International Journal of Analysis and Applications Volume 18, Number 6 (2020), 957-964 URL: https://doi.org/10.28924/2291-8639 DOI: 10.28924/2291-8639-18-2020-957 GENERALIZED ABSOLUTE RIESZ SUMMABILITY OF INFINITE SERIES AND FOURIER SERIES BAĞDAGÜL KARTAL∗ Department of Mathematics, Erciyes University, 38039 Kayseri, Turkey ∗Corresponding author: bagdagulkartal@erciyes.edu.tr Abstract. In this paper, two known theorems dealing with |N̄,pn|k summability of infinite series and Fourier series have been generalized to ϕ−|N̄,pn; β|k summability. 1. Introduction A sequence (An) is said to be δ-quasi-monotone if An → 0, An > 0 ultimately and ∆An ≥ −δn, where ∆An=An −An+1 and δ = (δn) is a sequence of positive numbers (see [1]). A sequence (gn) is said to be of bounded variation, denoted by (gn) ∈BV, if ∑∞ n=1 |∆gn| < ∞. Let ∑ an be a given infinite series with the partial sums (sn). Let (ϕn) be a sequence of positive real numbers. The series ∑ an is said to be summable ϕ−|N̄,pn; β|k, k ≥ 1 and β ≥ 0, if (see [22]) ∞∑ n=1 ϕβk+k−1n |un −un−1| k < ∞ where (pn) is a sequence of positive numbers such that Pn = n∑ v=0 pv →∞ as n →∞ (P−i = p−i = 0, i ≥ 1) , Received August 13th, 2020; accepted September 1st, 2020; published September 14th, 2020. 2010 Mathematics Subject Classification. 26D15, 40D15, 40F05, 40G99. Key words and phrases. absolute summability; Fourier series; Hölder’s inequality; infinite series; Minkowski’s inequality; Riesz mean; summability factor. ©2020 Authors retain the copyrights of their papers, and all open access articles are distributed under the terms of the Creative Commons Attribution License. 957 https://doi.org/10.28924/2291-8639 https://doi.org/10.28924/2291-8639-18-2020-957 Int. J. Anal. Appl. 18 (6) (2020) 958 and un = 1 Pn n∑ v=0 pvsv. For ϕn = Pn pn and β = 0, ϕ −|N̄,pn; β|k summability reduces to |N̄,pn|k summability (see [2]). Taking ϕn = n, β = 0 and pn = 1 for all values of n, ϕ −|N̄,pn; β|k summability reduces to |C, 1|k summability (see [8]). If we write Xn = n∑ v=1 pv/Pv, then (Xn) is a positive increasing sequence tending to infinity with n. In [3], the following theorem on δ-quasi-monotone sequences has been proved. Theorem 1.1. Let (λn) → 0 as n →∞ and (pn) be a sequence of positive numbers such that Pn = O(npn) as n →∞. Suppose that there exists a sequence of numbers (An) which is δ-quasi-monotone with∑ nXnδn < ∞, ∑ AnXn is convergent, and |∆λn| ≤ |An| for all n. If the condition m∑ n=1 pn Pn |tn|k = O(Xm) as m →∞(1.1) is satisfied, where (tn) is the n-th (C, 1) mean of the sequence (nan), then the series ∑ anλn is summable |N̄,pn|k, k ≥ 1. Lemma 1.1. [3] Under the conditions of Theorem 1.1, we have that |λn|Xn = O (1) as n →∞,(1.2) nXnAn = O(1) as n →∞,(1.3) ∞∑ n=1 nXn|∆An| < ∞.