• Aucun résultat trouvé

L’INSTITUTFOURIER DE ANNALES

N/A
N/A
Protected

Academic year: 2022

Partager "L’INSTITUTFOURIER DE ANNALES"

Copied!
22
0
0

Texte intégral

(1)

A L

E S

E D L ’IN IT ST T U

F O U R

ANNALES

DE

L’INSTITUT FOURIER

R. V. BESSONOV

Schatten properties of Toeplitz operators on the Paley–Wiener space Tome 68, no1 (2018), p. 195-215.

<http://aif.cedram.org/item?id=AIF_2018__68_1_195_0>

© Association des Annales de l’institut Fourier, 2018, Certains droits réservés.

Cet article est mis à disposition selon les termes de la licence CREATIVECOMMONS ATTRIBUTIONPAS DE MODIFICATION3.0 FRANCE. http://creativecommons.org/licenses/by-nd/3.0/fr/

L’accès aux articles de la revue « Annales de l’institut Fourier »

(http://aif.cedram.org/), implique l’accord avec les conditions générales d’utilisation (http://aif.cedram.org/legal/).

cedram

Article mis en ligne dans le cadre du

(2)

SCHATTEN PROPERTIES OF TOEPLITZ OPERATORS ON THE PALEY–WIENER SPACE

by R. V. BESSONOV (*)

Abstract. — We collect several old and new descriptions of Schatten class Toeplitz operators on the Paley–Wiener space and answer a question on discrete Hilbert transform commutators posed by Richard Rochberg.

Résumé. — Nous présentons plusieurs descriptions anciennes et nouvelles des opérateurs de Toeplitz de classe de Schatten sur l’espace de Paley-Wiener et ré- pondons à une question de Richard Rochberg sur les commutateurs discrets de la transformée de Hilbert.

1. Introduction

Given a bounded function ϕ on the real line, R, consider the Toeplitz operatorTϕon the classical Paley–Wiener space PWa,

(1.1) Tϕ:f 7→Pa(ϕf), f ∈PWa.

The space PWa could be regarded as the subspace in L2(R) of functions with Fourier spectrum in the interval [−a, a], symbolPa above denotes the orthogonal projection inL2(R) to PWa. Basic theory of Toeplitz operators on PWa can be found in paper [9] by R. Rochberg.

We are interested in description of Schatten class Toeplitz operators on PWa in terms of their standard symbols. By the standard symbol of an operator in (1.1) we mean the entire functionϕst =F−1χ2aFϕ, whereF denotes the Fourier transform on the Schwartz space of tempered distri- butions, andχ2a is the indicator function of the interval (−2a,2a). As we

Keywords:Paley–Wiener space, Schatten ideal, discrete Besov space, discrete Hilbert transform commutator.

2010Mathematics Subject Classification:47B35, 46E39.

(*) The work is supported by RFBR grant mol_a_dk 16-31-60053, by Grant MD- 5758.2015.1, and by “Native towns”, a social investment program of PJSC “Gazprom Neft”.

(3)

will see, a Toeplitz operatorTϕon PWa belongs to the Schatten classSp, 0< p <∞, if and only if e2iaxϕst belongs to a discrete oscillation Besov space introduced in 1987 by R. Rochberg [9]. Its definition we now recall.

For a measureµonRand a functionfL1loc(µ), the oscillation of order nof f on an intervalI⊂Rwith respect toµis defined by

osc(f, I, µ, n) = inf

Pn

1 µ(I)

Z

I

|f(x)−Pn(x)|dµ(x),

where the infimum is taken over all polynomialsPn of degree at mostn. If µ(I) = 0, we put oscI(f, I, µ, n) = 0. Define the familyIaof closed intervals

Ia,j,k= 2π

a k2j,

a (k+ 1)2j

, j, k∈Z, j>0.

Note that endpoints of intervals inIabelong to the latticeZa=

ak, k∈ Z . Letpbe a positive real number, and let [1p] be the integer part of1p. The discrete oscillation Besov spaceBp(a,osc) =B1/pp,p(Za, µa,osc) is defined by

Bp(a,osc) = (

fL1loca) :kfkp

Bp(a,osc)=X

I∈Ia

osc

f, I, µa, 1

p p

<∞ )

,

whereµa= a P

x∈Zaδx is the normalized counting measure onZa. Our main result is the following theorem.

