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M athematical I nequalities & A pplications Volume 16, Number 4 (2013), 971–979 doi:10.7153/mia-16-76

AN EXPERIMENTAL CONJECTURE INVOLVING CLOSED–FORM EVALUATION OF SERIES ASSOCIATED WITH THE ZETA FUNCTIONS

JUNESANG CHOI AND HARI M. SR I VA S TAVA

(Communicated by Yeol Je Cho)

Abstract. The subject of closed-form summation of series involving the Zeta functions has been remarkably widely investigated. Recently, in the course of his trying to give a closed-form expression for the Dirichlet beta function β(2n)(n ∈ N),Lima[16] posed a very interesting experimental conjecture for a closed-form evaluation of a certain class of series involving the ζ(s). Here, in the present sequel to Lima’s work, we aim at verifying correctness of Lima’s conjecture and presenting several general analogues of Lima’s conjecture. Our demonstration and derivations are based mainly upon a known formula for series associated with the Zeta functions. Relevant connections of some specialized results of the main identities presented here with those obtained in earlier works are also pointed out.

1. Introduction and preliminaries

A rather classical (over two centuries old) theorem of Christian Goldbach (1690– 1764), which was stated in a letter dated 1729 from Goldbach to Daniel Bernoulli (1700–1782), was revived in 1986 by Shallit and Zikan [20] as the following problem:

− ∑ (ω − 1) 1 = 1, (1.1) ω∈S where S denotes the set of all nontrivial integer kth powers, that is, S := nk : n,k ∈ N \{1} . (1.2)

In terms of the Riemann Zeta function ζ(s) defined by

⎧ ∞ ∞ ⎪ 1 1 1 ⎪ ∑ = ∑ ℜ(s) > 1 ⎨ s − −s ( − )s n=1 n 1 2 n=1 2n 1 ζ(s) := (1.3) ⎪ 1 ∞ (−1)n−1 ⎩⎪ ∑ ℜ(s) > 0; s = 1 , − 1−s s 1 2 n=1 n

Mathematics subject classification (2010): Primary 11M35, 11M36; Secondary 11M06, 33B15. Keywords and phrases: , psi (or digamma) function, Riemann Zeta function, , multiple gamma functions, Euler-Mascheroni constant, Glaisher-Kinkelin constant, series in- volving the Zeta functions.

 Ð c ,Zagreb 971 Paper MIA-16-76 972 JUNESANG CHOI AND HARI M. SRIVASTAVA

Goldbach’s theorem (1.1) assumes the elegant form (cf. Shallit and Zikan [20, p. 403]): ∞ ∑ {ζ(k) − 1} = 1 (1.4) k=2 or, equivalently, ∞ ∑ F ζ(k) = 1, (1.5) k=2 where F(x) := x − [x] denotes the fractional part of x ∈ R. Asamatteroffact,itis fairly straightforward to observe also that

∞ 1 ∑ (−1)k F ζ(k) = , (1.6) k=2 2

∞ 3 ∞ 1 ∑ F ζ(2k) = and ∑ F (ζ(2k + 1)) = . (1.7) k=1 4 k=1 4 The subject of closed-form summation of series involving the Zeta functions has been remarkably widely investigated (see [8, 9, 10, 11, 13, 21, 22, 23, 24]). Among the various methods and techniques used in the vast literature on the subject, Srivastava and Choi [23, 24] gave reasonably detailed accounts of those using the binomial theo- rem, generating functions, multiple Gamma functions (see [2, 3, 4, 5, 9, 10, 15, 25]), and hypergeometric identities, presented a rather extensive collection of closed-form sums of series involving the Zeta functions, and showed that many of those summation formulas find their applications in the evaluations of the determinants of the Laplacians for the n-dimensional sphere Sn with the standard metric (see [7, 8, 9, 14, 15, 17, 18, 19, 23, 24, 25, 26]). Recently, Lima [16, Eq. (29)] posed an interesting experimental conjecture on closed-form evaluation of series involving the Zeta functions which is recalled here, in a slightly modified form, as follows:

∞ ζ(2k) 1 ∑ = (lnπ − H − ) ( ) · 2k · ( − ) 2n 1 k=1 2k 2n 2 2 2n 1 ! n−1 (1.8) + ζ(2 j + 1) + ∑ (−1) j 1 (n ∈ N), π2 j · ( − − ) j=1 2 2n 1 2 j ! where N denotes the set of positive integers, Hn denotes the harmonic numbers defined by n 1 Hn := ∑ (n ∈ N) and H0 := 0, (1.9) k=1 k and the Pochhammer symbol (λ)n is defined (for λ ∈ C)by 1 (n = 0) (λ)n := (1.10) λ(λ + 1)···(λ + n − 1)(n ∈ N), AN EXPERIMENTAL CONJECTURE ON SERIES ASSOCIATED WITH THE ZETA FUNCTIONS 973

