NEGATIVE RESULTS CONCERNING FOURIER SERIES ON THE COMPLETE PRODUCT OF S3 Negative Results Concerning Fourier Series R. TOLEDO Institute of Mathematics and Computer Science College of Nyíregyháza P.O. Box 166, Nyíregyháza, H-4400 Hungary R. Toledo vol. 9, iss. 4, art. 99, 2008 Title Page 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 in Lp -norm of the Fourier series based on representative product systems on the complete product of finite groups. We restrict our attention to bounded groups with unbounded sequence Ψ. The most simple example of this groups is the complete product of S3 . In this case we proved the existence of an 1 < p < 2 number for which exists an f ∈ Lp such that its n-th partial sum of Fourier series Sn do not converge to the function f in Lp -norm. In this paper we extend this ”negative” result for all 1 < p < ∞ and p 6= 2 numbers. Contents JJ II J I Page 1 of 16 Go Back Full Screen Close Contents 1 Representative Product Systems 4 2 The Sequence of Functions Ψk (p) 7 3 Negative Results 13 Negative Results Concerning Fourier Series R. Toledo vol. 9, iss. 4, art. 99, 2008 Title Page Contents JJ II J I Page 2 of 16 Go Back Full Screen Close Introduction In Section 1 we introduce basic concepts in the study of representative product systems and Fourier analysis. We also introduce the system with which we work on the complete product of S3 , i.e. the symmetric group on 3 elements (see [2]). Section 2 extends the definition of the sequence Ψ for all p ≥ 1. Finally, we use the results of Section 2 to study the convergence in the Lp -norm (p ≥ 1) of the Fourier series on bounded groups with unbounded sequence Ψ, supposing all the same finite groups appearing in the product of G have the same system ϕ at all of their occurrences. These results appear in Section 3 and they complete the statement proved by G. Gát and the author of this paper in [2] for the complete product of S3 . There have been similar results proved with respect to Walsh-like systems in [4] and [5]. Throughout this work denote by N, P, C the set of nonnegative, positive integers and complex numbers, respectively. The notation which we have used in this paper is similar to [3]. Negative Results Concerning Fourier Series R. Toledo vol. 9, iss. 4, art. 99, 2008 Title Page Contents JJ II J I Page 3 of 16 Go Back Full Screen Close 1. Representative Product Systems Let m := (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 measure µk . Let G be the compact group formed by the complete direct product of Gk with 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 of x. The compact totally disconnected group G is called a bounded group if the sequence m is bounded. If M0 := 1 and PMk+1 := mk Mk , k ∈ N, then every n ∈ N can be uniquely expressed as n = ∞ k=0 nk Mk , 0 ≤ nk < mk , nk ∈ N. This allows us to say that the sequence (n0 , n1 , . . . ) is the expansion of n with respect to m. Denote by Σk the dual object of the finite group Gk (k ∈ N). Thus each σ ∈ Σk is a set of continuous irreducible unitary representations of Gk which are equivalent to some fixed representation U (σ) . Let dσ be the dimension of its representation space and let {ζ1 , ζ2 , . . . , ζdσ } be a fixed but arbitrary orthonormal basis in the representation space. The functions (σ) ui,j (x) := hUx(σ) ζi , ζj i (i, j ∈ {1, . . . , dσ }, x ∈ Gk ) are called the coordinate functions for U (σ) and the basis {ζ1 , ζ2 , . . . , ζdσ }. In this manner for each σ ∈ Σk we obtain d2σ number of coordinate functions, in total mk 2 number √ of functions for the whole dual object of Gk . The L -norm of these functions is 1/ 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 p (σ) ϕsk (x) = dσ ui,j (x) (x ∈ Gk ). Negative