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A result of Strichartz on a generalization of Wiener’s characterization of continuous

measures revisited

B´ erenger Akon KPATA

Laboratoire de Math´ ematiques et Informatique, UFR des Sciences Fondamentales et Appliqu´ ees, Universit´ e Nangui Abrogoua,

02 BP 801 Abidjan 02, Cˆ ote d’Ivoire kpata akon@yahoo.fr

Received: 19.8.2014; accepted: 18.5.2015.

Abstract. We give the reasons for which the continuous part of a measure that belongs to the Wiener amalgam space M

2

does not contribute to the Bohr mean of its Fourier transform.

Keywords: Fourier transform, Radon measure, Wiener amalgam space MSC 2010 classification: primary 42B10, secondary 42B35

1 Introduction

In this paper, for 1 < p < ∞, we denote by p 0 the real number satisfying

1

p + p 1

0

= 1. A Radon measure µ on R d belongs to the Wiener amalgam space M p , (1 ≤ p < ∞) if 1 kµk p < ∞ with

r kµk p =

 X

k∈Z

d

|µ|(I k r ) p

1 p

, r > 0

where I k r = Q d

i=1 [k i r, (k i + 1)r) for k = (k 1 , . . . , k d ) ∈ Z d and |µ| denotes the total variation of µ.

The Fourier transform on amalgam spaces has been studied by various authors including F. Holland ([8], [9]), J. Stewart [11], J. P. Bertrandias and C. Dupuis [2], J. J. F. Fournier ([6], [7]) and I. Fofana [5].

In [8], the Fourier transform f 7→ b f defined on the usual Lebesgue space L 1 by

f (x) = (2π) b

d2

Z

R

d

f (y) e −ixy dy, x ∈ R d

http://siba-ese.unisalento.it/ c 2015 Universit` a del Salento

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has been extended by F. Holland to the spaces (L q , l p ) defined for 1 ≤ q, p ≤ ∞ as follows:

(L q , l p ) = n

f ∈ L 0 | 1 kf k q, p < ∞ o

where L 0 stands for the space of (equivalence classes modulo the equality Lebesgue almost everywhere of) all complex-valued functions defined on R d and for r > 0,

r kf k q, p =

 

 

 

 

 X

k∈Z

d

 f χ I

kr

q

 p

1 p

if 1 ≤ p < ∞, sup

x∈R

d

f χ J

xr

q if p = ∞,

where J x r = Q d

i (x i − r 2 , x i + r 2 ) for x = (x 1 , . . . , x d ) ∈ R d , χ I

rk

denotes the characteristic function of I k r and k · k q is the usual Lebesgue norm. In the same paper, he extended to the spaces M p (1 < p ≤ 2) the Fourier transform µ 7→ µ b defined on the space M 1 of finite Radon measures on R d by

µ(x) = (2π) b

d2

Z

R

d

e −ixy dµ(y), x ∈ R d .

In fact, he proved that if µ belongs to M p (1 < p ≤ 2), then there exists a unique element µ ∈ (L b p

0

, l ) such that for any sequence (r n ) n≥1 of positive real numbers increasing to ∞, the sequence ( \ µbJ 0 r

n

) n≥1 converges in (L p

0

, l ) to b µ, where µbJ 0 r

n

is the measure defined by (µbJ 0 r

n

) (N ) = µ (J 0 r

n

∩ N ) for any Borel subset N of R d . In addition,

Z

R

d

g (x) µ (x) dx = b Z

R

d

b g(x) dµ (x) , g ∈ L p , l 1  . In [5], I. Fofana has proved the following Hausdorff-Young inequality :

r

p0d

r k µk b p

0

, ∞ ≤ C

1

r

kµk p , r > 0 (1.1) where the real constant C does not depend on µ and r.

The relation between the properties of a Radon measure and the asymptotic behavior of its Fourier transform is an important topic in Harmonic Analysis.

