Journal of Inequalities in Pure and Applied Mathematics LOCALIZATION OF FACTORED FOURIER SERIES HÜSEYİN BOR Department of Mathematics Erciyes University 38039 Kayseri, Turkey volume 6, issue 2, article 40, 2005. Received 20 April, 2005; accepted 02 May, 2005. Communicated by: L. Leindler EMail: bor@erciyes.edu.tr URL: http://fef.erciyes.edu.tr/math/hbor.htm Abstract Contents JJ J II I Home Page Go Back Close c 2000 Victoria University ISSN (electronic): 1443-5756 126-05 Quit Abstract 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. 2000 Mathematics Subject Classification: 40D15, 40G99, 42A24, 42B15. Key words: Absolute summability, Fourier series, Local property. Localization of Factored Fourier Series Contents 1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2 Known Results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3 The Main Result . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . References 3 5 6 Hüseyin Bor Title Page Contents JJ J II I Go Back Close Quit Page 2 of 12 J. Ineq. Pure and Appl. Math. 6(2) Art. 40, 2005 http://jipam.vu.edu.au 1. Introduction P Let an be a given infinite series with partial sums (sn ). Let (pn ) be a sequence of positive numbers such that (1.1) Pn = n X pv → ∞ as n → ∞, (P−i = p−i = 0, i ≥ 1). v=0 The sequence-to-sequence transformation tn = (1.2) 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 coefficients (pn ). P The series an is said to be summable N̄ , pn k , k ≥ 1, if (see [2]) (1.3) ∞ X n=1 Pn pn k−1 |tn − tn−1 |k < ∞. In the special case when pn = 1/(n + 1) for all values of n (resp. k = 1), N̄ , pn summability is the same as |C, 1| (resp. N̄ , pn ) summability. Also if k we take k = 1 and pn = 1/(n + 1), 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 . Localization of Factored Fourier Series Hüseyin Bor Title Page Contents JJ J II I Go Back Close Quit Page 3 of 12 J. Ineq. Pure and Appl. Math. 6(2) Art. 40, 2005 http://jipam.vu.edu.au 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 n=1 (an cos nt + bn sin nt) ≡ ∞ 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 . Localization of Factored Fourier Series Hüseyin Bor Title Page Contents JJ J II I Go Back Close Quit Page 4 of 12 J. Ineq. Pure and Appl. Math. 6(2) Art. 40, 2005 http://jipam.vu.edu.au 2. Known Results 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 (2.2) X An (t) , {log log(n + 1)}δ Localization of Factored Fourier Series Hüseyin Bor δ > 1. 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, P then the summability |R, log n, 1| of the series An (t)λn log n at a point can be ensured by a local property. Title Page Contents JJ J II I Go Back Close Quit Page 5 of 12 J. Ineq. Pure and Appl. Math. 6(2) Art. 40, 2005 http://jipam.vu.edu.au 3. The Main Result 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. sequence P Let k ≥ 1. If (λn ) is a non-negative and non-increasing such that pn λn is convergent, then the summability N̄ , pn k of the series P An (t)λn Pn at a point is a local property of the generating function f . Localization of Factored Fourier Series Hüseyin Bor We need the following lemmas for the proof of our theorem. Lemma 3.2. If (λn ) is a non-negative and non-increasing sequence such that P pn λn is convergent, where (pn ) is a sequence of positive P numbers such that Pn → ∞ as n → ∞, then Pn λn = O(1) as n → ∞ and Pn ∆λn < ∞. Pm λm = λ m pn = O(1) n=0 m X n=0 as m → ∞. n=0 Applying the Abel transform to the sum m X pn λn = O(1) Pn ∆λn = m X n=0 Contents JJ J Proof. Since (λn ) is non-increasing, we have that m X Title Page II