0,s1/2(Sn1) for all q, s > 1. Moreover, it is not hard to see that every Ω in L(logL)1/2(Sn1)B0,s1/2(Sn1) can be written as an infinite sum of functions inLq(Sn1).

This gives rise to the question whether the results pertaining theLpboundedness ofᏹΩin [2,3] can be obtained via certain correspondingLpestimates with kernels inLq(Sn1). It is one of our main goals in this paper to consider such problem. It should be pointed out here that a positive solution for this problem will not only make life easier when dealing with kernels inL(logL)1/2(Sn1) orB0,s1/2(Sn1), but also will pave the way for extending several results that are known when kernels are inLq(Sn1).

Our work in this paper will be mainly concerned with the following general class of maximal functions:

Ω,P(f)(x)=sup

hU

RneiP(y)f(xy)|y|nh|y|

Ω(y)d y, (1.3) whereP:RnRis a real-valued polynomial.

Clearly, ifP(y)=0, thenᏹΩ,P=Ω. For the significance of considering integral op- erators with oscillating kernels, we refer the readers to consult [1,4,11,16,19,22–24], among others.

Our result concerningLpestimates with kernels inLq(Sn1) is the following theorem.

Theorem 1.1. LetΩLq(Sn1),q >1, be a homogeneous function of degree zero onRn withΩ11. LetP:RnRbe a real-valued polynomial of degreed. LetΩ,Pbe given by (1.3). Then

Ω,P(f)p

1 + log1/2e+Ωq

Cp,qfp (1.4)

for allp2, whereCp,q=(21/q/(21/q1))Cp. Here 1/q=11/qandCpis a constant that may depend on the degree of the polynomialPbut it is independent of the functionΩ, the indexq, and the coefficients of the polynomialP.

We remark here that the constantCp,q inTheorem 1.1satisfiesCp,q→ ∞asq1+. That is, the constantCp,q diverges when q tends to 1. This behavior ofCp,q is natural since, by [2, Theorem B(b)], the special operatorᏹΩ=Ω,0is not bounded onL2if the functionΩis assumed to satisfy only the sole condition thatΩL1(Sn1) (i.e.,q=1).

By a suitable decomposition of the functionΩand an application ofTheorem 1.1, we prove the following theorem which is a proper extension of the corresponding result in [2].

(3)

Theorem 1.2. Suppose thatΩL(log+L)1/2(Sn1) satisfying (1.1). LetP:RnRbe a real-valued polynomial. ThenΩ,P is bounded onLp(Rn) for all p2 withLp bounds independent of the coefficients of the polynomialP.

We should point out here that an alternative proof ofTheorem 1.2can be obtained by observing thatCp,qCp/(q1), whereCp,qis the constant inTheorem 1.1, and then using a Yano-type extrapolation technique [27].

By another suitable application ofTheorem 1.1, we will prove the following extension of [3, Theorem 1.2].

Theorem 1.3. Suppose thatΩB0,q1/2(Sn1),q >1, satisfying (1.1). LetP:RnRbe a real-valued polynomial. ThenΩ,P is bounded onLp(Rn) for all p2 withLpbounds independent of the coefficients of the polynomialP.

As an immediate consequence ofTheorem 1.1and the observation that

TΩ,P,h(f)(x)hL2(R+,r1dr)Ω,P(f)(x), (1.5) we obtain the following result concerning oscillatory singular integrals.

Theorem 1.4. LetΩLq(Sn1),q >1, be a homogeneous function of degree zero onRn with Ω11. Let P : RnR be a real-valued polynomial of degree d and let h L2(R+,r1dr). Then the oscillatory singular integral operatorΩ,P;

TΩ,P,h(f)(x)=p·v

RneiP(y)f(xy)|y|nh|y|

Ωy)d y (1.6) satisfies

TΩ,P,h(f)p

1 + log1/2e+Ωq

hL2(R+,r1dr)Cp,qfp (1.7) for allp2, whereCp,q=(21/q/(21/q1))Cp. Here 1/q=11/qandCpis a constant that may depend on the degree of the polynomialPbut it is independent of the functionΩ, the indexq, and the coefficients of the polynomialP.