Theorem 1.1. — Leta,pbe positive real numbers, letϕbe a bounded function on R, and let ϕst be the standard symbol of the Toeplitz oper- atorTϕ on PWa. Then we have Tϕ ∈ Sp(PWa) if and only ife2iaxϕst ∈ Bp(4a,osc). Moreover, kTϕkSp is comparable to ke2iaxϕstkBp(4a,osc) with constants depending only onp.

Theorem 1.1 complements a classical description of Toeplitz operators in Sp(PWa) given by R. Rochberg [9] for 1 6 p < ∞ and extended by V. Peller [5] to the whole range 0 < p < ∞. To formulate the result, consider a system{νj}j6−1 of infinitely smooth functions on Rsuch that suppνj ⊂[2j−1,2j],

06νj61, νj−1(x) =νj(x/2), X

νj= 1 on

0,1 3

.

Define νj(x) = ν−j(1−x) for real x > 12 and integer j > 1, put ν0 = 1−P

j6=0νjforj= 0. Finally, letνa,j(x) =νj((x+a)/2a) for allx∈[−a, a]

andj∈Z. Observe that system{νa,j}provides a resolution of unity on the interval [−a, a] by functions supported on subintervalsIjwhose lengths are

(4)

comparable to the distance fromIj to the endpoints of [−a, a]. Rochberg–

Peller theorem says that Tϕ is in Sp(PWa) for 0 < p < ∞ if and only if

aX

j∈Z

2−|j|· kF−12a,j· Fϕ)kpLp(R)<∞,

with control of the norms. R. Rochberg gives yet another characterization of Toeplitz operators in classSp(PWa), 16p <∞, in terms of a reproducing kernel decomposition of their standard symbols, see Theorem 5.3 in [9].

Both the statement and the proof of his result forp= 1 contain errors that we correct in Section 3.

As a consequence of Theorem 1.1, we obtain the following result.

Theorem 1.2. — Leta >0. The discrete Hilbert transform commuta- tor

Cψ:f 7→ 1 π

Z

Za

ψ(x)ψ(t)

xt f(t) dµa(t), fL2a),

belongs to the trace classS1(L2a))if and only ifψ∈B1(a,osc)∩L(Za).

This answers the question posed by R. Rochberg in 1987. See Section 6 for a summary of results on discrete Hilbert transform commutators and an analogue of Theorem 1.2 for the case 0< p <1.

We would like to mention papers [11, 12] by R. Torres for readers in- terested in wavelet characterizations and interpolation theory of discrete Besov spaces. The problem of membership in Schatten classesSp for gen- eral truncated Toeplitz operators has been recently studied by P. Lopatto and R. Rochberg [3], see also Section 4.3 in author’s paper [1].

2. Proof of Theorem 1.1 for 1< p <

Theorem 1.1 for 1 < p < ∞ follows from known results. Let Bp(R) = B˙1/pp,p(R) be the standard homogeneous Besov space on the real lineR, see, e.g., Chapter 3 in [4] for definition and basic properties. Given a Toeplitz operatorTϕon PWa with symbolϕL(R), we denote

ϕst=F−1χ(−2a,0)Fϕ, ϕ+st=F−1χ[0,2a)Fϕ,

whereχS is the indicator function of a setS. As usual, F stands for the Fourier transform on the Schwartz space of tempered distributions. The following result is a combination of Theorem 5.1 and its Corollary in [9].

(5)

Theorem (R. Rochberg). — Let 1 < p < ∞ and let a > 0. Then a Toeplitz operatorTϕonPWa belongs toSp(PWa)if and only if

ke2iaxϕstkBp(R)+ke−2iaxϕ+stkBp(R)<∞,

in which casekTϕkSpis comparable toke2iaxϕstkBp(R)+ke−2iaxϕ+stkBp(R) with constants depending only onp.

Denote byEathe set of tempered distributions whose Fourier transforms are supported on the interval [−a, a]. Next result is Theorem 1 in [12].