A well-known theorem of Wiener [14] states that if µ ∈ M 1 , then

r→∞ lim r −d Z

J

0r

| µ(y)| b 2 dy = X

a∈D

|µ ({a})| 2 , (1.2)

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where D = { a ∈ R d | µ({a}) 6= 0 } is a countable set.

The left-hand side of (1.2) is the so-called Bohr mean of µ. Wiener’s result b has found many applications in various areas of mathematics, including ergodic theory and optimal control theory. Since then, Wiener-type characterizations of continuous measures are extensively investigated (see for example [1], [3], [4], [12] and [13, Section 12.5]). Strichartz has established that equality (1.2) continues to hold if the measure µ belongs to M 2 (see Theorem 4.4 in [12]).

The aim of this note is to give, by a new proof, the reasons for which the continuous part of a measure belonging to M 2 does not contribute to formula (1.2). To this end , we prove in Section 2 the following result: if µ is a continuous measure that belongs to M p , then

r→0 lim r kµk p = 0.

In Section 3, we show that if µ is a discrete measure that belongs to M p , then

r→0 lim r kµk p = X

a∈D

|µ ({a})| p

!

1

p

.

Since any Radon measure on R d has a decomposition into discrete and continu- ous parts, we combine these above results with inequality (1.1) to establish, in Section 4, the generalization of Wiener’s theorem obtained by Strichartz.

2 M p -estimate of a continuous measure

Let us recall the definition of a continuous Radon measure.

Definition 1. A Radon measure µ on R d is continuous if for any x ∈ R d we have µ({x}) = 0.

Notice that for any Radon measure µ on R d and any x ∈ R d , we have

|µ({x})| = |µ|({x}). Therefore, a Radon measure on R d is continuous if and only if its total variation is continuous.

The following proposition will be useful in the proof of the main result of this section.

Proposition 1. [10]. Let 1 ≤ p < ∞. If µ ∈ M p and 0 < r < s < ∞, then (i) s kµk p ≤ Int r s  + 2

p0d

2

dp

r kµk p , where Int s r 

denotes the greatest integer not exceeding r s ;

(ii) r kµk p ≤ 3

p0d

2

dp

s kµk p .

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We can now prove the following result.

Proposition 2. Suppose that 1 ≤ p < ∞ and µ is a continuous measure that belongs to M p . Then we have

(i) lim r→0 sup k∈Z

d

|µ|(I k r ) = 0, (ii) p > 1 =⇒ lim r→0 r kµk p = 0.

Proof. For each non-negative integer n, set s n = sup

k∈Z

d

|µ|(I k 2

−n

).

(i) Notice that (s n ) n is a decreasing sequence of positive real numbers. Suppose that lim n→∞ s n = s > 0. For each non-negative integer n, let

K n = n

k ∈ Z d | |µ|(I k 2

−n

) > s 2

o . Let us notice that for each positive integer n,

0 < card K n ≤  2

s 2

−n

kµk p

 p

≤  2

s 1 kµk p

 p

< ∞ and

k ∈ K n+1 =⇒ ∃ l ∈ K n : I k 2

−(n+1)

⊂ I l 2

−n

,

where card K n denotes the cardinality of K n . So there exists a sequence (k n ) n of elements of Z d such that for each non-negative integer n we have

k n ∈ K n and I k 2

n+1−(n+1)

⊂ I k 2

n−n

. It follows that ∩ n I k 2

−n

n

is a one point set and |µ|(∩ n I k 2

−n

n

) > 0. This is in contra- diction with the fact that µ is a continuous measure. So

n→∞ lim s n = 0.

Now let us consider a real number ε > 0. There exists an integer n 0 such that s n

0

< 2 ε

d

. Let us notice that for each element (r, k) of (0, 2 −n

0

) × Z d , the set I k r intersects at most 2 d elements of { I l 2

−n0

| l ∈ Z d }. So

|µ|(I k r ) ≤ 2 d s n

0

, (r, k) ∈ (0, 2 −n

0

) × Z d . It follows that

sup

k∈Z

d

|µ|(I k r ) < ε, r ∈ (0, 2 −n

0

).