ByTheorem 1.4, we obtain the following two results.

Corollary 1.5. Let ΩL(logL)1/2(Sn1) be a homogeneous function of degree zero on Rnand satisfies (1.1). LetP:RnRbe a real-valued polynomial of degreedand leth L2(R+,r1dr). Then the oscillatory singular integral operatorΩ,P;

TΩ,P,h(f)(x)=p·v

RneiP(y)f(xy)|y|nh|y|

Ω(y)d y (1.8) is bounded onLpfor allp2 withLpbounds that may depend on the degree of the polyno- mialPbut they are independent of the coefficients of the polynomialP.

Corollary 1.6. LetΩB0,q1/2(Sn1), s >1, be a homogeneous function of degree zero onRnand satisfies (1.1). LetP:RnRbe a real-valued polynomial of degreedand let

(4)

hL2(R+,r1dr). Then the oscillatory singular integral operatorΩ,P; TΩ,P,h(f)(x)=p·v

RneiP(y)f(xy)|y|nh|y|

Ω(y)d y (1.9) is bounded onLpfor allp2 withLpbounds that may depend on the degree of the polyno- mialPbut they are independent of the coefficients of the polynomialP.

Further applications of the results stated above will be presented inSection 6.

Throughout this paper, the letterCwill stand for a constant that may vary at each occurrence, but it is independent of the essential variables.

2. Preliminary estimates

We start by recalling the following result in [10].

Lemma 2.1 (see [10]). Letᏼ=(P1,. . .,Pd) be a polynomial mapping from Rn intoRd. Suppose thatΩL1(Sn1) and

MΩ,f(x)=sup

j∈Z

2j≤|y|<2j+1

fxᏼ(y)|y|nΩy)d y. (2.1)

Then for 1< p≤ ∞, there exist a constantCp>0 independent ofΩand the coefficients of P1,. . .,Pdsuch that

MΩ,fpCpΩL1(Sn1)fp (2.2) for every f Lp(Rd).

Lemma 2.2 (van der Corput [26]). Supposeφis real valued and smooth in (a,b), and that

|φ(k)(t)| ≥1 for allt(a,b). Then the inequality b

aeiλφ(t)ψ(t)dtCk|λ|1/k (2.3)

holds when (i)k2, or

(ii)k=1 andφis monotonic.

The boundCkis independent ofa,b,φ, andλ.

Lemma 2.3. LetΩLq(Sn1),q >1, be a homogeneous function of degree zero onRnwith Ω11. LetP(x)= |α|≤daαxα be a real-valued polynomial of degreed >1 such that

|x|d is not one of its terms. ForkZ, letEk,Ω: [1, log(e+Ωq)]×P(Sn1)×RCand let Jk,Ω:RnRbe given by

Ek,Ωr,P(y),s=ei[P(2(k+1) log(e+Ωq)r y)+2(k+1) log(e+Ωq)sr], Jk,Ω(ξ)=

22 log(e+Ωq)

1

Sn1Ω(y)Ek,Ω

r,P(y),ξ·ydσ(y)

2d rr.

(2.4)

(5)

Then, Jk,Ωsatisfies

sup

ξ∈Rn

Jk,Ω(ξ)2(k+1)/4qloge+Ωq

|α|=d

aαε/q

C (2.5)

for some 0< ε <1, whereCis a constant that may depend on the degree of the polynomialP but it is independent of the functionΩ, the indexq, and the coefficients of the polynomialP.

Proof ofLemma 2.3. First, we notice the following:

Jk,Ω(ξ)loge+Ωq

, (2.6)

Jk,Ω(ξ)qΩ2qq

Sn1

22 log(e+Ωq)

1 Ek,Ω

r,P(y),ξ·y

×Ek,Ωr,P(z),ξ·zdr r

qdσ(y)dσ(z).

