Journal of Inequalities in Pure and Applied Mathematics CESÁRO MEANS OF N -MULTIPLE TRIGONOMETRIC FOURIER SERIES volume 7, issue 3, article 86, 2006. USHANGI GOGINAVA Department of Mechanics and Mathematics Tbilisi State University Chavchavadze str. 1 Tbilisi 0128, Georgia Received 06 March, 2006; accepted 08 March, 2006. Communicated by: L. Leindler EMail: z_goginava@hotmail.com Abstract Contents JJ J II I Home Page Go Back Close c 2000 Victoria University ISSN (electronic): 1443-5756 068-06 Quit Abstract Zhizhiashvili proved sufficient condition for the Cesáro summability by negative order of N-multiple trigonometric Fourier series in the space Lp , 1 ≤ p ≤ ∞. In this paper we show that this condition cannot be improved . 2000 Mathematics Subject Classification: 42B08. Key words: Trigonometric system, Cesáro means, Summability. Cesáro Means of N -multiple Trigonometric Fourier Series Ushangi Goginava N N Let R be N -dimensional Euclidean space. The elements of R are denoted by x = (x1 , . . . , xN ), y = (y1 , . . . , yN ), . . . . For any x, y ∈ RN the vector (x1 + y1 , . . . , xN + yN ) of the space RN is denoted by x + y. Let P 1/2 N 2 kxk = x . i=1 i N Denote by C [0, 2] the space of continuous on [0, 2π]N , 2π-periodic relative to each variable functions with the following norm kf kC = x∈[0,2π] |f (x)| sup N and Lp [0, 2π]N , (1 ≤ p ≤ ∞) are the collection of all measurable, 2π-periodic relative to each variable functions f defined on [0, 2π]N , with the norms Z p1 p kf kp = |f (x)| dx < ∞. [0,2π] N Title Page Contents JJ J II I Go Back Close Quit Page 2 of 11 J. Ineq. Pure and Appl. Math. 7(3) Art. 86, 2006 http://jipam.vu.edu.au For the case p = ∞, by Lp [0, 2π]N we mean C [0, 2π]N . Let M := {1, 2, . . . , N } , B := {s1 , . . . , sr } , sk < sk+1 , k = 1, . . . , r − 1, B ⊂ M, B 0 := M \B. Let ∆{si } (f, x, hsi ) := f (x1 , . . . , xsi −1 , xsi + hsi , xsi +1 , . . . , xN ) − f (x1 , . . . , xsi −1 , xsi , xsi +1 , . . . , xN ) . The expression we get by successive application of operators ∆{s1 } (f, x, hs1 ) , . . . , ∆{sr } (f, x, hsr ) will be denoted by ∆B (f, x, hs1 , . . . , hsr ) , i. e. ∆B (f, x, hs1 , . . . , hsr ) := ∆{sr } ∆B\{sr } , x, hsr . N p Let f ∈ L [0, 2π] . The expression ωB (δs1 , . . . , δsr ; f ) := sup ∆B (f, ·, hs1 , . . . , hsr ) |hsi |≤δsi ,i=1,...,r p p is called a mixed or a particular modulus of continuity in the L norm, when card(B) ∈ [2, N ] or card(B) = 1. The total modulus of continuity of the function f ∈ Lp [0, 2π]N in the Lp norm is defined by ω (δ, f )p = sup kf (· + h) − f (·)kp (1 ≤ p ≤ ∞) . khk≤δ Suppose that f is a Lebesgue integrable function on [0, 2π]N , 2π periodic relative to each variable.Then its N -dimensional Fourier series with respect to Cesáro Means of N -multiple Trigonometric Fourier Series Ushangi Goginava Title Page Contents JJ J II I Go Back Close Quit Page 3 of 11 J. Ineq. Pure and Appl. Math. 7(3) Art. 86, 2006 http://jipam.vu.edu.au the trigonometric system is defined by ∞ X i1 =0 ··· ∞ X 2−λ(i) iN =0 where (B) ai1 ,...,iN X Z f (x) Y sin ik xk , k∈B cos ij xj j∈B 0 [0,2π]N Y cos ij xj j∈B 0 B⊂M 1 = N π Y (B) ai1 ,...,iN Y sin ik xk dx k∈B is the Fourier coefficient of f and λ (i) is the number of those coordinates of the vector i := (i1 , . . . , iN ) which are equal to zero. Let Sp1 ,...,pN (f, x) denote the (p1 , . . . , pN )-th rectangular partial sums of the N -dimensional Fourier series with respect to the trigonometric system, i. e. Sp1 ,...,pN (f, x) := p1 X ··· i1 =0 pN X X Ai1 ,...,iN (f, x) , iN =0 (B) ai1 ,...,iN B⊂M Y p1 =0 Contents JJ J cos ij xj j∈B 0 Y sin ik xk . k∈B The Cesáro (C; α1 , . . . , αN )-means of N -multiple trigonometric Fourier series defined by !