I Go Back Close Pm n=0 pn λn , we get that Quit Page 6 of 12 pn λn − Pm λm+1 . J. Ineq. Pure and Appl. Math. 6(2) Art. 40, 2005 http://jipam.vu.edu.au Since λn ≥ λn+1 , we obtain m X Pn ∆λn ≤ Pm λm + n=0 m X p n λn n=0 = O(1) + O(1) = O(1) as m → ∞. Lemma 3.3. Let k ≥ 1 and sP n = O(1). If (λn ) is a non-negative and nonincreasing sequence such that pn λn is convergent, where (pn ) is aPsequence of positive numbers an λ n P n such that Pn → ∞ as n → ∞, then the series is summable N̄ , pn k . P Proof. Let (Tn ) be the sequence of (N̄ , pn ) means of the series an λ n P n . Then, by definition, we have n n v 1 X X 1 X pv ar λ r P r = (Pn − Pv−1 )av λv Pv . Tn = Pn v=0 r=0 Pn v=0 Then, for n ≥ 1, we have Tn − Tn−1 Localization of Factored Fourier Series Hüseyin Bor Title Page Contents JJ J II I Go Back n pn X Pv−1 Pv av λv . = Pn Pn−1 v=1 Close Quit Page 7 of 12 J. Ineq. Pure and Appl. Math. 6(2) Art. 40, 2005 http://jipam.vu.edu.au By Abel’s transformation, we have Tn − Tn−1 n−1 n−1 pn X pn X = Pv Pv sv ∆λv − Pv 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 < ∞, Title Page Now, applying Hölder’s inequality with indices k and k 0 , where k > 1, we get that n=2 Pn pn k−1 ≤ m+1 X n=2 Since 1 k + 1 k0 = 1 and Contents JJ J |Tn,1 |k pn Pn Pn−1 Hüseyin Bor for r = 1, 2, 3, 4. n=1 m+1 X Localization of Factored Fourier Series II I Go Back ( n−1 X )( k |sv | Pv Pv ∆λv v=1 1 n−1 X Pn−1 v=1 )k−1 Pv Pv ∆λv Close . Quit Page 8 of 12 n−1 X v=1 Pv Pv ∆λv ≤ Pn−1 n−1 X v=1 Pv ∆λv , J. Ineq. Pure and Appl. Math. 6(2) Art. 40, 2005 http://jipam.vu.edu.au 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) n → ∞. as v=1 Therefore m+1 X n=2 Pn pn k−1 k |Tn,1 | = O(1) = O(1) = O(1) m+1 X n=2 m X v=1 m X n−1 pn X |sv |k Pv Pv ∆λv Pn Pn−1 v=1 k |sv | Pv Pv ∆λv Localization of Factored Fourier Series m+1 X pn P P n=v+1 n n−1 Pv ∆λv = O(1) Hüseyin Bor Title Page as m → ∞, Contents v=1 by virtue of the hypotheses of Theorem 3.1 and Lemma 3.2. Again m+1 X n=2 Pn pn k−1 |Tn,2 |k ≤ m+1 X n=2 pn Pn Pn−1 = O(1) m+1 X v=2 m X ( n−1 X )( |sv |k (Pv λv )k pv v=1 1 n−1 X Pn−1 v=1 n−1 pn X |sv |k (Pv λv )k pv Pn Pn−1 v=1 m+1 X pn = O(1) |sv | (Pv λv ) pv P P v=1 n=v+1 n n−1 k k )k−1 pv JJ J II I Go Back Close Quit Page 9 of 12 J. Ineq. Pure and Appl. Math. 6(2) Art. 40, 2005 http://jipam.vu.edu.au = O(1) m X |sv |k (Pv λv )k v=1 = O(1) m X pv Pv |sv |k (Pv λv )k−1 pv λv v=1 = O(1) m X 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 m+1 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 m X X Pn k |Tn,4 | = |sn |k (Pn λn )k−1 pn λn pn n=1 n=1 = O(1) m X pn λn = O(1) Localization of Factored Fourier Series Hüseyin Bor Title Page Contents JJ J as m → ∞, II I Go Back 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. pn n=1 This completes the proof of Lemma 3.3. Close Quit Page 10 of 12 J. Ineq. Pure and Appl. Math. 6(2) Art. 40, 2005 http://jipam.vu.edu.au 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 k ≥ 1 and and sn P = O(1). If (λn ) is a non-negative and λn is convergent, then the series P non-increasing sequence such that 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. Localization of Factored Fourier Series Hüseyin Bor Title Page Contents JJ J II I Go Back Close Quit Page 11 of 12 J. Ineq. Pure and Appl. Math. 6(2) Art. 40, 2005 http://jipam.vu.edu.au References [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. Localization of Factored Fourier Series Hüseyin Bor Title Page Contents JJ J II I Go Back Close Quit Page 12 of 12 J. Ineq. Pure and Appl. Math. 6(2) Art. 40, 2005 http://jipam.vu.edu.au