Bounds for Zeta and Related Functions

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Bounds for Zeta and Related Functions Journal of Inequalities in Pure and Applied Mathematics BOUNDS FOR ZETA AND RELATED FUNCTIONS volume 6, issue 5, article 134, P. CERONE 2005. School of Computer Science and Mathematics Received 13 April, 2005; Victoria University accepted 24 August, 2005. PO Box 14428, MCMC 8001 Communicated by: F. Qi VIC, Australia. EMail: [email protected] URL: http://rgmia.vu.edu.au/cerone/ Abstract Contents JJ II J I Home Page Go Back Close c 2000 Victoria University ISSN (electronic): 1443-5756 Quit 114-05 Abstract Sharp bounds are obtained for expressions involving Zeta and related functions at a distance of one apart. Since Euler discovered in 1736 a closed form ex- pression for the Zeta function at the even integers, a comparable expression for the odd integers has not been forthcoming. The current article derives sharp bounds for the Zeta, Lambda and Eta functions at a distance of one apart. The methods developed allow an accurate approximation of the function values at Bounds for Zeta and Related the odd integers in terms of the neighbouring known function at even integer Functions values. The Dirichlet Beta function which has explicit representation at the odd P. Cerone integer values is also investigated in the current work. Cebyševˇ functional bounds are utilised to obtain tight upper bounds for the Zeta function at the odd integers. Title Page Contents 2000 Mathematics Subject Classification: Primary: 26D15, 11Mxx, 33Exx; Sec- ondary: 11M06, 33E20, 65M15. JJ II Key words: Euler Zeta function, Dirichlet beta, eta and lambda functions, Sharp bounds, Cebyševˇ functional. J I This paper is based on the talk given by the author within the “International Go Back Conference of Mathematical Inequalities and their Applications, I”, December 06- 08, 2004, Victoria University, Melbourne, Australia [http://rgmia.vu.edu.au/ Close conference ] Quit Page 2 of 42 J. Ineq. Pure and Appl. Math. 6(5) Art. 134, 2005 http://jipam.vu.edu.au Contents 1 Introduction ......................................... 4 2 The Euler Zeta and Related Functions ................... 5 3 An Identity and Bounds Involving the Eta and Related Func- tions ............................................... 14 4 Some Zeta Related Numerics ........................... 23 5 An Identity and Bounds Involving the Beta Function ....... 28 6 Zeta Bounds via Cebyševˇ .............................. 31 Bounds for Zeta and Related References Functions P. Cerone Title Page Contents JJ II J I Go Back Close Quit Page 3 of 42 J. Ineq. Pure and Appl. Math. 6(5) Art. 134, 2005 http://jipam.vu.edu.au 1. Introduction The present paper represents in part a review of the recent work of the author in obtaining sharp bounds for expressions involving functions at a distance of one apart. The main motivation for the work stems from the fact that Zeta and related functions are explicitly known at either even function values (Zeta, Lambda and Eta) or at odd function values as for the Dirichlet Beta function. The approach of the current paper is to investigate integral identities for the η (x) β (x) secant slope for and from which sharp bounds are procured. The Bounds for Zeta and Related results for η (x) of Section 3 are extended to the ζ (x) and λ (x) functions be- Functions η (x) cause of the relationship between them. The sharp bounds procured in the P. Cerone for ζ (x) are obtained, it is argued, in a more straightforward fashion than in the earlier work of Alzer [2]. Some numerical illustration of the results relating to the approximation of the Zeta function at odd integer values is undertaken in Title Page Section 4. Contents The technique for obtaining the η (x) bounds is also adapted to developing the bounds for β (x) in Section 5. JJ II The final Section 6 of the paper investigates the use of bounds for the Ce-ˇ J I byšev function in extracting upper bounds for the odd Zeta functional values Go Back that are tighter than those obtained in the earlier sections. However, this ap- proach does not seem to be able to provide lower bounds. Close Quit Page 4 of 42 J. Ineq. Pure and Appl. Math. 6(5) Art. 134, 2005 http://jipam.vu.edu.au 