Acta Mathematica Academiae Paedagogicae Nyı́regyháziensis 21 (2005), 161–167 www.emis.de/journals ISSN 1786-0091 LOGARITHMIC SUMMABILITY OF FOURIER SERIES G. TKEBUCHAVA Abstract. A set of regular summations logarithmic methods is introduced. This set includes Riesz and Nörlund logarithmic methods as limit cases. The application to logarithmic summability of Fourier series of continuous and integrable functions are given. The kernels of these logarithmic methods for trigonometric system are estimated. 1. Introduction In the literature it is known Riesz and Nörlund logarithmic summation methods (see [H, HR, Z]). Applications of these methods to Fourier analysis are investigated by many authors (see for example [S, Zh, Y, MS, GG, GT]. We construct the set of logarithmic summation methods which in particular contains both mentioned methods. We study the application of these methods to Fourier series. The estimates of kernels and Lebesgue functions in trigonometric case are obtained. Necessary and sufficient condition which guarantee such logarithmic summability of Fourier series for continuous and integrable functions in corresponding metric are established. 2. Construction of logarithmic summation methods For any integers m and n such that 0 ≤ m ≤ n we put (m−1 ) n X Dk (x) X 1 Dk (x) (1) Fm,n (x) ≡ + Dm (x) + l(m, n) m−k+1 k−m+1 k=0 k=m+1 where (2) Dk (x) ≡ sin(k + 21 )x 2 sin x2 is Dirichlet kernel and (3) l(m, n) ≡ m−1 X k=0 n X 1 1 +1+ . m−k+1 k−m+1 k=m+1 2000 Mathematics Subject Classification. 42A24, 40G05. Key words and phrases. Fourier series, logarithmic summability, spaces of continuous and integrable functions. 161 162 G. TKEBUCHAVA Here and further we assume that if q < p then that l(m, n) ³ ln(n + 2). We call Pq k=p dk = 0 for any dk . It is clear tm,n f ≡ Fm,n ∗ f the logarithmic means of Fourier series of function f ∈ L1 [−π, π]. ∞ ∞ If we replace in (1) the sequence {Dn (x)}n=0 by arbitrary sequence {Sn }n=0 , then we define such logarithmic means in general case. It is easy to see that for each fixed sequence of integers {mn } under condition 0 ≤ mn ≤ n these means tmn ,n generate a regular logarithmic summation method. The set of all such methods in particular includes Riesz (for mn = 0) and Nörland (for mn = n) logarithmic methods. In the sequel C, Ci denote absolute positive constants. 