(2.7)

Next, notice that

P2γk,Ωr y+ 2γk,Ω·y)rP2γk,Ωrz+ 2γk,Ω·z)r

=2γk,Ωdrd

|α|=d

aαyα

|α|=d

aαzα

+ 2γk,Ωξ·(yz)r+Hk(r,y,z,ξ) (2.8) with (dd/drd)Hk=0, whereγk,Ω=(k+ 1) log(e+Ωq). Thus, byLemma 2.2, we have

22 log(e+Ωq)

1 Ek,Ω

r,P(y),ξ·yEk,Ω

r,P(z),ξ·zdr r

2k,ΩP(y)P(z)1/d. (2.9) Now, by (2.9) and the inequality

22 log(e+Ωq)

1 Ek,Ωr,P(y),ξ·yEk,Ωr,P(z),ξ·zdr r

Cloge+Ωq

, (2.10)

we obtain

22 log(e+Ωq)

1 Ek,Ωr,P(y),ξ·yEk,Ωr,P(z),ξ·zdr r

2k,ΩP(y)P(z)1/4dqCloge+Ωq

11/4q

.

(2.11)

Therefore, by (2.7), (2.11), and [12, (3.11)], we obtain Jk,Ω(ξ)2γk,Ω/4qΩ2qqCloge+Ωq

11/4q

. (2.12)

(6)

Hence, by (2.6) and (2.12), we get

Jk,Ω(ξ)2γk,Ω/4 log(e+Ωq)qΩ2/qlog(e+Ωq)loge+Ωq

2(k+1)/4qloge+Ωq C.

(2.13)

This completes the proof.

Now, we will need the following lemma.

Lemma 2.4. LetΩLq(Sn1),q >1, be a homogeneous function of degree zero onRnwith Ω11. Then

Ω(f)plog1/2e+Ωq

21/q 21/q1

Cpfp (2.14)

for allp2 with constantsCpindependent of the functionΩand the indexq.

We remark here that sinceLq(Sn1)Llog1/2L, it follows from [2, Theorem B(a)] that ΩpΩqCpfor allp2. But, clearly the constant{1 + log1/2(e+Ωq)}in (2.14) is sharper than the constantΩqthat can be deduced from [2, Theorem B(a)]. However, the former constant can be obtained by following a similar argument as in the proof of Theorem B(a) in [2] and keeping track of certain constants. For completeness, we, below, present the main ideas of the proof.

Proof ofLemma 2.4. Choose a collection of functions {ωk}k∈Z on (0,) with the properties sup(ωk)[2log(e+Ωq)(k+1), 2log(e+Ωq)(k1)], 0ωk1, k∈Zωk(u)=1,

|(dsωk/dus)(u)| ≤Csus, whereCsis a constant independent of log(e+Ωq). ForkZ, letGkbe the operator defined by (Gk(f))(ξ)=ωk(|ξ|)f(ξ). Let

Ej(f)(x)=

k∈Z

22 log(e+Ωq) 1

Sn1Ω(y)Gk+j(f)x2klog(e+Ωq)r ydσ(y)

2

r1dr 1/2

. (2.15) Then

Ω(f)(x)

j∈Z

Ej(f)(x). (2.16)

By exactly the same argument in [2], we obtain

Ej(f)2C2β|j|/qlog1/2e+Ωq

f2. (2.17)

On the other hand, by a duality argument; see (3.24)-(3.25) for similar argument, we get Ej(f)pClog1/2e+Ωq

fp (2.18)

for all 2< p <. Thus, by interpolation between (2.17) and (2.18), we have Ej(f)pC2ε(|j|/q)log1/2e+Ωq

fp (2.19)

(7)

for someε >0 and for all 2p <, andjZwith constantCindependent ofΩ,k, and j. Hence, (2.14) follows by (2.16) and (2.19). This completes the proof.

