Journal of Inequalities in Pure and Applied Mathematics http://jipam.vu.edu.au/ Volume 6, Issue 2, Article 40, 2005 LOCALIZATION OF FACTORED FOURIER SERIES HÜSEYİN BOR D EPARTMENT OF M ATHEMATICS E RCIYES U NIVERSITY 38039 K AYSERI , T URKEY bor@erciyes.edu.tr URL: http://fef.erciyes.edu.tr/math/hbor.htm Received 20 April, 2005; accepted 02 May, 2005 Communicated by L. Leindler A BSTRACT. In this paper we deal with a main theorem on the local property of | N̄ , pn |k summability of factored Fourier series, which generalizes some known results. Key words and phrases: Absolute summability, Fourier series, Local property. 2000 Mathematics Subject Classification. 40D15, 40G99, 42A24, 42B15. 1. I NTRODUCTION P Let an be a given infinite series with partial sums (sn ). Let (pn ) be a sequence of positive numbers such that n X (1.1) Pn = pv → ∞ as n → ∞, (P−i = p−i = 0, i ≥ 1). v=0 The sequence-to-sequence transformation (1.2) tn = n 1 X p v sv Pn v=0 defines the sequence (tn ) of the (N̄ , pn ) means of the sequence (sn ) generated by the sequence of coefficientsP(pn ). The series an is said to be summable N̄ , pn k , k ≥ 1, if (see [2]) k−1 ∞ X Pn (1.3) |tn − tn−1 |k < ∞. pn n=1 In the special case when pn = 1/(n + 1) for all values of n (resp. k = 1), N̄ , pn k summability is the same as |C, 1| (resp. N̄ , pn ) summability. Also if we take k = 1 and pn = 1/(n + 1), ISSN (electronic): 1443-5756 c 2005 Victoria University. All rights reserved. 126-05 2 H ÜSEYIN B OR summability N̄ , pn k is equivalent to the summability |R, log n, 1|. A sequence (λn ) is said to be convex if ∆2 λn ≥ 0 for every positive integer n, where ∆2 λn = ∆λn − ∆λn+1 and ∆λn = λn − λn+1 . Let f (t) be a periodic function with period 2π and integrable (L) over (−π, π). Without any loss of generality we may assume that the constant term in the Fourier series of f (t) is zero, so that Z π (1.4) f (t)dt = 0 −π and (1.5) f (t)∼ ∞ X (an cos nt + bn sin nt) ≡ n=1 ∞ X An (t). n=1 It is well known that the convergence of the Fourier series at t = x is a local property of the generating function f (i.e. it depends only on the behaviour of f in an arbitrarily small neighbourhood of x), and hence the summability of the Fourier series at t = x by any regular linear summability method is also a local property of the generating function f . 2. K NOWN R ESULTS Mohanty [4] has demonstrated that the |R, log n, 1| summability of the factored Fourier series X (2.1) An (t) log(n + 1) at t = x, is a local property of the generating function of f , whereas the |C, 1| summability of this series is not. Matsumoto [3] improved this result by replacing the series (2.1) by X An (t) (2.2) , δ > 1. {log log(n + 1)}δ Generalizing the above result Bhatt [1] proved the following theorem. P −1 Theorem A. If (λn ) is a convex sequence such that n λn is convergent, then the summaP bility |R, log n, 1| of the series An (t)λn log n at a point can be ensured by a local property. 3. T HE M AIN R ESULT The aim of the present paper is to prove a more general theorem which includes of the above results as special cases. Also it should be noted that the conditions on the sequence (λn ) in our theorem, are somewhat more general than in the above theorem. Now we shall prove the following theorem. Theorem 3.1. Let k ≥ 1. If (λn ) is a non-negative sequence such that and non-increasing P P pn λn is convergent, then the summability N̄ , pn k of the series An (t)λn Pn at a point is a local property of the generating function f . We need the following lemmas for the proof of our theorem. P Lemma 3.2. If (λn ) is a non-negative and non-increasing sequence such that pn λn is convergent, where (pn ) is a sequence of positive numbers such that P → ∞ as n → ∞, then n P Pn λn = O(1) as n → ∞ and Pn ∆λn < ∞. J. Inequal. Pure and Appl. Math., 6(2) Art. 40, 2005 http://jipam.vu.edu.au/ L OCALIZATION OF FACTORED F OURIER S ERIES 3 Proof. Since (λn ) is non-increasing, we have that m m X X Pm λm = λ m pn = O(1) pn λn = O(1) n=0 as m → ∞. n=0 