Theorem (R. Torres). — Let 1 < p < ∞ and let f be a function in Ea∩Bp(R)for somea >0. Then its restriction toZ2a belongs toBp(2a,osc) andkfkBp(2a,osc)is comparable tokfkBp(R)with constants depending only onp. Moreover, every sequence in Bp(a,osc) is the restriction toZa of a unique function (modulo polynomials) inEa∩Bp(R).

Proof of Theorem 1.1(1< p <∞). — Letϕbe a bounded function of Rand let ϕst =F−1χ(−2a,2a)Fϕbe the standard symbol of the Toeplitz operator Tϕ ∈ Sp(PWa). Then functions e2iaxϕst, e−2iaxϕ+st belong to E2a∩Bp(R) by R. Rochberg’s theorem above. From theorem by R. Torres we see that e2iaxϕst∈Bp(4a,osc) and e−2iaxϕ+st∈Bp(4a,osc) with control of the norms. Now observe that e4iax= 1 and e2iaxϕst= e2iaxϕst+ e−2iaxϕ+st onZ4a, hence e2iaxϕst∈Bp(4a,osc).

Conversely, assume that the restriction of e2iaxϕsttoZ4ais inBp(4a,osc).

Using theorem by R. Torres, find a functionf ∈ E2a∩Bp(R) such that its restriction to Z4a agrees with e2iaxϕst. Put f = F−1χ(−2a,0)Ff and f+ = F−1χ[0,2a)Ff. Observe that ˜ϕ = e−2iaxf+ + e2iaxf is an en- tire function of exponential type at most 2a coinciding with ϕst onZ4a. Since ϕst, ˜ϕ are the first order distributions supported on the finite in- terval [−2a,2a], we have |ϕ(x)|˜ +|ϕ(x)| 6 c+c|x| for all x ∈ R and a constant c > 0. It follows that the entire function ϕ−ϕ˜z of exponen- tial type at most 2a is bounded on R and vanishes on Z4a\ {0}, hence

˜

ϕϕst=psin(2az) for a polynomialpof degree at most 1. Therefore, we have Tϕ =Tϕst =Tϕ˜ on PWa, see Section 2.D in [9]. Since f± ∈Bp(R), we can use R. Rochberg’s theorem and conclude that Tϕ˜ ∈ Sp(PWa) with control of the norms: kTϕ˜kSp is controllable by ke2iaxϕ˜kBp(R)+ ke−2iaxϕ˜+kBp(R)6cpkfkBp(R)6c˜pke2iaxϕstkBp(4a,osc).

3. Reproducing kernel decomposition of standard symbols In this section we show that the standard symbol of a Toeplitz opera- tor on PWa from class Sp could be represented as a linear combination

(6)

of normalized reproducing kernels of PW2a with coefficients ck such that P|ck|p<∞. We consider only the case 0< p61. Proposition 3.1 below is a corrected version of Theorem 5.3 in [9]. In the original statement the au- thor of [9] forgot to normalize the exponentials in formula (5.6) of [9]. More importantly, he used the fact that the Fourier multiplierf 7→ F−1χ[0,1]Ff is bounded onBp(R). This is not the case forp= 1. Here is a more accurate implementation of the ideas from [9].

Let ψbe a bounded function on the real line R. Consider the standard Hardy spaceH2 in the upper half-planeC+={λ∈C: Imλ >0} of the complex planeC. Denote by H2 the anti-analytic subspace{f ∈L2(R) : f¯∈H2}ofL2(R). Recall that the classical Hankel operatorHψ:H2H2 is defined by

Hψ:f 7→P(ψf), fH2,

where P denotes the orthogonal projection from L2(R) to H2. The op- erator Hψ is completely determined by its standard anti-analytic symbol ψst=F−1χ(−∞,0)Fψ. The latter means thatHψf =Hψstf for allfH2 such that supx∈R|xf(x)| < ∞. Take a positive number ε > 0 and define the setsUε+,Uε by

Uε±={λ∈C: λ= (1 +ε)m(εx±i); x, m∈Z}.

Forλ∈C+, letkλ=−2πi1 z−1λ¯ denote the reproducing kernel ofH2 atλ.