C being the set of complex numbers. Here, and in what follows, an empty sum is understood (as usual) to be nil. Here, in our present sequel to Lima’s work, we aim at verifying correctness of Lima’s conjecture (1.8) and presenting several general analogues of Lima’s conjecture (1.8), by mainly using a known formula for the series associated with the Zeta functions (see [23, p. 149, Theorem 3.1], also see [11]). For this purpose, we begin by recalling the Hurwitz (or generalized) Zeta function ζ(s,a) defined by ∞ ζ( , ) = ( + )−s (ℜ( ) > ∈ C \ Z−), s a : ∑ k a s 1; a 0 (1.11) k=0 Z− where 0 denotes the set of nonpositive integers. It is noted that the Riemann Zeta function ζ(s) and the Hurwitz (or generalized) Zeta function ζ(s,a) can be continued meromorphically to the whole complex s-plane having simple poles only at s = 1 with their respective residues 1 at this point. For their easy use in the next section, we summarize some known formulas as the following lemmas (see, for details, [23, 24]).

LEMMA 1. The following formulas hold true: − 1 ζ(s,1)=ζ(s); ζ(s,1 + a)=ζ(s,a) − a s; ζ s, =(2s − 1) ζ(s); 2 ⎧ 1 ⎨⎪ − (n = 0) ζ(−2n)=0 (n ∈ N); ζ(−n)= 2 ⎩⎪ Bn+1 − (n ∈ N), n + 1 where Bn denotes the Bernoulli number of order n defined by the following generating function: ∞ n z = z (| | < π) z ∑ Bn z 2 ; e − 1 = n! ⎧ n 0 ⎪ 1 ⎨⎪ − ln(2π)(n = 0),  2 ζ (−2n)= ⎪ (2n)! ⎩⎪(−1)n ζ(2n + 1)(n ∈ N); 2(2π)2n the Psi (or Digamma) function ψ(z) is defined by Γ(z) ψ(z) := and ψ(1)=−γ, Γ(z) where Γ is the familiar Gamma function and γ denotes the Euler-Mascheroni constant defined by n 1 γ := lim ∑ − log n =∼ 0.577215664901532860606512···. n→∞ k=1 k 974 JUNESANG CHOI AND HARI M. SRIVASTAVA

LEMMA 2. (see Adamchik [1, p. 198, Eq. (20)] and Bendersky [6, pp. 273–275]). The set of constants Dk are defined by n k logDk := lim ∑ m logm − p(n,k) (k ∈ N0 := N ∪{0}) n→∞ m=1 with p(n,k) given as follows: k k+1 ( , ) =n + n − 1 p n k : logn + logn + 2 k 1 k 1 k k− j j + n B j+1 + − δ 1 , k! ∑ ( + ) ( − ) logn 1 kj ∑ − + j=1 j 1 ! k j ! =1 k 1 where δkj is the Kronecker symbol. Furthermore, the following relationship holds true:

B + H  log D = k 1 k − ζ (−k)(k ∈ N ). k k + 1 0

2. Closed-form evaluation of series involving the Zeta functions

We first verify the correctness of Lima’s conjecture (1.8) and then present several general analogues of Lima’s conjecture (1.8). For this purpose, we begin by recalling a known formula for the series associated the Zeta functions (see [23, p. 149, Theorem 3.1]; see also [11]), which is asserted by the following theorem.

THEOREM 1. For every nonnegative integer n,

∞ n ζ(k, a) + (−1)   ∑ tn k = [ζ (−n, a −t) − ζ (−n, a)] = (k)n+1 n! k 2 n (− )n+k 1 n  k + ∑ (Hn − Hn−k) ζ(k − n, a) − ζ (k − n, a) t k=1 n! k tn+1 +[H + ψ(a)] (|t| < |a|; n ∈ N ), n (n + 1)! 0 (2.1) where  ∂ ζ (s,a)= ζ(s,a). ∂s Substituting −t for t in (2.1), and considering the cases when n = 2m−1 (m ∈ N) and n = 2m (m ∈ N), and adding and subtracting the resulting identities, we obtain four general closed-form expressions for certain series involving the Zeta functions as in the following theorem. AN EXPERIMENTAL CONJECTURE ON SERIES ASSOCIATED WITH THE ZETA FUNCTIONS 975

THEOREM 2. Each of the following formulas holds true.