3. Logarithmic means and their kernels In following proposition we estimate the kernels Fm,n . Theorem 1. There exist positive constants Ci , i = 1, 2, 0 < C1 ≤ C2 such that for any integers m and n, 0 ≤ m ≤ n holds ¾ ¾ ½ ½ ln2 (m + 2) ln2 (m + 2) 1 (4) C1 1 + ≤ kFm,n kL [−π,π] ≤ C2 1 + . ln(n + 2) ln(n + 2) In particular from Theorem 1 we obtain well-known results. Corollary 1 (see [GT, Y]). For any n ≥ 0 we have kFn,n kL1 [−π,π] ³ C ln(n + 2) kF0,n kL1 [−π,π] ³ C. Theorem 2. ³ The following ´ conditions are equivalent √ a) mn = O exp ln n as n → ∞. b) ktm,n f − f kC[−π,π] → 0 as n → ∞ ∀f ∈ C [−π, π], c) ktm,n f − f kL1 [−π,π] → 0 as n → ∞ ∀f ∈ L1 [−π, π]. Theorem 2 is corollary of Theorem 1 because the condition a) is equivalent to the boundedness of Lebesgue constants for method tmn ,n what is sufficient and necessary condition for b) and c) (see [HR], Ch. 5.) We can construct a logarithmic summation method with given possible growth of logarithmic means. In particular we have p Theorem 3. For any τ (n) ∈ [1, ln n] and mn = [exp{ τ (n) ln n}] a logarithmic means tmn ,n is such that ktmn ,n f kC[−π,π] ≤ Cτ (n)kf kC[−π,π] . Another corollaries of Theorem 1 for divergence of Fourier series of continuous function one can obtain by well-known way using the uniform boundedness principle (see [E], Ch. 10.3.2.) LOGARITHMIC SUMMABILITY OF FOURIER SERIES 163 4. Proof of Theorem 1 Proof of Theorem 1. It is sufficient to prove the inequality (4) for n > 1. First note that m+1 n−m+1 X X Dm+1−j (x) Dj+m−1 (x) 1 (5) Fm,n (x) = + Dm (x) + l(m, n) j j j=2 and (6) "Z kFm,n kL1 = 2 Since |Dk (x)| ≤ k + (7) 1 n+2 j=2 Z |Fm,n (x)|dx + 0 1 2 # π 1 n+2 |Fm,n (x)|dx ≡ 2(A1 + A2 ). ∀k ∀x ∈ [−π, π], then (see(1) , (2), (3) , (6)) 1 Z n+2 A1 = |Fm,n (x)|dx ≤ 1. 0 Further from (5) we get sin ¡m + 1 + 1 ¢ x m+1 X cos jx 1 2 Fm,n (x) = x l(m, n) 2 sin 2 j j=2 − (8) ¡ ¢ m+1 cos m + 1 + 12 x X sin jx 2 sin x2 j j=2 n−m+1 sin(m − 1 + 12 )x X cos jx 2 sin x2 j j=2 n−m+1 cos(m − 1 + 12 )x X sin jx . + 2 sin x2 j +Dm (x) + j=2 We have for A2 the following decomposition ¯ ¯ ¯ Z π Z π ¯¯ sin(m + 1 + 1 )x ¯¯ ¯¯m+1 X cos jx ¯ 1 2 ¯ ¯ ¯ ¯ dx A2 = |Fm,n (x)|dx ≤ x ¯¯ ¯ 1 1 ¯ l(m, n) 2 sin j ¯ ¯ 2 n+2 n+2 j=2 ¯ ¯ ¯¯ ¯ Z π ¯ X sin jx ¯ ¯ cos(m + 1 + 12 )x ¯ ¯m+1 ¯ ¯ ¯ dx ¯ + x ¯ ¯¯ ¯ 1 2 sin j ¯ ¯ 2 n+2 j=2 ¯ ¯ ¯¯ ¯ Z π ¯ X cos jx ¯ ¯ sin(m − 1 + 12 )x ¯ ¯n−m+1 (9) ¯ ¯ ¯ ¯ dx + x ¯ ¯¯ ¯ 1 2 sin j ¯ ¯ 2 n+2 j=2 ¯ ¯ ¯¯ ¯ Z π Z π ¯ X sin jx ¯ ¯ cos(m − 1 + 12 )x ¯ ¯n−m+1 ¯¯ ¯ ¯ dx + |D (x)| dx + m ¯¯ ¯ 1 1 2 sin x2 j ¯¯ ¯ j=2 n+2 n+2 ≡ 1 {A2,1 + A2,2 + A2,3 + A2,4 + A2,5 } . l(m, n) By convention if m = 0 then A2,1 = A2,2 = 0 and if m = n then A2,3 = A2,4 = 0. 