3. Proof ofTheorem 1.1

Proof ofTheorem 1.1. We will argue by induction on the degree of the polynomialP. If d=deg(P)=0, then (1.4) follows easily fromLemma 2.4. In fact, ifd=0, then by duality it can be easily seen that

Ω,P(f)(x)CΩ(f)(x). (3.1) Thus, byLemma 2.4, we have

Ω,P(f)p 21/q

21/q1

log1/2e+Ωq

Cpfp

21/q

21/q1

1 + log1/2e+Ωq

Cpfp

(3.2)

for allp2.

Now, ifd=1, that is,P(y)= −a·yfor someaRn, then by (3.2), we have Ω,P(f)p

21/q 21/q1

log1/2Ωq Cpgp

= 21/q

21/q1

1 + log1/2e+Ωq

Cpfp,

(3.3)

whereg(y)=eiP(y)f(y).

Next, assume that (1.4) holds for all polynomialsQ of degree less than or equal to d >1. Let

P(x)=

|α|≤d+1

aαxα (3.4)

be a polynomial of degreed+ 1. Then by duality, we have ᏹΩ,P(f)(x)=

0

Sn1eiP(r y)Ω(y)f(xr y)dσ(y)

2

r1dr 1/2

. (3.5) We may assume thatPdoes not contain|x|d+1as one of its terms. By dilation invari- ance, we may also assume that

|α|=d+1

aα=1. (3.6)

(8)

We now choose a collection{ωk}k∈ZofᏯfunctions defined on (0,) that satisfy the following properties:

suppψk

2log(e+Ωq)(k+1), 2log(e+Ωq)(k1), 0ψk1,

k∈Z

ψk(u)=1. (3.7)

Set

η(u)= 0 k=−∞

ψk(u), η0(u)= k=1

ψk(u). (3.8)

Then,

η(u) +η0(u)=1, suppη(u)

2log(e+Ωq),

, suppη0(u)(0, 1]. (3.9) Define the operators᏿Ω,P,and᏿Ω,P,0by

Ω,P,(f)(x)=

2log(e+Ωq)

η(r)

Sn1eiP(r y)Ω(y)f(xr y)dσ(y)

2

r1dr 1/2

,

Ω,P,0(f)(x)= 1

0

η0(r)

Sn1eiP(r y)Ω(y)f(xr y)dσ(y)

2

r1dr 1/2

. (3.10) Thus, by (3.9), we have

Ω,P(f)(x)Ω,P,0(f)(x) +᏿Ω,P,(f)(x). (3.11) Now, we estimateΩ,P,0p.

Let

Q(x)=

|α|≤d

aαxα. (3.12)

Assume that deg(Q)=l, where 0ld. Define the operators(1)Ω,P,0and᏿(2)Ω,Q,0by

(1)Ω,P,0(f)(x)= 1

0

Sn1

eiP(r y)eiQ(r y)Ω(y)f(xr y)dσ(y)

2

r1dr 1/2

,

(2)Ω,Q,0(f)(x)= 1

0

Sn1eiQ(r y)Ω(y)f(xr y)dσ(y)

2

r1dr 1/2

.

(3.13)

Now, by the observation thatη0(r)1 and by Minkowski’s inequality, we obtain

Ω,P,0(f)(x)(1)Ω,P,0(f)(x) +᏿Ω(2),Q,0(f)(x). (3.14)

(9)

By induction assumption, it follows that (2)Ω,Q,0(f)p

1 + log1/2(e+Ωq) 21/q 21/q1

Cpfp (3.15) for allp2.

On the other hand, by Cauchy-Schwarz inequality, by the fact thatΩ11, and the inequality

eiP(r y)eiQ(r y)rd+1

|α|=d+1

aαyα

rd+1,

(3.16)

we get

Ω,P,0(1) (f)(x) 1

0

Sn1

eiP(r y)eiQ(r y)2Ω(y)f(xr y)2dσ(y)r1dr 1/2

1

0

Sn1

Ω(y)f(xr y)2dσ(y)r2d+1dr 1/2

= 1

j=−∞

2j+1 2j

Sn1

Ω(y)f(xr y)2dσ(y)r2d+1dr 1/2

1

j=−∞

2(2d+2)j 2j+1

2j

Sn1

Ω(y)f(xr y)2dσ(y)r1dr 1/2

CMΩ|f|21/2

(x),

(3.17) whereMΩis the operator given by (2.1) withᏼ(y)=y. Thus, by (3.17), by the fact that Ω11, andLemma 2.1, we obtain

