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Negative Results Concerning Fourier Series

R. Toledo vol. 9, iss. 4, art. 99, 2008

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NEGATIVE RESULTS CONCERNING FOURIER SERIES ON THE COMPLETE PRODUCT OF S

3

R. TOLEDO

Institute of Mathematics and Computer Science College of Nyíregyháza

P.O. Box 166, Nyíregyháza, H-4400 Hungary

EMail:toledo@nyf.hu

Received: 26 November, 2007

Accepted: 13 October, 2008

Communicated by: S.S. Dragomir 2000 AMS Sub. Class.: 42C10.

Key words: Fourier series, Walsh-system, Vilenkin systems, Representative product systems.

Abstract: The aim of this paper is to continue the studies about convergence inLp-norm of the Fourier series based on representative product systems on the complete prod- uct of finite groups. We restrict our attention to bounded groups with unbounded sequenceΨ. The most simple example of this groups is the complete product of S3. In this case we proved the existence of an1< p <2number for which ex- ists anfLpsuch that its n-th partial sum of Fourier seriesSndo not converge to the functionfinLp-norm. In this paper we extend this ”negative” result for all1< p <andp6= 2numbers.

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Negative Results Concerning Fourier Series

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Contents

1 Representative Product Systems 4

2 The Sequence of FunctionsΨk(p) 7

3 Negative Results 13

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Introduction

In Section1we introduce basic concepts in the study of representative product sys- tems and Fourier analysis. We also introduce the system with which we work on the complete product ofS3, i.e. the symmetric group on 3 elements (see [2]). Section2 extends the definition of the sequenceΨfor allp≥1. Finally, we use the results of Section2to study the convergence in theLp-norm (p ≥ 1) of the Fourier series on bounded groups with unbounded sequenceΨ, supposing all the same finite groups appearing in the product of Ghave the same system ϕ at all of their occurrences.

These results appear in Section3and they complete the statement proved by G. Gát and the author of this paper in [2] for the complete product ofS3. There have been similar results proved with respect to Walsh-like systems in [4] and [5].

Throughout this work denote byN,P,Cthe set of nonnegative, positive integers and complex numbers, respectively. The notation which we have used in this paper is similar to [3].

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1. Representative Product Systems

Letm := (mk, k ∈ N) be a sequence of positive integers such that mk ≥ 2 and Gk a finite group with order mk, (k ∈ N). Suppose that each group has discrete topology and normalized Haar measureµk. LetGbe the compact group formed by the complete direct product ofGkwith the product of the topologies, operations and measures (µ). Thus each x ∈ G consists of sequences x := (x0, x1, . . .), where xk ∈ Gk, (k ∈ N). We call this sequence the expansion ofx. The compact totally disconnected groupGis called a bounded group if the sequencemis bounded.

If M0 := 1and Mk+1 := mkMk, k ∈ N, then every n ∈ N can be uniquely expressed asn=P

k=0nkMk,0≤nk < mk,nk ∈N. This allows us to say that the sequence(n0, n1, . . .)is the expansion ofnwith respect tom.

Denote byΣkthe dual object of the finite groupGk(k ∈N). Thus eachσ ∈Σkis a set of continuous irreducible unitary representations ofGkwhich are equivalent to some fixed representationU(σ). Letdσ be the dimension of its representation space and let{ζ1, ζ2, . . . , ζdσ}be a fixed but arbitrary orthonormal basis in the representa- tion space. The functions

u(σ)i,j(x) :=hUx(σ)ζi, ζji (i, j ∈ {1, . . . , dσ}, x∈Gk)

are called the coordinate functions forU(σ) and the basis {ζ1, ζ2, . . . , ζdσ}. In this manner for eachσ ∈ Σk we obtaind2σ number of coordinate functions, in totalmk number of functions for the whole dual object ofGk. TheL2-norm of these functions is1/√

dσ.

Let{ϕsk : 0 ≤ s < mk}be the set of all normalized coordinate functions of the group Gk and suppose that ϕ0k ≡ 1. Thus for every 0 ≤ s < mk there exists a σ∈Σk,i, j ∈ {1, . . . , dσ}such that

ϕsk(x) = p

dσu(σ)i,j (x) (x∈Gk).