Theorem (R. Rochberg [8]). — There exists a numberε >0such that Hψ ∈ Sp(H2) if and only if ψst = P

λ∈Uε+cλ kλ

kkλk2, where P

|cλ|p is fi- nite and the infimum of P|cλ|p over all possible representations of ψst

in this form is comparable to kHψkpSp with constants depending only on p∈(0,∞).

Remark that for p∈(0,1] the series definingψst in the theorem above converges absolutely to a bounded function on R, while for p > 1 the convergence holds only in the Besov spaceBp(R) (one need to extract con- stant terms from every summand to get the convergent series, see discussion in [8]). In order to prove an analogous result for Toeplitz operators on the Paley–Wiener space, let us consider the sets

Uηa,ε± =

λ∈ Uε±:|Imλ|> ε ηa

, Ληa,ε=Uηa,ε ∪Zηa∪ Uηa,ε+ . HereZηa ={ηak, k ∈Z}. Next, for a >0 andλ∈C, denote byρa,λ the reproducing kernel of the space PWa at the pointλ. Recall that

ρa,λ:z7→ 1 π

sina(z−¯λ)

zλ¯ , z∈C.

(7)

We are going to prove the following proposition.

Proposition 3.1. — Leta >0and letϕL(R). There existε >0, η >1 such that Tϕ ∈ Sp(PWa) if and only if ϕst = P

λ∈Ληa,εcλ ρ2a,λ a,λk2, where P

λ|cλ|p is finite and the infimum of P

|cλ|p over all possible rep- resentations of ϕst in this form is comparable to kTϕkpSp with constants depending only onp∈(0,1].

We will show how to reduce Proposition 3.1 to the above theorem for Hankel operators using a splitting of the standard symbol into three pieces:

analytic, anti-analytic and a piece with “small” Fourier support.

The following two results for 0 < p 61 are consequences of Lemma 1 and Lemma 2 from [5]. The range 16p <∞has been treated earlier in [9], see also Section 2 in [10].

Lemma 3.2. — Let a > 0 and let ϕL(R). There exist bounded functionsϕ`, ϕc, and ϕr such thatTϕ=Tϕ`+Tϕc+Tϕr onPWa,

suppFϕ`⊂[−4a,−a

2], suppFϕc⊂[−a, a], suppFϕr⊂[a 2,4a], and we havekTϕskSp6cpkTϕkSp for every s=`, c, r forTϕ∈ Sp(PWa).

Herecp is a constant depending only onp.

Lemma 3.3. — Let a > 0 and let ϕL(R) be such thatsupp ˆϕ ⊂ [−a, a]. Then Tϕ ∈ Sp(PWa) if and only if ϕLp(R), in which case kϕkLp(R)is comparable tokTϕkSp with constants depending only onp.

Proof of Proposition 3.1. — Let ϕL(R) and let ϕst = F−1χ(−2a,2a)Fϕbe the standard symbol of the operatorTϕon PWa. Then Tϕ=Tϕst, see Section 2.D in [9]. Suppose thatϕst=P

λ∈Ληa,εcλ ρ2a,λ a,λk2 for someε >0,η >0, and some coefficientscλ such thatP

λ∈Ληa,ε|cλ|p<∞.

It follows from the estimate

2a,λ(z)|

a,λk2 6ce2a|Imz|, z∈C, λ∈C,

that this series converges absolutely to an entire function of exponential type at most 2a bounded on the real line R. By triangle inequality (see, e.g., Theorem A1.1 in [6]), we have

kTϕkpSp=kTϕstkpSp6 X

λ∈Ληa,ε

|cλ|p sup

λ∈C

kTϕλkpSp, where we denotedϕλ=ρ2a,λ

a,λk2. Takeλ∈C. For everyf, g∈PWawe have (Tρ2a,λf, g) = (f¯g, ρ2a,¯λ) =fλ)·g(λ) = (f, ρa,¯λ)(ρa,λ, g).

(8)

It follows that the operatorTϕλ has rank one andkTϕλkSp= 1. HenceTϕ belongs toSp(PWa) andkTϕkpSp 6P

λ|cλ|p.