2. The Euler Zeta and Related Functions The Zeta function ∞ X 1 (2.1) ζ(x) := , x > 1 nx n=1 was originally introduced in 1737 by the Swiss mathematician Leonhard Euler (1707-1783) for real x who proved the identity Bounds for Zeta and Related −1 Functions Y 1 (2.2) ζ(x) := 1 − , x > 1, px P. Cerone p where p runs through all primes. It was Riemann who allowed x to be a complex Title Page z variable and showed that even though both sides of (2.1) and (2.2) diverge for Contents Re(z) ≤ 1, the function has a continuation to the whole complex plane with a simple pole at z = 1 with residue 1. The function plays a very significant JJ II role in the theory of the distribution of primes (see [2], [4], [5], [15] and [16]). J I One of the most striking properties of the zeta function, discovered by Riemann himself, is the functional equation Go Back πz Close (2.3) ζ(z) = 2zπz−1 sin Γ(1 − z)ζ(1 − z) 2 Quit that can be written in symmetric form to give Page 5 of 42 − z z − 1−z 1 − z J. Ineq. Pure and Appl. Math. 6(5) Art. 134, 2005 (2.4) π 2 Γ ζ(z) = π ( 2 )Γ ζ(1 − z). 2 2 http://jipam.vu.edu.au In addition to the relation (2.3) between the zeta and the gamma function, these functions are also connected via the integrals [13] 1 Z ∞ tx−1dt (2.5) ζ(x) = t , x > 1, Γ(x) 0 e − 1 and 1 Z ∞ tx−1dt (2.6) ζ(x) = , x > 0, t Bounds for Zeta and Related C(x) 0 e + 1 Functions where P. Cerone Z ∞ (2.7) C(x) := Γ(x) 1 − 21−x and Γ(x) = e−ttx−1dt. 0 Title Page In the series expansion Contents ∞ JJ II text X tm (2.8) = B (x) , et − 1 m m! J I m=0 Go Back where B (x) are the Bernoulli polynomials (after Jacob Bernoulli), B (0) = m m Close Bm are the Bernoulli numbers. They occurred for the first time in the formula [1, p. 804] Quit m Page 6 of 42 X Bn+1(m + 1) − Bn+1 (2.9) kn = , n, m = 1, 2, 3,.... n + 1 k=1 J. Ineq. Pure and Appl. Math. 6(5) Art. 134, 2005 http://jipam.vu.edu.au One of Euler’s most celebrated theorems discovered in 1736 (Institutiones Cal- culi Differentialis, Opera (1), Vol. 10) is 22n−1π2n (2.10) ζ(2n) = (−1)n−1 B ; n = 1, 2, 3,.... (2n)! 2n The result may also be obtained in a straight forward fashion from (2.6) and a change of variable on using the fact that Z ∞ 2n−1 n−1 t Bounds for Zeta and Related (2.11) B2n = (−1) · 4n 2πt dt 0 e − 1 Functions from Whittaker and Watson [25, p. 126]. P. Cerone We note here that 2n ζ(2n) = Anπ , Title Page where Contents n−1 j−1 n−1 n X (−1) A = (−1) · + A n (2n + 1)! (2j + 1)! n−j JJ II j=1 1 J I and A1 = 3! . Further, the Zeta function for even integers satisfy the relation (Borwein et Go Back al. [4], Srivastava [21]) Close −1 n−1 1 X Quit ζ(2n) = n + ζ(2j)ζ(2n − 2j), n ∈ N\{1} . 2 Page 7 of 42 j=1 Despite several efforts to find a formula for ζ(2n+1), (for example [22, 23]), J. Ineq. Pure and Appl. Math. 6(5) Art. 134, 2005 there seems to be no elegant closed form representation for the zeta function at http://jipam.vu.edu.au the odd integer values. Several series representations for the value ζ(2n + 1) have been proved by Srivastava and co-workers in particular. From a long list of these representations, [22, 23], we quote only a few H − log π (2.12) ζ(2n + 1) = (−1)n−1π2n 2n+1 (2n + 1)! n−1 ∞ # X (−1)k ζ(2k + 1) X (2k − 1)! ζ(2k) + + 2 , (2n − 2k + 1)! π2k (2n + 2k + 1)! 22k k=1 k=1 Bounds for Zeta and Related Functions 2n "n−1 k−1 (2π) X (−1) k ζ(2k) P. Cerone (2.13) ζ(2n + 1) = (−1)n n(22n+1 − 1) (2n − 2k)! π2k k=1 ∞ # X (2k)! ζ(2k) Title Page + , (2n + 2k)! 22k Contents k=0 and JJ II "n−1 (2π)2n X (−1)k−1k ζ(2k + 1) J I (2.14) ζ(2n + 1) = (−1)n (2n − 1)22n + 1 (2n − 2k + 1)! π2k Go Back k=1 ∞ # X (2k)! ζ(2k) Close + , n = 1, 2, 3,.... (2n + 2k + 1)! 22k Quit k=0 There is also an integral representation for ζ (n + 1) namely, Page 8 of 42 2n+1 Z δ n+1 (2π) J. Ineq. Pure and Appl. Math. 6(5) Art. 134, 2005 (2.15) ζ(2n + 1) = (−1) · B2n+1 (t) cot (πt) dt, http://jipam.vu.edu.au 2δ (n + 1)! 0 1 where δ = 1 or 2 ([1, p. 807]). Recently, Cvijovic´ and Klinkowski [12] have given the integral representations (2.16) ζ(2n + 1) 2n+1 Z δ n+1 (2π) = (−1) · −2n B2n+1 (t) tan (πt) dt, 2δ (1 − 2 ) (2n + 1)! 0 and 2n+1 Z δ n π Bounds for Zeta and Related Functions (2.17) ζ(2n + 1) = (−1) · −(2n+1) E2n (t) csc (πt) dt.
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