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Letψ be the product system ofϕsk, namely ψn(x) :=

Y

k=0

ϕnkk(xk) (x∈G),

wherenis of the formn =P

k=0nkMkandx= (x0, x1, . . .). Thus we say thatψ is the representative product system ofϕ. The Weyl-Peter’s theorem (see [3]) ensures that the systemψis orthonormal and complete onL2(G).

The functionsψn(n∈N)are not necessarily uniformly bounded, so define Ψk:= max

n<Mk

nk1nk (k ∈N).

It seems that the boundedness of the sequenceΨplays an important role in the norm convergence of Fourier series.

For an integrable complex functionf defined inGwe define the Fourier coeffi- cients and partial sums by

fbk:=

Z

Gm

f ψkdµ (k ∈N), Snf :=

n−1

X

k=0

fbkψk (n ∈P).

According to the theorem of Banach-Steinhauss,Snf → f asn → ∞in theLp norm forf ∈Lp(G)if and only if there exists aCp >0such that

kSnfkp ≤Cpkfkp (f ∈Lp(G)).

Thus, we say that the operator Sn is of type (p, p). Since the system ψ forms an orthonormal base in the Hilbert spaceL2(G), it is obvious thatSnis of type(2,2).

The representative product systems are the generalization of the well known Walsh-Paley and Vilenkin systems. Indeed, we obtain the Walsh-Paley system if

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Negative Results Concerning Fourier Series

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mk = 2 and Gk := Z2, the cyclic group of order 2 for allk ∈ N. Moreover, we obtain the Vilenkin systems if the sequencem is an arbitrary sequence of integers greater than 1 andGk :=Zmk, the cyclic group of ordermkfor allk ∈N.

Letmk = 6for allk ∈NandS3be the symmetric group on 3 elements. LetGk :=

S3 for allk ∈ N. S3 has two characters and a 2-dimensional representation. Using a calculation of the matrices corresponding to the 2-dimensional representation we construct the functionsϕsk. In the notation the indexk is omitted because all of the groupsGkare the same.

e (12) (13) (23) (123) (132) kϕsk1sk

ϕ0 1 1 1 1 1 1 1 1

ϕ1 1 −1 −1 −1 1 1 1 1

ϕ2

2 −√ 2

2 2

2

2

2

2

2 2

2 2 3

√2 ϕ3

2 √

2 −

2

2

2

2

2

2

2 2

2 2 3

√2

ϕ4 0 0 −

6 2

6 2

6

2

6 2

6 3

6 2

ϕ5 0 0 −

6 2

6

2

6 2

6 2

6 3

6 2

Notice that the functions ϕsk can take the value 0, and the product system of ϕ is not uniformly bounded. These facts encumber the study of these systems. On the other hand, max

0≤s<6sk1sk = 43, thus Ψk = 43k

→ ∞if k → ∞. More examples of representative product systems have appeared in [2] and [7].

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2. The Sequence of Functions Ψ

k

(p)

We extend the definition of the sequenceΨfor allp≥1as follows:

Ψk(p) := max

n<Mk

nkpnkq

p≥1, 1 p +1

q = 1, k ∈N

(ifp= 1thenq=∞). Notice thatΨk = Ψk(1)for allk ∈N. Clearly, the functions Ψk(p)can be written in the form

Ψk(p) =

k−1

Y

i=0

maxs<mi

sikpsikq

=:

k−1

Y

i=0

Υi(p)

p≥1, 1 p +1

q = 1, k ∈N

.

Therefore, we study the productkfkpkfkqfor normalized functions on finite groups.

In this regard we use the Hölder inequality (see [3, p. 137]). First, we prove the following lemma.

Lemma 2.1. Let Gbe a finite group with discrete topology and normalized Haar measure µ, and let f be a normalized complex valued function on G (kfk2 = 1).

Thus,

1. ifkfk1kfk= 1, thenkfkpkfkq = 1for allp≥1and 1p +1q = 1.

2. ifkfk1kfk>1, thenkfkpkfkq >1for allp≥1,p6= 2and 1p + 1q = 1.

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Proof.

1. The conditions imply the equality Z

G

|f|dµ· kfk= 1 = Z

G

|f|2 dµ.

Letf0 := kfkf

. Then

(2.1) |f0(x)| ≤1 (x∈G)

and (2.2)

Z

G

|f0|dµ= Z

G

|f0|2 dµ.

Thus by (2.1) we obtain|f0(x)| − |f0(x)|2 ≥0 (x∈G)and by (2.2) we have Z

G

|f0| − |f0|2 dµ= 0.