Results Concerning Fourier Series R. Toledo vol. 9, iss. 4, art. 99, 2008 Title Page Contents JJ II J I Page 4 of 16 Go Back Full Screen Close Let ψ be the product system of ϕsk , namely ψn (x) := ∞ Y ϕnk k (xk ) (x ∈ G), k=0 P∞ where n is of the form n = k=0 nk Mk and x = (x0 , x1 , . . .). Thus we say that ψ is the representative product system of ϕ. The Weyl-Peter’s theorem (see [3]) ensures that the system ψ is orthonormal and complete on L2 (G). The functions ψn (n ∈ N) are not necessarily uniformly bounded, so define Negative Results Concerning Fourier Series R. Toledo vol. 9, iss. 4, art. 99, 2008 Ψk := max kψn k1 kψn k∞ n<Mk (k ∈ N). It seems that the boundedness of the sequence Ψ plays an important role in the norm convergence of Fourier series. For an integrable complex function f defined in G we define the Fourier coefficients and partial sums by Z f ψ k dµ (k ∈ N), fbk := Gm Sn f := n−1 X fbk ψk (n ∈ P). Title Page Contents JJ II J I Page 5 of 16 k=0 According to the theorem of Banach-Steinhauss, Sn f → f as n → ∞ in the Lp norm for f ∈ Lp (G) if and only if there exists a Cp > 0 such that kSn f kp ≤ Cp kf kp (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 space L2 (G), it is obvious that Sn is 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 Go Back Full Screen Close mk = 2 and Gk := Z2 , the cyclic group of order 2 for all k ∈ N. Moreover, we obtain the Vilenkin systems if the sequence m is an arbitrary sequence of integers greater than 1 and Gk := Zmk , the cyclic group of order mk for all k ∈ N. Let mk = 6 for all k ∈ N and S3 be the symmetric group on 3 elements. Let Gk := S3 for all k ∈ 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 functions ϕsk . In the notation the index k is omitted because all of the groups Gk are the same. Negative Results Concerning Fourier Series R. Toledo ϕ0 ϕ1 ϕ2 ϕ3 s s e (12) (13) (23) (123) (132) kϕ k1 kϕ k∞ 1 1 1 1 1 1 1 1 −1 1 1 1 √ √ √ √ 1 √ 2 √ 2 1 −1 −1 √ √ √ 2 2 − 2 2 √ √ √ 2 2 − 22 √ ϕ4 0 0 ϕ5 0 0 6 2 √ − 26 − 2 2 √ − √ 2 2 6 2 √ 6 2 2 2 √ − 22 √ 6 2 √ − 26 − 2 2 √ − 22 √ − 26 √ 6 2 − 2 2 3 √ 2 2 3 √ 6 3 √ 6 3 √ 6 2 √ 6 2 vol. 9, iss. 4, art. 99, 2008 Title Page Contents JJ II J I Page 6 of 16 Go Back 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 k the other hand, max kϕs k1 kϕs k∞ = 34 , thus Ψk = 43 → ∞ if k → ∞. More 0≤s<6 examples of representative product systems have appeared in [2] and [7]. Full Screen Close 2. The Sequence of Functions Ψk (p) We extend the definition of the sequence Ψ for all p ≥ 1 as follows: 1 1 Ψk (p) := max kψn kp kψn kq p ≥ 1, + = 1, k ∈ N n<Mk p q (if p = 1 then q = ∞). Notice that Ψk = Ψk (1) for all k ∈ N. Clearly, the functions Ψk (p) can be written in the form Ψk (p) = =: k−1 Y Negative Results Concerning Fourier Series R. Toledo vol. 9, iss. 4, art. 99, 2008 max kϕsi kp kϕsi kq s<mi i=0 k−1 Y i=0 Title Page Υi (p) p ≥ 1, 1 1 + = 1, k ∈ N . p q Contents Therefore, we study the product kf kp kf kq for 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 G be a finite group with discrete topology and normalized Haar measure µ, and let f be a normalized complex valued function on G (kf k2 = 1). Thus, 1. if kf k1 kf k∞ = 1, then kf kp kf kq = 1 for all p ≥ 1 and 1 p + 1 q 2. if kf k1 kf k∞ > 1, then kf kp kf kq > 1 for all p ≥ 1, p 6= 2 and + II J I Page 7 of 16 Go Back Full Screen Close = 1. 1 p JJ 1 q = 1. Proof. 