Now let ϕ be a bounded function on R such that Tϕ ∈ Sp(PWa). We want to show that the standard symbolϕst=F−1χ(−2a,2a)Fϕof Tϕ can be represented in the form

ϕst= X

λ∈Ληa,ε

cλ ρ2a,λa,λk2

for some positive numbersε, η depending only onpand a sequence{cλ} such thatP

λ|cλ|p is comparable tokTϕkpSp. By Lemma 3.2, it suffices to consider separately the following three cases:

(1) supp ˆϕ⊂(−∞,0];

(2) supp ˆϕ⊂[−a, a];

(3) supp ˆϕ⊂[0,+∞).

Let us treat the third case first. Denote by Me−iax the operator of multi- plication by e−iax onL2(R). Since supp ˆϕ⊂[0,+∞), we have

He−2iaxϕ=Me−iaxTϕPaMe−iax,

where He−2iaxϕ : H2H2 is the Hankel operator with symbol ψ = e−2iaxϕ. In particular, we havekHψkSp6kTϕkSp. By Rochberg’s Theorem above, the anti-analytic functionψst =F−1χ(−∞,0)Fe−2iaxϕadmits the following representation:

ψst= X

λ∈Uε+

cλ

kλ kkλk2, whereP

λ∈Uε+|cλ|p is comparable to kHψkpSp, andε > 0 does not depend onψ. This gives us decomposition forϕst:

ϕst= e2iaxψst= X

λ∈Uε+

cλe2iaxkλ kkλk2 = X

λ∈Uε+

cλP2a(e2iaxkλ) kkλk2 ,

whereP2a denotes the orthogonal projection inL2(R) to PW2a. It is easy to see that P2a(e2iaxkλ) = e2iaλ¯ρ2a,λ¯ and kρa,¯λk2 6 2 e2aImλ·kkλk2L2(R), hence

ϕst= X

λ∈Uε

cλ¯βλ ρ2a,λa,λk2

for some complex numbersβλ such that supλλ| 62. Next, in the case where suppϕ⊂ (−∞,0] we can consider the adjoint operator Tϕ =Tϕst

(9)

with the standard symbol ϕst : z 7→ ϕstz) and conclude that in this situation

ϕst= X

λ∈Uε+

cλβλ¯

ρ2a,λ

a,λk2.

Now let suppϕ ⊂ [−a, a]. By Lemma 3.3, we have ϕLp(R). In par- ticular,ϕ∈ PW2a and Plancherel–Polya theorem [7] yields the following decomposition:

ϕ=ϕst= π 2a

X

λ∈Z2a

f(λ)ρ2a,λ, X

λ∈Z2a

|f(λ)|p6cpapkϕkpLp(R), where the constantcp depends only on p. Put Λε =Uε+∪Z2a∪ Uε. To summarize, we have proved that for every bounded functionϕon Rsuch thatTϕ∈ Sp(PWa) there are coefficientscλ,λ∈Λε, such that

(3.1) ϕst = X

λ∈Λε

cλ ρ2a,λ

a,λk2, X

λ∈Λε

|cλ|p6cpkTϕkpSp.

It remains to show that the set Λεand coefficientscλin this decomposition could be replaced by the set Ληa,ε and some new coefficientscλ satisfying the second estimate in (3.1). To this end, for every pointλ ∈ Λε denote byζλ the nearest point toλin Ληa,ε ⊂Λε, whereη = 2k andk ∈Z is a positive integer number that will be specified later. Consider the function

˜

ϕ(1)= X

λ∈Λε

cλ ρ2a,ζλ

a,ζλk2 = X

λ∈Ληa,ε

˜

c(1)λ ρ2a,λ

a,λk2, c˜(1)λ = X

ν∈Λε, ζν

cν.

Note that ˜ϕ(1) has the required representation and P

c(1)λ |p 6 P

|cλ|p. Moreover, we have kTϕTϕ˜(1)kpSp 6 P

λ∈Λεηa,ε|cλ|p· kTϕλTϕζλkpSp. On the other hand, the quasi-norm inSp of the rank two operator

TϕλTϕζλ = ρa,λ

a,λk⊗ ρa,λ

a,λ¯k − ρa,ζλ

a,ζλk ⊗ ρa,ζλ

a,ζλk

does not exceed 21p

ρa,ζλ

a,ζλk− ρa,λa,λk

L2(R)

621p+12

1− Reρa,ζλ(λ) kρa,ζλk · kρa,λk

12 .