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Therefore,

r→0 lim sup

k∈Z

d

|µ|(I k r ) = 0.

(ii) Suppose p > 1. Let us consider a real number t > 0. There exists a finite subset L of Z d such that

X

k∈Z

d

\L

|µ|(I k 1 ) p < t.

Let us set

E = [

k∈L

I k 1

and for each non-negative integer n, L n = n

k ∈ Z d | I k 2

−n

⊂ E o

, α n = X

k∈L

n

|µ|(I k 2

−n

) p and t n = X

k∈Z

d

\L

n

|µ|(I k 2

−n

) p .

Then, for each non-negative integer n,

2

−n

kµk p = (α n + t n )

1p

, α n ≤ s p−1 n |µ|(E) and t n ≤ t.

Let us notice that

|µ|(E) ≤ card L 1 kµk p < ∞

(where card L denotes the cardinality of L) and ( 2

−n

kµk p ) n is a decreasing sequence. It follows that

n→∞ lim 2

−n

kµk p ≤ t

p1

.

Since the above inequality holds for an arbitrary real number t > 0, we deduce that

n→∞ lim 2

−n

kµk p = 0.

Further, for each non-negative integer n, it follows from Proposition 1 (ii) that

0 ≤ r kµk p ≤ 3

p0d

2

dp

2

−n

kµk p , r ∈ (0, 2 −n ).

So

r→0 lim r kµk p = 0.

QED

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3 M p -estimate of a discrete measure

This section is devoted to the proof of the following result.

Proposition 3. Suppose that 1 ≤ p < ∞ and µ is a discrete measure that belongs to M p . Then

r→0 lim r kµk p = X

a∈D

|µ({a})| p

!

1p

,

where D = { a ∈ R d | µ({a}) 6= 0 }.

Proof. Let us consider a real number ε > 0. There exists a finite subset K of Z d such that

 X

k∈Z

d

\K

|µ| I k 1  p

1 p

< ε 2

dp

.

Set

E = [

k∈K

I k 1 , D n =



a ∈ D | |µ({a})| ≥ 1 n



and µ n (B) = µ(B ∩ D n )

for any positive integer n and any Borel subset B of R d . Then, for each positive integer n and each element r of (0, 1), we have

r kµk p

 X

k∈Z

d

|µ| (I k r ∩ E) p

1 p

+

 X

k∈Z

d

|µ| (I k r \ E) p

1 p

 X

k∈Z

d

|µ| (I k r ∩ E) p

1 p

+

2 d X

k∈Z

d

\K

|µ| I k 1  p

1 p

 X

k∈Z

d

|µ| (I k r ∩ E) p

1 p

+ ε

 X

k∈Z

d

n | (I k r ∩ E) p

1 p

+ |µ| (E ∩ (D \ D n )) + ε

 X

k∈Z

d

n | (I k r ) p

1 p

+ |µ| (E ∩ (D \ D n )) + ε.

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Since for each positive integer n the set D n is finite, then there exists an element r n of (0, 1) such that for all a, b ∈ D n ,

a 6= b =⇒ ∃ i ∈ { 1, . . . , d } : |a i − b i | > r n and for each element r of (0, r n )

 X

k∈Z

d

n | (I k r ) p

1 p

= X

a∈D

n

|µ({a})| p

!

p1

≤ X

a∈D

|µ({a})| p

!

1p

.

Therefore, for each element r of (0, r n ) we have

r kµk p ≤ X

a∈D

|µ({a})| p

!

1p

+ |µ| (E ∩ (D \ D n )) + ε.

Since |µ|(E) < ∞ and (D \ D n ) n is a decreasing sequence that converges to the empty set, we get

lim sup

r→0 r kµk p ≤ X

a∈D

|µ({a})| p

!

1p

+ ε.