Hence|f0(x)|=|f0(x)|2for allx∈G. Thus, we have|f0(x)|= 1or|f0(x)|= 0 for allx ∈ G, therefore |f(x)| = kfk or|f(x)| = 0for all x ∈ G. For this reason we obtain an equality in the Hölder inequality for all1 < p < ∞,

1

p + 1q = 1and the equality 1 =

Z

G

|f|2 dµ=kfkpkfkq holds.

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Negative Results Concerning Fourier Series

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2. Suppose there is a1< p <2such that kfkpkfkq = 1 =

Z

G

|f|2 dµ.

Then the equality in the Hölder inequality holds. For this reason there are nonnegative numbersAandB not both 0 such that

A|f(x)|p =B|f(x)|q (x∈G).

Thus, there is ac > 0such that|f| = cor|f| = 0for allx ∈G(c =kfk).

Then |f| · kfk = |f|2. Integrating boths part of the last equation we have kfk1kfk = 1. We obtain a contradiction.

However, the following lemma states much more.

Lemma 2.2. Let Gbe a finite group with discrete topology and normalized Haar measureµ, and letf be a complex valued function onG. Thus, the functionΨ(p) :=

kfkpkfkq(1p + 1q = 1)is a monotone decreasing function on the interval[1,2].

Proof. Letf0 := kfkf

. Then Ψ(p) = kfk2kf0kpkf0kq. Letm be the order of the groupG. We take the elements ofGin the order,G ={g1, g2, . . . , gm}, to obtain the numbers

ai :=|f0(gi)| ≤1 (i= 1, . . . , m), with which we write

Ψ(p) = kfk2 m

m

X

i=1

api

!1p m X

i=1

aqi

!1q .

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Sinceq = p−1p ,we have

∂q

∂p =− 1

(p−1)2 =−q2 p2. Therefore,

∂Ψ

∂p = Ψ(p)

"

− 1 p2 log

m

X

i=1

api

! + 1

p Pm

i=1api logai Pm

i=1api

#

+ Ψ(p)

"

−1 q2 log

m

X

i=1

aqi

! +1

q Pm

i=1aqi logai Pm

i=1aqi

#

−q2 p2

.

The condition1< p <2ensures that

−1 q · q2

p2 =− 1

p(p−1) <−1 p, from which we have

1 Ψ(p)

∂Ψ

∂p ≤ 1 p2

"

log

m

X

i=1

aqi

!

−log

m

X

i=1

api

!#

+ 1 p

Pm

i=1api logai Pm

i=1api − Pm

i=1aqi logai Pm

i=1aqi

. Both addends in the sum above are not positive. Indeed, the facts ai ≤ 1 for all 1≤ i ≤ mandp < qimply thataqi ≤ api for all1≤ i ≤ m, from which it is clear that

(2.3) log

m

X

i=1

aqi

!

−log

m

X

i=1

api

!

≤0.

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Secondly,

h(x) :=

Pm

i=1axi logai

Pm i=1axi is a monotone increasing function. Indeed,

h0(x) = Pm

i=1axi log2ai Pm

i=1axi −(Pm

i=1axi logai)2 (Pm

i=1axi)2

= Pm

i,j=1axiaxj(logai−logaj)2 (Pm

i=1axi)2 ≥0.

Consequently, we have (2.4)

Pm

i=1api logai Pm

i=1api − Pm

i=1aqi logai Pm

i=1aqi ≤0.

By (2.3) and (2.4) we obtain ∂Ψ∂p ≤ 0for all1 < p < 2, which completes the proof of the lemma.

We can apply Lemma2.1 and Lemma2.2 to obtain similar properties forΥk(p) andΨk(p)because these functions are the maximum value and the product of finite functions satisfying the conditions of the two lemmas. Consequently, we obtain:

Theorem 2.3. Let Gk be a coordinate group of G such thatskk1 = 1 for all s < mk. Then Υk(p) ≡ 1. Otherwise, the function Υk(p) is a strictly monotone decreasing function on the interval[1,2].

The functionΨk(p) ≡ 1ifsik1 = 1for alls < mi andi ≤ k. Otherwise, the functionΨk(p)is a strictly monotone decreasing function on the interval[1,2].

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It is important to remark that the functions Υk(p) and Ψk(p) are monotone in- creasing if p > 2. It follows from the property Υk(p) = Υk

p p−1

. In order to illustrate these properties we plot the values ofΥ(p)for the groupS3.