Since|ζλ−λ|6ηa for allλby construction, one can choose a large number η= 2k so thatkTϕTϕ˜kpSp 6 12kTϕkpSp. Clearly, this choice ofη does not depend onϕanda. Iterating the process, we see that there are functions

˜

ϕ(n)= X

λ∈Ληa,ε

˜

c(n)λ ρ2a,λ

a,λk2, n= 1,2, . . .

(10)

such thatkTϕ−Tϕ˜(1)−· · ·−Tϕ˜(n)kpSp621nkTϕkpSp,P

n,λc(n)λ |p6cppkTϕkpSp. SinceSp(PWa) is a complete quasi-normed space and a Toeplitz operator on PWa is zero if and only if its standard symbol is zero (see Section 2.D in [9]), this gives us the required decomposition of ϕst with coefficients cλ=P

n>1c˜(n)λ , λ∈Ληa,ε.

4. Interpolation of discrete Besov sequences

Denote by PW[0,a] the Paley–Wiener space of functions inL2(R) with Fourier spectrum in the interval [0, a]. Recall that the reproducing kernel ka,λ of the space PW[0,a] at a pointλ∈C+has the form

ka,λ(z) =− 1 2πi

1−eia(z−¯λ)

zλ¯ , z∈C.

Denote byC0(Za) the set of functions onZa tending to zero at infinity. Our aim in this section is to prove the following proposition.

Proposition 4.1. — Let 0 < p 6 1, let Λ be the set Ληa,ε from Proposition 3.1, and letF =P

λ∈Λcλkkkaa,λ

2k2 for some cλ ∈ C such that P

λ∈Λ|cλ|p <∞. Then the restriction ofF to Za belongs toBp(a,osc)∩ C0(Za). Conversely, for every functionf ∈Bp(a,osc)there exists the unique functionF as above and a polynomial q of degree at most[p1] such that f = q+F on Za. Moreover, the infinum of P

λ∈Λ|cλ|p over all possi- ble representations ofF =P

λ∈Λcλ ka,λ

kka

2k2 in this form is comparable to kfkp

Bp(osc,a) with constants depending only onp.

The proof of Proposition 4.1 is based on the following lemma.

Lemma 4.2. — We have kka,λkBp(a,osc) 6 cpkka

2k2 for every a > 0, 0< p61, andλ∈C, where the constantcp depends only onp.

Proof. — At first, consider the pointsλin the support ofµa. Forλ∈Za

we have

ka,λ(x) =

(kka,λk2, x=λ;

0, x∈suppµa\ {λ}.

(11)

TakingPI = 0 for intervalsI∈ Ia in the definition of osc ka,λ, I, µa,1

p

, we obtain the estimate

kka,λkp

Bp(a,osc)6 X

I∈Ia

1 µa(I)

Z

I

|ka,λ(x)|dµa(x) p

=kka,λk2pµa({λ})p X

I∈Ia

χI(λ) µa(I)p 6cpkka

2k2p.

Now letλbe an arbitrary point inC\suppµa. Thenka,λ(x) =−2πi1 1−ex−−iaλ¯λ¯ for allx∈suppµa. Thus, we need to estimate an oscillation of the function x7→ x−1λ¯ on the lattice Za. Divide collection Ia from Section 1 into two parts:

Ia,1={I∈ Ia: I=Ia,j,k, Reλ /Ia,j,k−1Ia,j,kIa,j,k+1}, Ia,2=Ia\ Ia,1.

For an intervalI∈ Ia,1with center xc, define the polynomialPI of degree [1p] by

(4.1) 1

xλ¯ −PI(x) = (x−xc)[p1]+1 (x−λ)(¯¯ λxc)[1p]+1

.