(1.4) 2. Main Result There are some papers on absolute summability (see [4–6,9–12,16–18,23–25]). Now we generalize Theorem 1.1 as in the following form. Theorem 2.1. Let (ϕn) be a sequence of positive real numbers such that ϕnpn = O(Pn),(2.1) m+1∑ n=v+1 ϕβk−1n 1 Pn−1 = O ( ϕβkv 1 Pv ) as m →∞.(2.2) Int. J. Anal. Appl. 18 (6) (2020) 959 If all conditions of Theorem 1.1 are satisfied with the condition (1.1) replaced by m∑ n=1 ϕβk−1n |tn| k = O(Xm) as m →∞,(2.3) then the series ∑ anλn is summable ϕ−|N̄,pn; β|k, k ≥ 1 and 0 ≤ β < 1/k. 3. Proof of Theorem 2.1 Let (In) indicates (N̄,pn) mean of the series ∑ anλn. Then, for n ≥ 1, we obtain ∆̄In = In − In−1 = pn PnPn−1 n∑ v=1 Pv−1avλv = pn PnPn−1 n∑ v=1 Pv−1λv v vav. Applying Abel’s transformation, we get ∆̄In = pn PnPn−1 n−1∑ v=1 λv+1 v Pvtv − pn PnPn−1 n−1∑ v=1 v + 1 v pvλvtv + pn PnPn−1 n−1∑ v=1 v + 1 v Pvtv∆λv + (n + 1) nPn pnλntn = In,1 + In,2 + In,3 + In,4. For the proof of Theorem 2.1, it is sufficient to show that ∞∑ n=1 ϕβk+k−1n | In,r | k< ∞, for r = 1, 2, 3, 4. First, m+1∑ n=2 ϕβk+k−1n | In,1 | k ≤ m+1∑ n=2 ϕβk+k−1n ( pn PnPn−1 )k (n−1∑ v=1 Pv |tv| |λv+1| v )k = m+1∑ n=2 ϕβk−1n ( ϕnpn Pn )k 1 Pkn−1 ( n−1∑ v=1 Pv |tv| |λv+1| v )k . Here (2.1) gives ( ϕnpn Pn )k = O(1), also using Hölder’s inequality, we obtain m+1∑ n=2 ϕβk+k−1n | In,1 | k = O(1) m+1∑ n=2 ϕβk−1n 1 Pn−1 ( n−1∑ v=1 Pv |tv| k |λv+1|k v )( 1 Pn−1 n−1∑ v=1 Pv v )k−1 . Now using the fact that Pv = O(vpv), m+1∑ n=2 ϕβk+k−1n | In,1 | k = O(1) m+1∑ n=2 ϕβk−1n 1 Pn−1 ( n−1∑ v=1 pv |tv| k |λv+1|k )( 1 Pn−1 n−1∑ v=1 pv )k−1 . Int. J. Anal. Appl. 18 (6) (2020) 960 Then, we have m+1∑ n=2 ϕβk+k−1n | In,1 | k = O(1) m+1∑ n=2 ϕβk−1n 1 Pn−1 n−1∑ v=1 pv |tv| k |λv+1|k = O(1) m∑ v=1 pv|λv+1|k−1|λv+1| |tv| k m+1∑ n=v+1 ϕβk−1n 1 Pn−1 . Here, by using (2.2) and (1.2), m+1∑ n=2 ϕβk+k−1n | In,1 | k = O(1) m∑ v=1 ϕβkv pv Pv |λv+1| |tv| k = O(1) m∑ v=1 ϕβk−1v ( ϕvpv Pv ) |λv+1| |tv| k . Again, from (2.1), we obtain m+1∑ n=2 ϕβk+k−1n | In,1 | k = O(1) m∑ v=1 ϕβk−1v |λv+1| |tv| k . Hence, we get m+1∑ n=2 ϕβk+k−1n | In,1 | k = O(1) m−1∑ v=1 ∆|λv+1| v∑ r=1 ϕβk−1r |tr| k + O(1)|λm+1| m∑ v=1 ϕβk−1v |tv| k = O(1) m−1∑ v=1 |Av+1|Xv+1 + O(1)|λm+1|Xm+1 = O(1) as m →∞, by using Abel’s transformation, hypotheses of Theorem 2.1, and Lemma 1.1. Now, we have m+1∑ n=2 ϕβk+k−1n | In,2 | k = O(1) m+1∑ n=2 ϕβk+k−1n ( pn PnPn−1 )k (n−1∑ v=1 pv |λv| |tv| )k = O(1) m+1∑ n=2 ϕβk−1n ( ϕnpn Pn )k 1 Pkn−1 ( n−1∑ v=1 pv |λv| |tv| )k = O(1) m+1∑ n=2 ϕβk−1n 1 Pkn−1 ( n−1∑ v=1 pv |λv| |tv| )k . Using Hölder’s inequality, we get m+1∑ n=2 ϕβk+k−1n | In,2 | k = O(1) m+1∑ n=2 ϕβk−1n 1 Pn−1 ( n−1∑ v=1 pv |λv| k |t v |k )( 1 Pn−1 n−1∑ v=1 pv )k−1 = O(1) m∑ v=1 pv|λv|k|tv|k m+1∑ n=v+1 ϕβk−1n 1 Pn−1 . Int. J. Anal. Appl. 18 (6) (2020) 961 By (2.2), (2.1) and (1.2), we get m+1∑ n=2 ϕβk+k−1n | In,2 | k = O(1) m∑ v=1 ϕβk−1v |λv||tv| k. Here, using Abel’s transformation as in In,1, we have m+1∑ n=2 ϕβk+k−1n | In,2 | k = O(1) as