−1 m mN Y N N 1 X Y X α1 ,...,αN αi −1 Aαmjj− σm1 ,...,mN (f, x) = Ami ··· pj Sp1 ,...,pN (f, x) , i=1 Ushangi Goginava Title Page where Ai1 ,...,iN (f, x) := 2−λ(i) Cesáro Means of N -multiple Trigonometric Fourier Series pN =0 j=1 II I Go Back Close Quit Page 4 of 11 J. Ineq. Pure and Appl. Math. 7(3) Art. 86, 2006 http://jipam.vu.edu.au where Aαn = (α + 1) (α + 2) · · · (α + n) , n! α 6= −1, −2, . . . , n = 0, 1, . . . . It is well-known that [4] (1) c1 (α) nα ≤ Aαn ≤ c2 (α) nα . For the uniform summability of Cesáro means of negative order of onedimensional trigonometric Fourier series the following result of Zygmund [3] is well-known: if ω (δ, f )C = o (δ α ) Cesáro Means of N -multiple Trigonometric Fourier Series Ushangi Goginava and α ∈ (0, 1), then the trigonometric Fourier series of the function f is uniformly (C, −α) summable to f. In [2] Zhizhiashvili proved sufficient conditions for the convergence of Cesáro means order of N -multiple trigonometric Fourier series in the space of negative N p L [0, 2π] , (1 ≤ p ≤ ∞). The following is proved. N p Theorem A (Zhizhiashvili). Let f ∈ L [0, 2π] for some p ∈ [1, +∞] and α1 + · · · + αN < 1, where αi ∈ (0, 1), i = 1, 2, . . . , N . If ω (δ, f )p = o δ α1 +···+αN , JJ J then Page 5 of 11 −α1 ,...,−αN σm (f ) − f 1 ,...,mN p →0 as mi → ∞, i = 1, . . . , N. Title Page Contents II I Go Back Close Quit J. Ineq. Pure and Appl. Math. 7(3) Art. 86, 2006 http://jipam.vu.edu.au In case p = ∞ the sharpness of Theorem A has been proved by Zhizhiashvili [2]. The following theorem shows that Theorem A cannot be improved in cases 1 ≤ p < ∞. Moreover, we prove the following Theorem 1 (for N = 1 see [1]). Let α1 + · · · + αN < 1 and αi ∈ (0, 1), N i = 1, 2, . . . , N, then there exists the function f0 ∈ C [0, 2π] for which (2) ω (δ, f0 )C = O δ α1 +···+αN and lim m→∞ −α1 ,...,−αN σm,...,m (f0 ) − f0 1 Cesáro Means of N -multiple Trigonometric Fourier Series > 0. Ushangi Goginava Proof. We can define the sequence {nk : k ≤ 1} satisfying the properties ∞ X 1 1 (3) , α1 +···+αN = O α1 +···+αN n n j k j=k+1 (4) k−1 X 1−(α1 +···+αN ) nj 1−(α1 +···+αN ) = O nk j=1 (5) , Title Page Contents JJ J II I Go Back 1 nk−1 < . nk k Consider the function f0 defined by f0 (x1 , . . . , xN ) := Close Quit Page 6 of 11 ∞ X j=1 fj (x1 , . . . , xN ) , J. Ineq. Pure and Appl. Math. 7(3) Art. 86, 2006 http://jipam.vu.edu.au where 1 N Y sin nj xi . nαj 1 +···+αN i=1 N From (3) it is easy to show that f0 ∈ C [0, 2π] . First we shall prove that fj (x1 , . . . , xN ) := ωi (δ, f )C = O δ α1 +···+αN , (6) Let 1 nk ≤δ< 1 . nk−1 i = 1, . . . , N. Then from (3) and (4) we can write that |f0 (x1 , . . . , xi−1 , xi + δ, xi+1 , . . . , xN ) − f0 (x1 , . . . , xi−1 , xi , xi+1 , . . . , xN )| ∞ X 1 ≤ α1 +···+αN |sin nj (xi + δ) − sin nj xi | n j=1 j ≤ ≤ k−1 X 1 j=1 nαj 1 +···+αN k−1 X nj δ +O 1 nαk 1 +···+αN 1 1−(α1 +···+αN ) = O δnk−1 +O nαk 1 +···+αN = O δ α1 +···αN , j=1 nαj 1 +···+αN |sin nj (xi + δ) − sin nj xi | + 2 which proves (6). ∞ X 1 j=k nαj 1 +···+αN Cesáro Means of N -multiple Trigonometric Fourier Series Ushangi Goginava Title Page Contents JJ J II I Go Back Close Quit Page 7 of 11 J. Ineq. Pure and Appl. Math. 7(3) Art. 86, 2006 http://jipam.vu.edu.au Since ω (δ, f )C ≤ N X ωi (δ, f )C , i=1 we obtain the proof of estimation (2). N 1 1 ,...,−αN Next we shall prove that σn−α (f ) diverge in the metric of L [0, 2π] . 