Using this polynomial, we can estimate (4.2)

osc 1

xλ¯, I, µa, 1

p

6sup

x∈I

(x−xc)[1p]+1 (x−λ)(¯¯ λxc)[1p]+1

6 |I|[1p]+1 dist(λ, I)[1p]+2

,

where|I|denotes the length ofI. SinceI∈ Ia,1, we have dist(λ, I)>|I|, hence

(4.3) X

I∈Ia,1

osc 1

¯λx, I, µa, 1

p p

6 X

I∈Ia,1

1

|I|p 6cp·ap.

We also will need a more accurate estimate for the left hand side of the inequality above in the case where|Imλ|is large. For everyj>0, letIa,1j

(12)

be the set of intervalsIa,j,k,k∈Z, belonging to the familyIa,1. We have X

I∈Ija,1

|I|[1p]+1 dist(λ, I)[1p]+2

!p

= X

I∈Ia,1j

|I|[1p]+1

|Imλ|2+ dist(Reλ, I)2([1p]+2)/2

p

6cpa 2j

pX

m>1

1 a

2j 2

|Imλ|2+m2

1 2[p1]p+p

6cpa 2j

p γ1−[

1 p]p−2p

j ,

whereγj = max 1,2aj|Imλ|

. Indeed, the last inequality follows from ele- mentary estimates

X

m=1

m−1−2p<∞,

Z 1

dx

(r2+x2)s 6csr1−2s, wherer >0, and the constantcsdepends ons >1/2. Put

Nλ=

(log2(a|Imλ|)

, ifa|Imλ|>2, 0, ifa|Imλ|<2.

Note that ˜p=−1 + [1p]p+pis a positive number. It follows X

I∈Ia,1

osc 1

λ¯−x, I, µa, 1

p p

6cp

X

j=0

a 2j

p γ1−[

1 p]p−2p j

6cpap˜|Imλ|p−p˜

Nλ

X

j=0

2pj˜ +cp

X

j=Nλ

ap 2pj 6 cp

|Imλ|p. Combining the last estimate with (4.3), we get

X

I∈Ia,1

osc 1

¯λx, I, µa, 1

p p

6cpmin

ap, 1

|Imλ|p

.

Now consider the familyIa,2=Ia,21∪ Ia,22,

Ia,21={I∈ Ia,2:|I|6|Imλ|}, Ia,22={I∈ Ia,2:|I|>|Imλ|}.

For an intervalI∈ Ia,21 we use the polynomialPI defined by (4.1). Then formula (4.2) implies

X

I∈Ia,21

osc 1

λ¯−x, I, µa, 1

p p

6 X

I∈Ia,21

|I|[p1]+1

|Imλ|[p1]+2

!p

6 cp

|Imλ|p.

(13)

Note that if|Imλ| < a , the set Ia,21 is empty. This shows that we can write

X

I∈Ia,21

osc 1

λ¯−x, I, µa, 1

p p

6cpmin

ap, 1

|Imλ|p

.

ForI∈ Ia,22we putPI = 0. Denote byx0the nearest point toλin suppµa, and setI0=I\ {x∈R:|x−Reλ|< π/a}. We have

1 µa(I)

Z

I

1 x−¯λ

a(x)6 µa({x0})

µa(I)|x0−¯λ| + 1 µa(I)

Z

I0

dx

|x−¯λ|

6 c

a|I||x0λ|¯ + c

|I|

Z |I|

πa−1

dx px2+|Imλ|2

6 c

a|I||x0λ|¯ + c

|I|min

loga|I|

π ,log+ |I|

|Imλ|

.

Using estimatesP

I∈Ia,2

1

|I|p 6cpap, P

I∈Ia,2

log

a|I|

|I|

p

6cpap, and X

I∈Ia,22

1

|I|log |I|

|Imλ|

p

6 cp

|Imλ|p, we see that

X

I∈Ia,22

osc cp

λ¯−x, I, µa, 1

p p

6 cp

|x0−¯λ|p +cpmin

ap, 1

|Imλ|p

.

Eventually, we obtain

1 xλ¯

p

Bp(a,osc)

6 cp

|x0λ|¯p +cpmin

ap, 1

|Imλ|p

.