m →∞. Again, using Hölder’s inequality, we have m+1∑ n=2 ϕβk+k−1n | In,3 | k = O(1) m+1∑ n=2 ϕβk+k−1n ( pn PnPn−1 )k (n−1∑ v=1 Pv |tv| |∆λv| )k = O(1) m+1∑ n=2 ϕβk−1n ( ϕnpn Pn )k 1 Pkn−1 ( n−1∑ v=1 Pv |tv| |Av| )k = O(1) m+1∑ n=2 ϕβk−1n 1 Pn−1 ( n−1∑ v=1 pv |tv| k (v |Av|)k )( 1 Pn−1 n−1∑ v=1 pv )k−1 = O(1) m+1∑ n=2 ϕβk−1n 1 Pn−1 n−1∑ v=1 pv |tv| k (v |Av|)k−1(v |Av|). Using (1.3), we get (v |Av|)k−1 = O(1), then m+1∑ n=2 ϕβk+k−1n | In,3 | k = O(1) m∑ v=1 pv|tv|kv |Av| m+1∑ n=v+1 ϕβk−1n 1 Pn−1 . Now using the conditions (2.2) and (2.1), we get m+1∑ n=2 ϕβk+k−1n | In,3 | k = O(1) m∑ v=1 ϕβk−1v |tv| kv |Av| . Then, we have m+1∑ n=2 ϕβk+k−1n | In,3 | k = O(1) m−1∑ v=1 ∆(v |Av|) v∑ r=1 ϕβk−1r |tr| k + O(1)m |Am| m∑ v=1 ϕβk−1v |tv| k = O(1) m−1∑ v=1 ∆(v |Av|)Xv + O(1)m |Am|Xm = O(1) m−1∑ v=1 vXv|∆Av| + O(1) m−1∑ v=1 |Av+1|Xv+1 + O(1)m |Am|Xm = O(1) as m →∞, by using Abel’s transformation, hypotheses of Theorem 2.1, and Lemma 1.1. Int. J. Anal. Appl. 18 (6) (2020) 962 Finally, we get m∑ n=1 ϕβk+k−1n | In,4 | k = O(1) m∑ n=1 ϕβk+k−1n ( pn Pn )k |λn|k−1|λn||tn|k = O(1) m∑ n=1 ϕβk−1n |λn||tn| k. Here, as in In,1, we get m∑ n=1 ϕβk+k−1n | In,4 | k = O(1) as m →∞. Hence, the proof of Theorem 2.1 is completed. 4. Applications There are some different papers dealing with applications of Fourier series (see [14, 15, 19–21]). Let f be a periodic function with period 2π and Lebesgue integrable over (−π,π). The trigonometric Fourier series of f is defined as f(x) ∼ 1 2 a0 + ∞∑ n=1 (an cos nx + bn sin nx) = ∞∑ n=0 Cn(x) where a0 = 1 π ∫ π −π f(x)dx, an = 1 π ∫ π −π f(x) cos(nx)dx and bn = 1 π ∫ π −π f(x) sin(nx)dx. Write φ(t) = 1 2 {f(x + t) + f(x− t)} and φ1(t) = 1 t ∫ t 0 φ(u)du. If φ1(t) ∈ BV(0,π), then tn(x) = O(1), where tn(x) is the n-th (C, 1) mean of the sequence (nCn(x)) (see [7]). By using this, the following theorem has been obtained in [3]. Theorem 4.1. If φ1(t) ∈BV(0,π), and the sequences (pn), (λn) and (Xn) satisfy the conditions of Theorem 1.1, then the series ∑ Cn(x)λn is summable | N̄,pn |k, k ≥ 1. The following theorem gives a generalization of Theorem 4.1 for ϕ−|N̄,pn; β|k summability. Theorem 4.2. If φ1(t) ∈BV(0,π), and the sequences (pn), (λn), (An), (ϕn) and (Xn) satisfy the conditions of Theorem 2.1, then the series ∑ Cn(x)λn is summable ϕ−|N̄,pn; β|k, k ≥ 1 and 0 ≤ β < 1/k. Int. J. Anal. Appl. 18 (6) (2020) 963 5. Conclusions If we take ϕn = Pn pn and β = 0 in Theorem 2.1, then the condition (2.3) reduces to the condition (1.1), and the conditions (2.1) and (2.2) are provided. Thus, Theorem 2.1 reduces to Theorem 1.1. If we take ϕn = n, β = 0 and pn = 1 for all values of n, then we have a result for |C, 1|k summability of an infinite series (see [13]). Also, if we take ϕn = Pn pn and β = 0 in Theorem 4.2, then we get Theorem 4.1. 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