0 k ,...,nk It is clear that (7) 1 ,...,−αN σn−α (f0 ) − f0 k ,...,nk 1 1 ,...,−αN ≥ σn−α (fk ) k ,...,nk − − k−1 X Cesáro Means of N -multiple Trigonometric Fourier Series 1 1 ,...,−αN (fj ) − fj σn−α k ,...,nk j=1 ∞ X 1 ,...,−αN σn−α (fj ) k ,...,nk C j=k+1 ∞ X kfj kC Title Page Contents JJ J It is evident that 1 ,...,−αN σn−α (fj ) = 0, k ,...,nk − j=k = I − II − III − IV. (8) Ushangi Goginava C j = k + 1, k + 2, . . . . II I Go Back Close Using (3) for IV we have (9) IV ≤ ∞ X Quit 1 nα1 +···+αN j=k j =O 1 nαk 1 +···+αN . Page 8 of 11 J. Ineq. Pure and Appl. Math. 7(3) Art. 86, 2006 http://jipam.vu.edu.au Since [2] 1 ,...,−αN σn−α (fj ) − fj k ,...,nk C X =O ωB B⊂M 1 , fj nk and ωi 1 , fj nk 1 =O nαj 1 +···+αN nj nk P αs ! ns∈B k C ! , from (4) and (5) we get (10) II = O =O 1 k−1 X 1−(α +···+αN ) nk 1 j=1 1 k−2 X 1−(α +···+αN ) nk 1 j=1 Cesáro Means of N -multiple Trigonometric Fourier Series ! 1−(α1 +···+αN ) nj Ushangi Goginava 1−(α1 +···+αN ) 1−(α1 +···+αN ) nj + nk−1 1−(α1 +···+αN ) nk ! =O 1−(α +···+αN ) nk−1 1 1−(α +···+αN ) nk 1 1−(α1 +···+αN ) ! 1 k =O ! Title Page Contents JJ J = o (1) as k → ∞. II I Go Back Close Since (B) ai1 ,...,iN (fk ) = 0, and (M ) ai1 ,...,iN (fk ) = for B ⊂ M, B 6= M −α1 −···−αN , for nk Quit Page 9 of 11 i1 = · · · = iN = n k ; J. Ineq. Pure and Appl. Math. 7(3) Art. 86, 2006 0, otherwise, http://jipam.vu.edu.au from (1) we have 1 ,...,−αN (11) σn−α (fk ) k ,...,nk Z 2π Z 2π 1 1 ,...,−αN = ··· σn−α (fk ; x1 , . . . , xN ) dx1 · · · dxN k ,...,nk 0 0 2π Z ≥ Z ··· 0 = 2π 0 1 1 A−α nk Z × ··· =π N (fk ; x1 , . . . , xN ) N Y sin nk xi dx1 · · · dxN i=1 nk X 1 nk Y N X 1 −1 A−α nk− ij ··· N A−α nk i1 =0 iN =0 j=1 Z N 2π 2π Y ··· Si1 ,...,iN (fk ; x1 , . . . , xN ) sin nk xi dx1 · · · dxN 0 = πN 1 ,...,−αN σn−α k ,...,nk 1 1 A−α nk 1 1 A−α nk 0 ··· ··· i=1 1 N A−α nk 1 N A−α nk ) a(M nk ,...,nk (fk ) 1 −···−αN n−α k ≥ c (α1 , . . . , αN ) > 0. Combining (7) – (11) we complete the proof of Theorem 1. Cesáro Means of N -multiple Trigonometric Fourier Series Ushangi Goginava Title Page Contents JJ J II I Go Back Close Quit Page 10 of 11 J. Ineq. Pure and Appl. Math. 7(3) Art. 86, 2006 http://jipam.vu.edu.au References [1] U. GOGINAVA, Cesáro means of trigonometric Fourier series, Georg. Math. J., 9 (2002), 53–56. [2] L.V. ZHIZHIASHVILI, Trigonometric Fourier Series and their Conjugates, Kluwer Academic Publishers, Dobrecht, Boston, London, 1996. [3] A. ZYGMUND, Sur la sommabilite des series de Fourier des functions verfiant la condition de Lipshitz, Bull. de Acad. Sci. Ser. Math. Astronom. Phys., (1925), 1–9. [4] A. ZYGMUND, Trigonometric Series, Vol. 1, Cambridge Univ. Press, 1959. Cesáro Means of N -multiple Trigonometric Fourier Series Ushangi Goginava Title Page Contents JJ J II I Go Back Close Quit Page 11 of 11 J. Ineq. Pure and Appl. Math. 7(3) Art. 86, 2006 http://jipam.vu.edu.au