It follows that kka,λkp

Bp(a,osc)6cp(1 + e−aImλ)pmin

ap, 1

|Imλ|p

+cp

1−e−iaλ¯ x0λ

p

6cpkka

2k2p,

which is the desired estimate.

LetC0(R) denote the set of all continuous functions onRtending to zero at infinity. For completeness, we include the proof of the following known lemma.

Lemma 4.3. — Let0< p61,a >0. For every functionf ∈Bp(osc, a) there exists a functionF ∈Bp(R)such thatF =f onZa, and

kFkBp(R)6cpkfkBp(osc,a),

(14)

where the constantcp depends onlyp.

Proof. — Fork∈ZputIk= [a [1p]k,a [1p](k+ 1)]. Interiors of intervals Ik are disjoint and every set Ik∩Za contains [1p] + 1 points. On everyIk define the polynomial Pk of degree at most [1p] such that Pk(x) = f(x) for all xIk ∩Za. Next, set F(x) = Pk(x) for xIk. We claim that the function F is in Bp(R). To check this, let us take an interval Jj,k = [a [1p]k·2j,a[1p](k+1)·2j] withk, j∈Z. In the case wherej <0 we clearly have osc(F, Jj,k, m,[1p]) = 0 because the function F is a polynomial of degree at most [p1] onI. Hence, we can assume thatJ =Jj,k=I`∪. . .∪I`+N

for some`∈Zand N >1. Consider the polynomialPJ of degree at most [1p] such that

osc

f, J, µa, 1

p

= 1

µa(J) Z

J

|f(x)−PJ(x)|dµa(x).

We have 1

|J| Z

J

|F(x)−PJ(x)|dx= 1

|J|

N

X

s=0

Z

I`+s

|P`+s(x)−PJ(x)|dx

6 cp

|J|

N

X

s=0

Z

I`+s

|P`+s(x)−PJ(x)|dµa(x)6cposc

f, I, µa, 1

p

,

where we used the fact that Z

I`

|P(x)|dx6cp

Z

I`

|P(x)|dµa(x)

for every intervalI`,`∈Z, and every polynomialP of degree at most [p1].

It follows that kFkp

Bp(R,m,osc)6cppX

j,k

osc

f, Jj,k, µa, 1

p p

6cppkfkp

Bp(osc,a),

and henceF belongs to the spaceB1/pp,p(R, dx,osc) =Bp(R), as required.

Proof of Proposition 4.1. — Consider a functionF of the form F =X

λ∈Λ

cλ

ka,λ

kka

2k2, X

λ∈Λ

|cλ|p<∞.

Since 0< p61 and|ka,λ(x)|6ckka

2k2 for everyλ∈Candx∈R, the series above converges absolutely to a function fromC0(R) by the Lebesgue dominated convergence theorem. By Lemma 4.2, the restriction ofF toZa

(to be denoted byf) is inBp(a,osc) andkfkp

Bp(a,osc)6cpP

λ∈Λ|cλ|p for a constantcp depending only on p.

Références

Documents relatifs

have proved that an integrable p-almost tangent (cotangent) manifold satisfying some global hypotheses is an afhne bundle modelled in a tangent.. (cotangent) bundle

Treves conjectured a general criterion for analytic hypoellipticity [31]: “For a sum of squares of analytic vector fields to be analytic hypoelliptic it is necessary and sufficient

TREVES, On local solvability of linear partial differential equations, I-Necessary conditions. POPIVANOV, On the local solvability of a class of partial

the classical Cauchy-filter approach does not yield the absolute closedness property in locales, it was replaced by another construction the idea of which was to

In Section 4 we show Theorems A and B: the Bergman kernel on a compact quantizable real-analytic Kähler manifold, and the composition of analytic covariant Toeplitz operators, are

— We have seen in the previous section that the subshift associated to an irreducible Pisot substitution has pure discrete spectrum as soon as the interior of a piece of the

Nous savons que à l’optimum le TMST est égal au rapport des prix. 3) Quelle est la fonction de coût total, la fonction de coût marginal et la fonction de coût moyen de cette

Avant de commencer cette fiche de révisions, il faut d’abord connaître parfaitement son cours (vocabulaire et propriétés). Exercice n°1 : Compléter par les formules