As this inequality holds for an arbitrary real number ε > 0, we deduce that

lim sup

r→0 r kµk p ≤ X

a∈D

|µ({a})| p

!

1p

.

Further, for all real numbers r > 0, we have

X

a∈D

|µ({a})| p

!

1p

=

 X

k∈Z

d

 X

a∈D∩I

kr

|µ({a})| p

1 p

r kµk p .

So

r→0 lim r kµk p = X

a∈D

|µ({a})| p

!

1p

.

QED

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4 Generalization of Wiener’s theorem

Throughout this section, for 1 < p < ∞ and µ ∈ M p , we set D = { a ∈ R d | µ({a}) 6= 0 }.

Proposition 4. Let 1 < p < ∞. If µ ∈ M p then

r→0 lim r kµk p = X

a∈D

|µ({a})| p

!

1p

.

Proof. Let us write µ = µ c + µ δ , where µ c is a continuous measure and µ δ is a discrete measure. For each real number r > 0, we have

r kµ δ k pr kµk prc k p + rδ k p .

The desired result follows from Propositions 2 and 3.

QED

As an immediate consequence of (1.1) and Proposition 4, we have the fol- lowing result.

Corollary 1. Let 1 < p ≤ 2. There exists a real constant C > 0 such that for any µ ∈ M p we have

lim sup

r→∞

r

d

p0

r k µk b p

0

, ∞ ≤ C X

a∈D

|µ({a})| p

!

1p

.

In the case p = 2, we obtain the following generalization of Wiener’s theorem.

Proposition 5. If µ ∈ M 2 then

r→∞ lim r

d2

Z

J

0r

| µ(y)| b 2 dy

!

12

= X

a∈D

|µ({a})| 2

!

12

.

Proof. a) Let us write µ = µ c + µ δ , where µ c is a continuous measure and µ δ is a discrete measure. It follows from Propositions 2 and 3 that

r→∞ lim

1r

c k 2 = 0 and lim

r→∞

1r

δ k 2 = X

a∈D

|µ({a})| 2

!

12

< ∞.

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Note that for each element (r, x) of (0, ∞) × R d , we have Z

J

xr

| µ(y)| b 2 dy = Z

J

xr

| c µ δ (y)| 2 dy + 2Re Z

J

xr

c µ δ (y) µ b c (y) dy + Z

J

xr

| µ b c (y)| 2 dy,

where Re Z

J

xr

c µ δ (y) µ b c (y) dy denotes the real part of Z

J

xr

c µ δ (y) µ b c (y) dy.

By the H¨ older’s inequality and (1.1), we have

Z

J

xr

c µ δ (y) µ b c (y) dy

≤ Z

J

xr

| c µ δ (y)| 2 dy

!

12

Z

J

xr

| µ b c (y)| 2 dy

!

12

r k c µ δ k 2, +∞ r k µ b c k 2, +∞

≤ C 2

1

r

k µ δ k 2

1

r

k µ c k 2 r d and

Z

J

xr

| µ b c (y)| 2 dy ≤ r k µ b c k 2 2, +∞ ≤ C 2

1 r

c k 2 2 r d .

It follows that

lim sup

r→∞

r

d2

r k µk b 2, ∞ = lim sup

r→∞

r

d2

r k c µ δ k 2, ∞ and

lim inf

r→∞ r

d2

r k µk b 2, ∞ = lim inf

r→∞ r

d2

r k c µ δ k 2, ∞ .

Therefore, it suffices to consider the case where µ is a discrete measure to prove the desired result.

b) Suppose now that µ is a discrete measure.

Let us consider an element ε of



0, 1 3 P

a∈D |µ({a})| 2 

12

 . For each positive integer n and each Borel subset B of R d , set

D n =



a ∈ D | |µ({a})| ≥ 1 n



and µ n (B) = µ(B ∩ D n ).

There exists a positive integer N such that

 X

a∈D\D

N

|µ({a})| 2

1 2

< ε

3(C + 1) , (4.1)

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where C is a real constant as in Corollary 1. So

lim sup

r→+∞

r

d2

r k µ − b µ c N k 2, ∞ ≤ C

 X

a∈D\D

N

|µ({a})| 2

1 2

< ε 3 .