Pm Applying the Abel transform to the sum n=0 pn λn , we get that m m X X Pn ∆λn = pn λn − Pm λm+1 . n=0 n=0 Since λn ≥ λn+1 , we obtain m m X X Pn ∆λn ≤ Pm λm + p n λn n=0 n=0 = O(1) + O(1) = O(1) as m → ∞. Lemma 3.3. P Let k ≥ 1 and sn = O(1). If (λn ) is a non-negative and non-increasing sequence such that pn λn is convergent, of positive numbers such that Pn → P where (pn ) is a sequence ∞ as n → ∞, then the series an λn Pn is summable N̄ , pn k . P Proof. Let (Tn ) be the sequence of (N̄ , pn ) means of the series an λn Pn . Then, by definition, we have n v n 1 X 1 X X Tn = pv ar λ r P r = (Pn − Pv−1 )av λv Pv . Pn v=0 r=0 Pn v=0 Then, for n ≥ 1, we have Tn − Tn−1 n pn X = Pv−1 Pv av λv . Pn Pn−1 v=1 By Abel’s transformation, we have Tn − Tn−1 n−1 n−1 pn X pn X = Pv Pv sv ∆λv − P v s v p v λv Pn Pn−1 v=1 Pn Pn−1 v=1 n−1 pn X − Pv pv+1 sv λv+1 + sn pn λn Pn Pn−1 v=1 = Tn,1 + Tn,2 + Tn,3 + Tn,4 , say. By Minkowski’s inequality for k > 1, to complete the proof of Lemma 3.3, it is sufficient to show that ∞ X (3.1) (Pn /pn )k−1 |Tn,r |k < ∞, for r = 1, 2, 3, 4. n=1 Now, applying Hölder’s inequality with indices k and k 0 , where k1 + k10 = 1 and k > 1, we get that ( n−1 )( )k−1 m+1 m+1 n−1 X Pn k−1 X X X p 1 n |Tn,1 |k ≤ |sv |k Pv Pv ∆λv Pv Pv ∆λv . p P P P n n n−1 n−1 n=2 v=1 n=2 v=1 Since n−1 X Pv Pv ∆λv ≤ Pn−1 v=1 J. Inequal. Pure and Appl. Math., 6(2) Art. 40, 2005 n−1 X Pv ∆λv , v=1 http://jipam.vu.edu.au/ 4 H ÜSEYIN B OR it follows by Lemma 3.2 that 1 n−1 X Pn−1 v=1 Pv Pv ∆λv ≤ n−1 X Pv ∆λv = O(1) as n → ∞. v=1 Therefore m+1 X n=2 Pn pn k−1 k |Tn,1 | = O(1) m+1 X n−1 pn X |sv |k Pv Pv ∆λv Pn Pn−1 v=1 n=2 = O(1) m X |sv |k Pv Pv ∆λv v=1 = O(1) m X m+1 X pn P P n=v+1 n n−1 Pv ∆λv = O(1) as m → ∞, v=1 by virtue of the hypotheses of Theorem 3.1 and Lemma 3.2. Again ( n−1 )( )k−1 m+1 n−1 m+1 X pn X X X Pn k−1 1 k k |Tn,2 | ≤ |sv | (Pv λv )k pv pv p P P Pn−1 v=1 n n n−1 n=2 v=1 n=2 = O(1) m+1 X v=2 = O(1) m X n−1 pn X |sv |k (Pv λv )k pv Pn Pn−1 v=1 k k |sv | (Pv λv ) pv v=1 = O(1) m X |sv |k (Pv λv )k v=1 = O(1) = O(1) m X v=1 m X m+1 X pn P P n=v+1 n n−1 pv Pv |sv |k (Pv λv )k−1 pv λv pv λv = O(1) as m → ∞, v=1 in view of the hypotheses of Theorem 3.1 and Lemma 3.2. Using the fact that Pv < Pv+1 , similarly we have that m+1 m X Pn k−1 X k |Tn,3 | = O(1) pv+1 λv+1 = O(1) as m → ∞. pn n=2 v=1 Finally, we have that k−1 m X Pn n=1 pn k |Tn,4 | = m X |sn |k (Pn λn )k−1 pn λn n=1 = O(1) m X pn λn = O(1) as m → ∞, n=1 by virtue of the hypotheses of the theorem and Lemma 3.2. Therefore, we get that k−1 m X Pn |Tn,r |k = O(1) as m → ∞, for r = 1, 2, 3, 4. p n n=1 J. Inequal. Pure and Appl. Math., 6(2) Art. 40, 2005 http://jipam.vu.edu.au/ L OCALIZATION OF FACTORED F OURIER S ERIES This completes the proof of Lemma 3.3. 5 In the particular case if we take pn = 1 for all values of n in Lemma 3.3, then we get the following corollary. Corollary 3.4. Let P k ≥ 1 and and sn = O(1). If (λnP ) is a non-negative and non-increasing sequence such that λn is convergent, then the series nan λn is summable |C, 1|k . Proof of Theorem 3.1. Since the behaviour of the Fourier series, as far as convergence is concerned, for a particular value of x depends on the behaviour of the function in the immediate neighbourhood of this point only, hence the truth of Theorem 3.1 is a consequence of Lemma 3.3. If we take pn = 1 for all values of n in this theorem, then we get a new local property result concerning the |C, 1|k summability. R EFERENCES [1] S.N. BHATT, An aspect of local property of |R, log n, 1| summability of the factored Fourier series, Proc. Nat. Inst. Sci. India, 26 (1960), 69–73. [2] H. BOR, On two summability methods, Math. Proc. Cambridge Philos Soc., 97 (1985), 147–149. [3] K. MATSUMOTO, Local property of the summability |R, log n, 1|, Tôhoku Math. J. (2), 8 (1956), 114–124. [4] R. MOHANTY, On the summability |R, log w, 1| of Fourier series, J. London Math. Soc., 25 (1950), 67–72. J. Inequal. Pure and Appl. Math., 6(2) Art. 40, 2005 http://jipam.vu.edu.au/