1. The conditions imply the equality Z Z |f | dµ · kf k∞ = 1 = |f |2 dµ. G Let f0 := f . kf k∞ G Then Negative Results Concerning Fourier Series |f0 (x)| ≤ 1 (2.1) (x ∈ G) R. Toledo vol. 9, iss. 4, art. 99, 2008 and Z Z |f0 | dµ = (2.2) G |f0 |2 dµ. Title Page G Contents 2 Thus by (2.1) we obtain |f0 (x)| − |f0 (x)| ≥ 0 (x ∈ G) and by (2.2) we have Z |f0 | − |f0 |2 dµ = 0. JJ II J I G Page 8 of 16 Hence |f0 (x)| = |f0 (x)|2 for all x ∈ G. Thus, we have |f0 (x)| = 1 or |f0 (x)| = 0 for all x ∈ G, therefore |f (x)| = kf k∞ or |f (x)| = 0 for all x ∈ G. For this reason we obtain an equality in the Hölder inequality for all 1 < p < ∞, 1 + 1q = 1 and the equality p Z 1= |f |2 dµ = kf kp kf kq G holds. Go Back Full Screen Close 2. Suppose there is a 1 < p < 2 such that Z kf kp kf kq = 1 = |f |2 dµ. G Then the equality in the Hölder inequality holds. For this reason there are nonnegative numbers A and B not both 0 such that p q A|f (x)| = B|f (x)| Negative Results Concerning Fourier Series (x ∈ G). R. Toledo Thus, there is a c > 0 such that |f | = c or |f | = 0 for all x ∈ G (c = kf k∞ ). Then |f | · kf k∞ = |f |2 . Integrating boths part of the last equation we have kf k1 kf k∞ = 1. We obtain a contradiction. vol. 9, iss. 4, art. 99, 2008 Title Page Contents However, the following lemma states much more. Lemma 2.2. Let G be a finite group with discrete topology and normalized Haar measure µ, and let f be a complex valued function on G. Thus, the function Ψ(p) := kf kp kf kq ( p1 + 1q = 1) is a monotone decreasing function on the interval [1, 2]. Proof. Let f0 := kffk∞ . Then Ψ(p) = kf k2∞ kf0 kp kf0 kq . Let m be the order of the group G. We take the elements of G in the order, G = {g1 , g2 , . . . , gm }, to obtain the numbers ai := |f0 (gi )| ≤ 1 (i = 1, . . . , m), with which we write Ψ(p) = kf k2∞ m m X i=1 ! p1 api m X i=1 ! 1q aqi . JJ II J I Page 9 of 16 Go Back Full Screen Close Since q = p , p−1 we have ∂q 1 q2 =− = − . ∂p (p − 1)2 p2 Therefore, " # Pm p ∂Ψ 1 1 i=1 ai log ai Pm p = Ψ(p) − 2 log api + ∂p p p i=1 ai i=1 " ! # Pm q m X 1 1 i=1 ai log ai q2 q Pm q ai + + Ψ(p) − 2 log − 2 . q q p i=1 ai i=1 m X ! The condition 1 < p < 2 ensures that R. Toledo vol. 9, iss. 4, art. 99, 2008 Title Page 1 q2 1 1 <− , − · 2 =− q p p(p − 1) p from which we have " ! !# m m X X 1 ∂Ψ 1 ≤ 2 log aqi − log api Ψ(p) ∂p p i=1 i=1 Pm q Pm p ai log ai ai log ai 1 i=1 i=1 Pm p Pm q + − . p i=1 ai i=1 ai Both addends in the sum above are not positive. Indeed, the facts ai ≤ 1 for all 1 ≤ i ≤ m and p < q imply that aqi ≤ api for all 1 ≤ i ≤ m, from which it is clear that ! ! m m X X q p ai ≤ 0. (2.3) log ai − log i=1 Negative Results Concerning Fourier Series i=1 Contents JJ II J I Page 10 of 16 Go Back Full Screen Close Secondly, Pm x a log a Pm i x i h(x) := i=1 i=1 ai is a monotone increasing function. Indeed, Pm x Pm x 2 Pm x 2 i=1 ai log ai i=1 ai − ( i=1 ai log ai ) 0 h (x) = P x 2 ( m i=1 ai ) Pm x x 2 i,j=1 ai aj (log ai − log aj ) = ≥ 0. Pm x 2 ( i=1 ai ) Consequently, we have (2.4) Negative Results Concerning Fourier Series R. Toledo vol. 9, iss. 4, art. 99, 2008 Title Page Pm p Pm q ai log ai a log a i=1 Pm p Pm i q i ≤ 0. − i=1 i=1 ai i=1 ai By (2.3) and (2.4) we obtain of the lemma. ∂Ψ ∂p Contents ≤ 0 for all 1 < p < 2, which completes the proof We can apply Lemma 2.1 and Lemma 2.2 to obtain similar properties for Υk (p) and Ψk (p) because these functions are the maximum value and the product of finite functions satisfying the conditions of the two lemmas. Consequently, we obtain: kϕsk k1 Theorem 2.3. Let Gk be a coordinate group of G such that = 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 function Ψk (p) ≡ 1 if kϕsi k1 = 1 for all s < mi and i ≤ k. Otherwise, the function Ψk (p) is a strictly monotone decreasing function on the interval [1, 2]. JJ II J I Page 11 of 16 Go Back Full Screen Close It is important to remark that the functions Υk (p) and Ψk (p) aremonotone inp creasing if p > 2. It follows from the property Υk (p) = Υk p−1 . In order to illustrate these properties we plot the values of Υ(p) for the