Thus, there exists a real number R 1 > 0 such that for any r ≥ R 1 and any x ∈ R d ,

r

d2

Z

J

xr

| b µ(y)| 2 dy

!

12

− r

d2

Z

J

xr

| µ c N (y)| 2 dy

!

12

< ε

3 . (4.2)

Since µ N is a finite measure, it follows from (1.2) that

r→∞ lim r

d2

Z

J

0r

| µ c N (y)| 2 dy

!

12

=

 X

a∈D

N

|µ({a})| 2

1 2

.

Thus, there exists a real number R 2 > 0 such that for any r ≥ R 2 ,

r

d2

Z

J

0r

| µ c N (y)| 2 dy

!

12

 X

a∈D

N

|µ({a})| 2

1 2

< ε

3 . (4.3)

Let R = max{ R 1 , R 2 }. From inequalities (4.1), (4.2) and (4.3), we obtain

r

d2

Z

J

0r

| µ(y)| b 2 dy

!

1

2

− X

a∈D

|µ({a})| 2

!

1

2

< ε, r ≥ R.

Hence

r→+∞ lim r

d2

Z

J

0r

| µ(y)| b 2 dy

!

12

= X

a∈D

|µ({a})| 2

!

12

.

QED

As an immediate consequence of Proposition 5 and Definition 1, we have the following criterion.

Corollary 2. Let µ ∈ M 2 . Then µ is continuous if and only if

r→∞ lim r −d Z

J

0r

| µ(y)| b 2 dy = 0.

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Acknowledgements. The author would like to thank Professor I. Fofana for his help and guidance in the preparation of this paper.

References

[1] M. Anoussis and A. Bisbas, Continuous measures on compact Lie groups, Ann. Inst.

Fourier (Grenoble) 50 (2000), no. 4, 1277-1296.

[2] J. P. Bertrandias et C. Dupuis, Transformation de Fourier sur les espaces l

p

(L

p0

), Ann. Inst. Fourier (Grenoble) 29 (1979), no. 1, 189-206.

[3] A. Bisbas and C. Karanikas, On the continuity of measures, Appl. Anal. 48 (1993), 23-35.

[4] M. Bj¨ orklund and A. Fish, Continuous measures on homogenous spaces, Ann. Inst.

Fourier (Grenoble) 59 (2009), no. 6, 2169-2174.

[5] I. Fofana, Transformation de Fourier dans (L

q

, l

p

)

α

et M

p, α

, Afrika Mat. (3) 5 (1995), 53-76.

[6] J. J. F. Fournier, On the Hausdorff-Young theorem for amalgams, Monatsh. Math. 95 (1983), 117-135.

[7] J. J. F. Fournier and J. Stewart, Amalgams of L

p

and l

q

, Bull. Amer. Math. Soc.

13 (1985), 1-21.

[8] F. Holland, Harmonic Analysis on amalgams of L

p

and l

q

, J. London Math. Soc. (2) 10 (1975), 295-305.

[9] F. Holland, On the representation of functions as Fourier transforms of unbounded measures , Proc. London Math. Soc (3) 30 (1975), 347-365.

[10] B. A. Kpata, I. Fofana and K. Koua, On Fourier asymptotics of a generalized Cantor measure, Colloq. Math. 119 (2010), no 1, 109-122.

[11] J. Stewart, Fourier transforms of unbounded measures, Canad. J. Math. 31 (1979), 1281-1292.

[12] R. S. Strichartz, Fourier asymptotics of fractal measures, J. Funct. Anal. 89 (1990), 154-187.

[13] M. E. Taylor, Pseudodifferential Operators, Princeton Univ. Press, Princeton, NJ, 1981.

[14] N. Wiener, The Fourier Integral and Certain of its Applications, Dover, New York, 1933.

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