164 G. TKEBUCHAVA Since for N ≥ 1 and−π ≤ x ≤ π we have the estimate ([Z], Ch.5.) (10) | N X sin jx j=1 then (see (9)) Z (11) A2,2 = π 1 n+2 j | ≤ C, ¯ ¯ ¯ ¯¯X ¯ Z π ¯ cos(m + 1 + 12 )x ¯ ¯m+1 ¯ sin jx ¯¯ ¯ ¯ dx ≤ C ¯¯ ¯ ¯ 1 2 sin x2 ¯ j=2 j ¯ n+2 ¯ ¯ ¯ 1 ¯ ¯ ¯ ¯ 2 sin x ¯ dx 2 ≤ C ln(n + 2) and Z (12) A2,4 = π 1 n+2 ¯ ¯ ¯¯ X ¯ ¯ Z π ¯ cos(m − 1 + 12 )x ¯ ¯n−m+1 sin jx ¯¯ ¯ ¯¯ dx ≤ C ¯ ¯¯ 1 2 sin x2 j ¯¯ ¯ j=2 n+2 ¯ ¯ ¯ 1 ¯ ¯ ¯ ¯ 2 sin x ¯ dx 2 ≤ C ln(n + 2). Moreover Z (13) A2,1 = π 1 n+2 ¯ ¯ ¯ ¯¯ ¯ m+1 X 1Z π X cos jx ¯ ¯ sin(m + 1 + 21 )x ¯ ¯m+1 ¯ ¯¯ ¯ dx ≤ C |Dm+1 (x)|dx ¯ ¯¯ ¯ 1 2 sin x2 j n+2 ¯ j=2 j ¯ j=2 ≤ C ln(m + 2)kDm+1 kL1 [−π,π] ≤ C ln2 (m + 2). Now we estimate A2,3 ¯ ¯ ¯ ¯¯ ¯ X cos jx ¯ ¯ sin(m − 1 + 21 )x ¯ ¯n−m+1 ¯ ¯ ¯ dx ¯ = x ¯ ¯¯ ¯ 1 2 sin j ¯ ¯ 2 n+2 j=2 ¯ ¯ ¯ ¯¯ ¯ 1 Z m+2 X cos jx ¯ ¯ sin(m − 1 + 21 )x ¯ ¯n−m+1 ¯ ¯ ¯ dx ¯ = x ¯ ¯¯ ¯ 1 2 sin j ¯ ¯ 2 n+2 j=2 ¯ ¯ ¯¯ ¯ Z π ¯ X cos jx ¯ ¯ sin(m − 1 + 12 )x ¯ ¯n−m+1 ¯ ¯ ¯ ¯ dx = A2,3,1 + A2,3,2 . + x ¯ ¯¯ ¯ 1 2 sin j ¯ ¯ 2 m+2 j=2 Z A2,3 (14) π Since (see [Z], Ch.5) ¯ ¯ ¯ ¯X ¯ N cos jx ¯ ¯ ≤ C + ln 1 ¯ ¯ ¯ x ¯ j=1 j ¯ then (15) ¯ ¯ ¯ s ¯ ¯X cos jx ¯ ¯ ¯ ≤ C + ln(m + 2) ¯ ¯ ¯ j=2 j ¯ and we obtain the estimates Z (16) ∀x ∈ (0, π] A2,3,1 ≤ (m + 2) 1 m+2 1 n+2 x∈[ ∀N ≥ 1 1 , π] m+2 µ ¶ 1 C + ln dx ≤ C + ln(m + 2) x LOGARITHMIC SUMMABILITY OF FOURIER SERIES and (17) Z A2,3,2 ≤ (C + ln(m + 2)) Since (18) Z A2,5 = π 1 m+2 165 ¡ ¢ 1 dx ≤ C ln2 (m + 2) + ln(m + 2) . 2 sin x2 π 1 n+2 |Dm (x)| dx ≤ kDm kL1 [−π,π] ≤ C ln(m + 2), then we have from (9), (11), (12), (13), (14), (16), (17), (18) (19) A2 ≤ C ln2 (m + 2) + C. ln(n + 2) Finally (see (6), (7), (19)) we obtain the right estimate of (4). Now we prove the left side of (4) From (8) it is evident that l(m, n)Fm,n (x) = Dm (x) + n−m+1 cos(m − 1 + 21 )x X sin jx 2 sin x2 j j=2 − m+1 m+1 cos(m + 1 + 12 )x X sin jx cos(m + 12 )x sin x X cos jx + 2 sin x2 j 2 sin x2 j j=2 j=2 − n−m+1 m+1 X cos jx cos(m + 12 )x sin x X cos jx + D (x) cos x m x 2 sin 2 j j j=2 j=2 (20) + Dm (x) cos x n−m+1 X j=2 7 cos jx X = Bk . j k=1 By virtue of (10) for all x ∈ [0, π2 ] we obtain the following estimate (21) |Bk | ≤ C x k = 1, 2, 3. 1 By virtue of estimate (15) we get for x ∈ [ m+2 , π] (22) |Bk | ≤ C ln (m + 2) k = 4, 5. Since for s ≥ 2 s X cos jx (23) j=2 j s−2 X = j=1 + sin2 j+1 2 2 x 2 j(j + 1)(j + 2) 2 sin x2 sin2 sx 1 1 3 2 + Ds (x) − − cos x s(s − 1) 2 sin2 x2 s 4 then for m ≥ 3 B6 = Dm (x) cos x m−1 X j=1 (24) j+1 sin2 2 x Dm (x) cos x sin2 m+1 1 2 x + 2 2 x j(j + 1)(j + 2) sin 2 m(m + 1) 2 sin x2 5 + Dm (x) cos x X 1 3 Dm+1 (x) − Dm (x) cos x − Dm (x) cos2 x = B6,i . m+1 4 i=1 166 G. TKEBUCHAVA It is clear that for x ∈ [0, π] by analogical assertions it follows for j = 2, . . . , 5 C (25) |B6,j | ≤ . x √ Since for 0 ≤ k ≤ m + 1 and ½ ¾ 1 1 π 1 π 1 <x< √ x ∈ Jm = x : sin(m + )x ≥ , 2 2 2 m+1 2 