Acta Mathematica Academiae Paedagogicae Nyíregyháziensis Tomus 14 (1998), 19-23 A HARDY{LITTLEWOOD{LIKE INEQUALITY ON COMPACT TOTALLY DISCONNECTED SPACES I. Blahota Abstract. In this paper we deal with a new system was introduced by Gat (see [Gat1]). This is a common generalization of several well-known systems (see the follows). We prove an inequality of type Hardy-Littlewood with respect to this system. Introduction, Examples Let P = N nf0g; and let m := (m0 ; m1 ; :::) denote a sequence of positive integers not less than 2: Denote by Gmj a set, where the number of the elements of Gmj is mj (j 2 P): Dene the measure on Gmj as follows k (fj g) := m1 (j 2 Gmk ; k 2 N ) : k Dene the set Gm as the complete direct product of the sets Gmj ; with the product of the topologies and measures (denoted by ). This product measure is a regular Borel one on Gm with (Gm ) = 1: If the sequence m is bounded, then Gm is called bounded Vilenkin space, else its name is unbounded one. The elements of Gm can be represented by sequences x := (x0 ; x1; :::) (xj 2 Gmj ): It easy to give a base the neighborhoods of Gm : I0 (x) := Gm ; In (x) := fy 2 Gm jy0 = x0 ; :::; yn,1 = xn,1 g for x 2 Gm ; n 2 N . Dene In := In (0) for n 2 P. If M0 := 1; Mk+1 := mk Mk (k 2 N ); 1 P then every n 2 N can be uniquely expressed as n = nj Mj ; where nj 2 Gmj (j 2 P) j =0 and only a nite number of nj 's dier from zero. We use the following notations. Let P 1 (k ) jnj := maxfk 2 N : nk 6= 0g (that is, Mjnj n < Mjnj+1) and n = j=k nk Mk . Denote by Lp (Gm ) the usual Lebesgue spaces (k:kp the corresponding norms) (1 p 1), An the algebra generated by the sets In (x) (x 2 Gm ) and En the conditional expectation operator with respect to An (n 2 N ). From now the boundedness of the Vilenkin space Gm is supposed. 1980 Mathematics Subject Classication (1985 Revision ). primary: 42C10, secondary: 42C15. Research supported by the Hungarian National Foundation for Scientic Research (OTKA) , grant no. F020334 and by the Hungarian \M}uvel}odesi es Kozoktatasi Miniszterium", grant no. FKFP 0710/1997. Typeset by AMS-TEX 1 2 I. BLAHOTA The concept of the maximal Hardy space H 1(Gm ) is dened by the maximal function f := supn jEn f j (f 2 L1(Gm )) , saying that f belongs to the Hardy space H 1 (Gm ) if f 2 L1 (Gm). H 1 (Gm) is a Banach space with the norm kf kH := kf k 1 1 This deniton is suitable if the sequence m is bounded. In this case a good propery of the space H 1 (Gm ) is the atomic structure [SWS]. A Rfunction a is said to be atom if a = 1 or a : Gm ! C ; ja(x)j jIn j,1; supp a(x) In and a(x) = 0: We say that f element is of the Hardy space H (Gm ) (or in brief H ), In if there exists j 2C (j 2 P) that 1 P jj j < 1; and if exists aj (j 2 P) atoms, that j =1 1 P f = j aj : Moreover, H is Banach space with the norm j =1 kf kH := inf 1 X i=0 ji j; P where the inmum is taken over all decompositions f = 1 i=0 i ai 2 H . If the sequence m is bounded (in this paper this is supposed), then H = H 1 , moreover, the two norms are equivalent. (If the sequence m is not bounded , then the situation changes.) Next we introduce on Gm an orthonormal system (see [Gat1]) we call Vilenkin-like system. The complex valued functions which we call the generalized Rademacher functions rkn : Gm ! C have these properties: i. rkn is Ak+1 measurable (i.e. rkn (x) depends only on x0 ; :::; xk (x 2 Gm )), rk0 = 1 for all k; n 2 N . ii. If Mk is a divisor of n; l and n(k+1) = l(k+1) (k; l; n 2 N ), then 1 if n = l ; k k n l Ek (rk rk ) = 0 if nk 6= lk (z is the complex conjugate of z). iii. If Mk is a divisor of n (that is, n = nk Mk + nk+1Mk+1 + ::: + njnj Mjnj). Then mX k ,1 nk =0 jrkn (x)j = mk 2 for all x 2 Gm . p iv. There exists a > 1 for which krkn k1 mk =. Dene the Vilenkin-like system := ( n : n 2 N ) as follows. n := 1 Y k=0 rkn k ; n 2 N : ( ) Q A HARDY{LITTLEWOOD... 3 j rn k ). The Vilenkin-like system is orthonormal (see (Since rk0 = 1, then n := jkn=0 k [Gat2]). And now let us list some well-known examples to this system. 