(1)Ω,P,0(f)pCpfp (3.18)

for allp2 with constantCpindependent of the functionΩand the coefficients of the polynomialP. Therefore, by (3.14), by Minkowski’s inequality, by (3.15), and (3.18), we obtain

Ω,P,0(f)p

1 + log1/2e+Ωq

21/q 21/q1

Cpfp (3.19) for allp2.

(10)

Finally, we prove theLpboundedness of᏿Ω,P,. By generalized Minkowski’s inequal- ity, we can write᏿Ω,P,as

Ω,P,(f)(x)=

2log(e+Ωq)

η(r)

Sn1eiP(r y)Ω(y)f(xr y)dσ(y)

2

r1dr 1/2

=

0

0 k=−∞

ψk(r)

Sn1eiP(r y)Ω(y)f(xr y)dσ(y)

21 rdr

1/2

0 k=−∞

Ω,P,,k(f)(x),

(3.20) where

Ω,P,,k(f)(x)=

2log(e+Ωq)(k1)

2log(e+Ωq)(k+1)

Sn1eiP(r y)Ω(y)f(xr y)dσ(y)

2

r1dr 1/2

. (3.21) By Plancherel’s theorem, Fubini’s theorem, andLemma 2.3, we have

Ω,P,,k(f)22=

Rn f(ξ)2Jk,Ω(ξ)dξ2(k+1)/4qloge+Ωq

f22. (3.22) Thus,

Ω,P,,k(f)22(k+1)/8qlog1/2e+Ωq

f2. (3.23)

Now, forp >2, choosegL(p/2)withg(p/2)=1 such that Ω,P,,k(f)2p

=

Rn

22 log(e+Ωq) 1

Sn1Ek,Ωr,P(y), 0Ω(y)fx2γk,Ωr ydσ(y)

2

r1drg(x)dx

Rn

f(z)2

22 log(e+Ωq) 1

Sn1

Ω(y)gz+ 2γk,Ωr ydσ(y)dr

r dz

Cloge+Ωq

f2pMΩg(z) (p/2),

(3.24) whereMΩ is the operator given by (2.1) withᏼ(y)=y. Thus,Lemma 2.1 and (3.24) imply that

Ω,P,,k(f)plog1/2e+Ωq

Cfp, (3.25)

which when combined with (3.23) implies

Ω,P,,k(f)p2(k+1)δ/8qlog1/2e+Ωq

Cfp, (3.26)

参照

関連したドキュメント

Ouahab, Existence results for second order boundary value problem of impulsive dynamic equations on time scales, Journal of Mathematical Analysis and Applications 296 (2004),

Schinas, Global asymptotic stability and oscillation of a family of difference equations, Journal of Mathematical Analysis and Applications 294 (2004), no. Thompson, On

He, Existence of two solutions of m-point boundary value problem for second order dynamic equations on time scales, Journal of Mathematical Analysis and Applications 296 (2004),

MÜLLER, Damped oscillatory integrals and boundedness of maximal operators associated to mixed homogeneous hypersurfaces, Duke Math. RICCI

The method of proof is applied in a random discrete setting, yielding the first weighted inequalities for operators defined on sparse sets of

By means of an expression with a kind of integral operators, some properties of the weighted Hadamard-type singular integrals are revealed.. As applications, the solution for

Agarwal, “Multiple positive solutions to superlinear periodic boundary value problems with repulsive singular forces,” Journal of Mathematical Analysis and Applications, vol..

Pan, A singular integral operator with rough kernel, Proceedings of the American Mathematical Society 125 (1997), no.. Yang, A weighted norm inequality for rough singular integrals,