m+1 follows 0 ≤ kx ≤ π 2 and sin kx ≥ B6,1 ≥ Dm (x) cos x (26) ≥C 2 π kx, then we obtain X √ 1≤k≤ m+1 sin(m + 12 )x 2 sin x2 sin2 k+1 1 2 x 2 k(k + 1)(k + 2) sin x2 X √ 1≤k≤ m+1 1 C ≥ ln(m + 2), k x x ∈ Jm . We note that if m = n then B7 = 0 and if m = n − 1 then B7 ≤ For m < n − 1 we have (see (23)) B7 = Dm (x) cos x n−m−1 X j=1 C x ∀x ∈ [−π, π]. sin2 j+1 2 2 x j(j + 1)(j + 2) 2 sin2 x2 x sin2 n−m+1 Dm (x) cos x 2 2 x (n − m + 1)(n − m) 2 sin 2 1 + Dm (x) cos x Dm−n+1 (x) n−m+1 5 X 3 − Dm (x) cos x − Dm (x) cos2 x = B7,i 4 i=1 + (27) and we obtain the same estimates for B7,i , i = 2, . . . , 5 as for B6,i , i = 2, . . . , 5. We note also that B7,1 > 0. Thus for x ∈ Jm and m big enough we have (see (21-22), (24-27)) ½ ¾ 1 ln(m + 2) C ln(m + 2) |Fm,n (x)| ≥ C − − C ln(m + 2) ≥ C . l(m, n) x x xl(m, n) It imply that for m big enough Z ln2 (m + 2) (28) kFm,n kL1 [−π,π] ≥ |Fm,n (x)|dx ≥ C ln (n + 2) Jm and since for all m and n holds (29) kFm,n kL1 [−π,π] ¯Z ¯ ≥ ¯¯ 2π 0 ¯ ¯ Fm,n (x)dx¯¯ = 1 then from (28) and (29) follows the left side estimate in (4). ¤ References [E] R. Edwards. Fourier series. A modern introduction. Vol. 1. 2nd ed., volume 64 of Graduate Textes in Mathematics. Springer-Verlag, New York, Heidelberg. Berlin, 1979. [GG] G. Gát and U. Goginava. Uniform and L-convergence of logarithmic means of Walsh-Fourier series. to appear in Acta Math. Sinica. [GT] U. Goginava and G. Tkebuchava. Convergence of logarithmic means of Fourier series. submitted. LOGARITHMIC SUMMABILITY OF FOURIER SERIES 167 [H] G. Hardy. Divergent series. Oxford: At the Clarendon Press, 1949. [HR] G. Hardy and W. Rogosinski. Fourier series. 3rd ed., volume 38 of Cambridge Tracts in Mathematics and Mathematical Physics. Cambridge: At the University Press, 1956. [MS] F. Móricz and A. Siddiqi. Approximation by Nörlund means of Walsh-Fourier series. J. Approximation Theory, 70(3):375–389, 1992. [S] O. Szász. On the logarithmic means of rearranged partial sums of a Fourier series. Bull. Am. Math. Soc., 48:705–711, 1942. [Y] K. Yabuta. Quasi-Tauberian theorems, applied to the summability of Fourier series by Riesz’s logarithmic means. Tohoku Math. J., II. Ser., 22:117–129, 1970. [Zh] L. Zhizhiashvili. Trigonometric Fourier series and their conjugates. Mathematics and its Applications (Dordrecht). Kluwer Academic Publishers, 1996. [Z] A. Zygmund. Trigonometric series. Vol. 1, 2nd ed. Cambridge: At the University Press, 1959. Received March 16, 2005. Department of Mechanics and Mathematics, Tbilisi State University, Chavchavadze str. 1, Tbilisi 0128, Georgia E-mail address: george tkebuchava@hotmail.com