1 1.05 1.1 1.15 1.2 1.25 1.3

2 4 6 8 10

p

Figure 1: Values ofΥ(p)for the groupS3

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3. Negative Results

Theorem 3.1. Letpbe a fixed number on the interval(1,2)and 1p +1q = 1. IfGis a group with unbounded sequenceΨk(p), then the operatorSn is not of type (p, p) or(q, q).

Proof. To prove this theorem, chooseik < mk the index for which the normalized coordinate functionϕikk of the finite groupGk satisfies

ϕikk p

ϕikk

q = max

s<mk

skkpskkq. Define

fk(x) :=ϕikk(x)

ϕikk(x)

q−2 (x∈Gk).

Thus,|fk(x)|p =|ϕikk(x)|qandfk(x)ϕikk(x) =|ϕikk(x)|q ∈R+ifϕikk(x)6= 0. Hence both equalities hold in Hölder’s inequality. For this reason

(3.1)

Z

Gk

fkϕikkk

ϕikk

p =kfkkp ϕikk

q

ϕikk p. Ifkis an arbitrary positive integer andn:=Pk−1

j=0ijMj, then defineFk ∈Lp(G)by Fk(x) :=

k−1

Y

j=0

fj(xj) (x= (x0, x1, . . .)∈G).

SincekFkkp =Qk−1

j=0kfjkp,it follows from (3.1) that kSn+1Fk−SnFkkp =

Z

G

Fkψn

nkp

(3.2)

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Negative Results Concerning Fourier Series

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=

k−1

Y

j=0

Z

G

fjϕsjj

sjkp ≥Ψk(p)kFkkp.

On the other hand, ifSnis of type(p, p), then there exists aCp >0such that kSn+1Fk−SnFkkp ≤ kSn+1Fkkp+kSnFkkp ≤2CpkFkkp

for eachk >0, which contradicts (3.2) because the sequenceΨk(p)is not bounded.

For this reason, the operatorsSnare not uniformly of type(p, p). By a duality argu- ment (see [6]) the operators Sn cannot be uniformly of type (q, q). This completes the proof of the theorem.

By Theorem3.1we obtain:

Theorem 3.2. LetGbe a bounded group and suppose that all the same finite groups appearing in the product ofGhave the same systemϕat all of their occurrences. If the sequenceΨis unbounded, then the operatorSnis not of type(p, p)for allp6= 2.

Proof. If the sequenceΨk = Ψk(1)is not bounded, there exists a finite groupF with system{ϕs : 0≤s <|F|}(|F|is the order of the groupF) which appears infinitely many times in the product ofGand

Υ(1) := max

s<|F|sk1sk>1.

Hence by Theorem2.3we have

Υ(p) := max

s<|F|skpskq >1

for allp6= 2. Denote byl(k)the number of times the groupF appears in the firstk

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coordinates ofG. Thusl(k)→ ∞ifk → ∞and Ψk(p)≥

l(k)

Y

i=1

Υ(p)→ ∞ ifk→ ∞,

for allp6= 2. Consequently, the groupGsatisfies the conditions of Theorem3.1for all1< p <2. This completes the proof of the theorem.

Corollary 3.3. If G is the complete product ofS3 with the system ϕ appearing in Section2, then the operatorSnis not of type(p, p)for allp6= 2.

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References

[1] G. BENKE, Trigonometric approximation theory in compact totally discon- nected groups, Pacific J. of Math., 77(1) (1978), 23–32.

[2] G. GÁT AND R. TOLEDO,Lp-norm convergence of series in compact totally disconected groups, Anal. Math., 22 (1996), 13–24.

[3] E. HEWITTANDK. ROSS Abstract Harmonic Analysis I, Springer-Verlag, Hei- delberg, 1963.

[4] F. SCHIPP, On Walsh function with respect to weights, Math. Balkanica, 16 (2002), 169–173.

[5] P. SIMON, On the divergence of Fourier series with respect to weighted Walsh systems, East Journal on Approximations, 9(1) (2003), 21–30.

[6] R. TOLEDO, On Hardy-norm of operators with property ∆, Acta Math. Hun- gar., 80(3) (1998), 157–168.

[7] R. TOLEDO, Representation of product systems on the interval[0,1], Acta Acad.

Paed. Nyíregyháza, 19(1) (2003), 43–50.

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