group S3 . Negative Results Concerning Fourier Series 1.3 R. Toledo vol. 9, iss. 4, art. 99, 2008 1.25 Title Page 1.2 Contents 1.15 JJ II J I 1.1 1.05 Page 12 of 16 Go Back 1 2 4 6 8 p 10 Full Screen Close Figure 1: Values of Υ(p) for the group S3 3. Negative Results Theorem 3.1. Let p be a fixed number on the interval (1, 2) and p1 + 1q = 1. If G is a group with unbounded sequence Ψk (p), then the operator Sn is not of type (p, p) or (q, q). Proof. To prove this theorem, choose ik < mk the index for which the normalized coordinate function ϕikk of the finite group Gk satisfies i i ϕ k ϕ k = max kϕsk k kϕsk k . k q k p p q s<mk Define q−2 fk (x) := ϕikk (x) ϕikk (x) (x ∈ Gk ). Thus, |fk (x)|p = |ϕikk (x)|q and fk (x)ϕikk (x) = |ϕikk (x)|q ∈ R+ if ϕikk (x) 6= 0. Hence both equalities hold in Hölder’s inequality. For this reason Z ik (3.1) fk ϕk dµk ϕikk p = kfk kp ϕikk q ϕikk p . Gk If k is an arbitrary positive integer and n := Fk (x) := k−1 Y Pk−1 j=0 ij Mj , (3.2) R. Toledo vol. 9, iss. 4, art. 99, 2008 Title Page Contents JJ II J I Page 13 of 16 Go Back Full Screen fj (xj ) (x = (x0 , x1 , . . . ) ∈ G). j=0 Since kFk kp = then define Fk ∈ Lp (G) by Negative Results Concerning Fourier Series Qk−1 kfj kp , it follows from (3.1) that Z kSn+1 Fk − Sn Fk kp = Fk ψ n dµ kψn kp j=0 G Close = k−1 Y Z j=0 G fj ϕsj dµj kϕsj kp ≥ Ψk (p)kFk kp . On the other hand, if Sn is of type (p, p), then there exists a Cp > 0 such that kSn+1 Fk − Sn Fk kp ≤ kSn+1 Fk kp + kSn Fk kp ≤ 2Cp kFk kp for each k > 0, which contradicts (3.2) because the sequence Ψk (p) is not bounded. For this reason, the operators Sn are not uniformly of type (p, p). By a duality argument (see [6]) the operators Sn cannot be uniformly of type (q, q). This completes the proof of the theorem. Negative Results Concerning Fourier Series R. Toledo vol. 9, iss. 4, art. 99, 2008 Title Page By Theorem 3.1 we obtain: Theorem 3.2. Let G be a bounded group and suppose that all the same finite groups appearing in the product of G have the same system ϕ at all of their occurrences. If the sequence Ψ is unbounded, then the operator Sn is not of type (p, p) for all p 6= 2. Proof. If the sequence Ψk = Ψk (1) is not bounded, there exists a finite group F with system {ϕs : 0 ≤ s < |F |} (|F | is the order of the group F ) which appears infinitely many times in the product of G and s s Υ(1) := max kϕ k1 kϕ k∞ > 1. s<|F | Contents JJ II J I Page 14 of 16 Go Back Full Screen Close Hence by Theorem 2.3 we have Υ(p) := max kϕs kp kϕs kq > 1 s<|F | for all p 6= 2. Denote by l(k) the number of times the group F appears in the first k coordinates of G. Thus l(k) → ∞ if k → ∞ and Ψk (p) ≥ l(k) Y Υ(p) → ∞ if k → ∞, i=1 for all p 6= 2. Consequently, the group G satisfies the conditions of Theorem 3.1 for all 1 < p < 2. This completes the proof of the theorem. Corollary 3.3. If G is the complete product of S3 with the system ϕ appearing in Section 2, then the operator Sn is not of type (p, p) for all p 6= 2. Negative Results Concerning Fourier Series R. Toledo vol. 9, iss. 4, art. 99, 2008 Title Page Contents JJ II J I Page 15 of 16 Go Back Full Screen Close References [1] G. BENKE, Trigonometric approximation theory in compact totally disconnected 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. HEWITT AND K. ROSS Abstract Harmonic Analysis I, Springer-Verlag, Heidelberg, 1963. Negative Results Concerning Fourier Series R. Toledo vol. 9, iss. 4, art. 99, 2008 [4] F. SCHIPP, On Walsh function with respect to weights, Math. Balkanica, 16 (2002), 169–173. Title Page [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. Hungar., 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. Contents JJ II J I Page 16 of 16 Go Back Full Screen Close