1. The Vilenkin and the Walsh system. For more on these see e.g. [SWS, AVD] 2. The group of 2-adic (m-adic) integers (if mk = 2 for each k 2 N then 2-adic). [HR, SW2, Tai] 3. Noncommutative Vilenkin groups (In this case the group is the cartesian product of common nite groups.) [GT, Gat2] 4. A system in the eld of number theory. This system (on Vilenkin groups) was a new tool in order to investigate limit periodic arithmetical functions. [Mau] 5. The UDMD product system (is introduced by F. Schipp on the Walsh-Paley group). [SW2, SW] 6. The universal contractive projections system (UCP) (is introduced by F. Schipp). [Sch4]) For more on these examples and their proves see [Gat1]. Finally, let us introduce the usual denitions of the Fourier-analysis. With notation already adopted for f 2 L1 (Gm ) we dene the Fourier coecients and partial sums by ( ) fb(k) := Sn f := The Dirichlet kernels: Dn (y; x) := It is clear that nX ,1 k=0 Z Gm f k d fb(k) k nX ,1 k=0 Sn f (x) = (n 2 P; S0 f := 0): k (y ) k (x) Z Gm (k 2 N ) (n 2 P; D0 := 0): f (x)Dn(y; x)d(x): Result and Proof Theorem. There exists a C > 0 absolute constant that if f 2 H (Gm); then 1 X k,1 jf^(k)j C kf kH : k=1 Proof of the theorem. Since f 2 H (Gm ); let us form f := 1 P atoms, and jk j < 1: k=1 1 X 1 P k ak (x); where ak (x) are k=1 1 1 1 1 X X X X , 1 ^ , 1 k jf (k)j = k j j a^i (k)j jj j k,1 ja^j (k)j; j =1 j =1 k=1 k=1 k=1 4 I. BLAHOTA that is why it will be sucient to show that there exists C > 0 absolute constant that for all a(x) atoms 1 X k,1 ja^(k)j C: k=1 Let a(x) 2 H (Gm ) be an atom. If a 1 then Z jkj Y jkj Y (j ) k k(j) a^(k) = k = E0 ( k ) = E0 ( rj ) = E0 (Ejkj ( rj )) = j =1 j =1 Gm jkY j,1 (j) E0( rkj Ejkj(rj0kjrkjk(jk ) )) = 0 j =1 because k(jkj) = kjkjMjkj 6= 0 if k 2 P and Ek (rknrkl ) = 0 if nk 6= lk : In this case the statement of the theorem is trivial. So, assume that aR6 1: In this case let In be an interval for which ja(x)j jInj,1 ; supp a(x) In and a(x) = 0: In Since supp a(x) In than j j a^(k) = Z Gm Z a(x) k (x) = a(x) k (x): In If k = 0; :::; Mn , 1 than k (x) depend only on the rst n coordinate of x; hence the function k (x) on the set In is invariable Z Z In In a^(k) = a(x) k (x) = c a(x) = 0 1 1 X X , 1 =) k ja^(k)j = k,1 ja^(k)j: k=1 k=Mn Using the Cauchy{Buniakovski{Schwarz inequality v v u u 1 1 1 X X X u u , 1 2 t t ja^(k)j k,2; k ja^(k)j k=Mn k=Mn and from Bessel's inequality k=Mn v u 1 X u t ja^(k)j2 ka(x)k2; k=Mn A HARDY{LITTLEWOOD... 5 and estimate the approximate sum of the Riemann integral of function x12 v u 1 X u t k,2 pC : Mn k=Mn These gives by 1 X k,1 ja^(k)j C; Z k=Mn ka(x)k = jaj jIn j, jInj = jIn j, Mn = mn Mn CMn ; 2 2 2 2 1 +1 +1 In because of the boundedness of the sequence m. This completes the proof of Theorem. Acknowledgement I would like to thank Professor G. Gat for setting the problem. 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[Sch4] Schipp, F., Universal conctractive projections and a.e. convergence, Probability Theory and Applications, Essays to the Memory of Jozsef Mogyorodi, Eds.: J. Galambos, I. Katai, Kluwer Academic Publishers, Dordrecht, Boston, London (1992), 47-75. [SW] Schipp,F. , Wade,W.R., Norm convergence and summability of Fourier series with respect to certain product systems in Pure and Appl. Math. Approx. Theory, vol. 138, Marcel Dekker, New York-Basel-Hong Kong, 1992, pp. 437-452. [SW2] Schipp,F. , Wade,W.R., Transforms on normed elds, Janus Pannonius Tudomanyegyetem, Pecs, 1995. [SWS] Schipp,F.,Wade,W.R.,Simon,P.,Pal,J., Walsh series: an introduction to dyadic harmonic analysis, Adam Hilger, Bristol and New York, 1990. [Tai] Taibleson,M.H., Fourier Analysis on Local Fields, Princeton Univ. Press., Princeton ,N.J., 1975. [Vil] Vilenkin , N.Ja., On a class of complete orthonormal systems (in Russian), Izv. Akad. Nauk. SSSR, Ser. Math. 11 (1947), 363-400. Bessenyei College, Dept. of Math., Nyregyhaza, P.O.Box 166., H{4400,Hungary E-mail : blahota@ny1.bgytf.hu (Received October 1, 1997)