∞ ζ(2k + 1, a) + 1 ∑ t2m 2k = − (2k + 1) 2 · (2m − 1)! k=1 2m    · ζ (−2m + 1,a −t)+ζ (−2m + 1,a +t) − 2ζ (−2m + 1,a) 1 m−1 2m − 1 − ∑ (2.2) (2m − 1)! 2k k=1  2k · (H2m−1 − H2m−1−2k) ζ(2k − 2m + 1,a) − ζ (2k − 2m + 1,a) t t2m +[H − + ψ(a)] (|t| < |a|; m ∈ N); 2m 1 (2m)!

∞ ζ(2k,a) − + 1   ∑ t2m 1 2k = ζ (−2m+1,a+t) − ζ (−2m+1,a−t) (2k) 2 · (2m−1)! k=1 2m 1 m 2m − 1 + ∑ (2.3) (2m − 1)! 2k − 1 k=1  2k−1 · (H2m−1 − H2m−2k) ζ(2k − 2m,a) − ζ (2k − 2m,a) t (|t| < |a|; m ∈ N);

∞ ζ(2k,a) + 1    ∑ t2m 2k = ζ (−2m,a−t)+ζ (−2m,a+t)−2ζ (−2m,a) (2k) + 2 · (2m)! k=1 2m 1 1 m 2m + ∑ (2.4) (2m)! 2k k=1  2k · (H2m − H2m−2k) ζ(2k − 2m,a) − ζ (2k − 2m,a) t (|t| < |a|; m ∈ N);

∞ ζ(2k + 1, a) + + 1   ∑ t2m 2k 1 = ζ (−2m,a −t) − ζ (−2m,a +t) (2k + 1) + 2 · (2m)! k=1 2m 1 m − 1 2m ( ) ∑ − 2m ! = 2k 1 (2.5) k 1  2k−1 · (H2m − H2m−2k+1) ζ(2k − 1 − 2m,a) − ζ (2k − 1 − 2m,a) t t2m+1 +[H + ψ(a)] (|t| < |a|; m ∈ N). 2m (2m + 1)!

Setting a = 1 in (2.2) to (2.5) and using suitable identities given in Lemma 1, we get the following four closed-form expressions for some series involving the Zeta functions. 976 JUNESANG CHOI AND HARI M. SRIVASTAVA

COROLLARY 1. Each of the following formulas holds true.

∞ ζ(2k + 1) + 1 ∑ t2m 2k = − (2k + 1) 2 · (2m − 1)! k=1 2m    · ζ (−2m + 1,1 −t)+ζ (−2m + 1,1 +t) − 2ζ (−2m + 1) m−1 − + 1 ∑ 2m 1 (2m − 1)! 2k (2.6) k=1 B2(m−k)  2k · (H − − H − − )+ζ (2k − 2m + 1) t 2(m − k) 2m 1 2m 1 2k t2m +(H − − γ) (|t| < 1; m ∈ N); 2m 1 (2m)!

∞ ζ(2k) − + 1 ∑ t2m 1 2k = (2k)2m 2 · (2m − 1)! k=1   2m−1 · ζ (−2m + 1,1 +t) − ζ (−2m + 1,1 −t)+{ln(2π) − H2m−1} t (2.7) m−1 j+1 1 (−1) ζ(2 j + 1) − − + ∑ t2m 2 j 1 (|t| < 1; m ∈ N); ( − − ) ( π)2 j 2 j=1 2m 2 j 1 ! 2

∞ ζ( ) ζ( + ) 2k 2m+2k =(− )m+1 2m 1 + 1 ∑ t 1 2m (2k)2m+1 2(2π) 2 · (2m)! k=1   2m · ζ (−2m,1 +t)+ζ (−2m,1 −t)+{ln(2π) − H2m} t (2.8) m−1 j+1 1 (−1) ζ(2 j + 1) − + ∑ t2m 2 j (|t| < 1; m ∈ N); ( − ) ( π)2 j 2 j=1 2m 2 j ! 2

∞ ζ(2k + 1) + + 1   ∑ t2m 2k 1 = ζ (−2m,1 −t) − ζ (−2m,1 +t) (2k + 1) + 2 · (2m)! k=1 2m 1 m + 1 ∑ 2m (2m)! 2k − 1 k=1 (2.9) B2(m−k+1)  2k−1 · (H − H − + )+ζ (2k − 1 − 2m) t 2(m − k + 1) 2m 2m 2k 1 t2m+1 +(H − γ) (|t| < 1; m ∈ N). 2m (2m + 1)!

= 1 Setting t 2 in (2.6) to (2.9) and using suitable identities given in Lemma 1 and Lemma 2, we find the following more explicit closed-form expressions for several series involving the Zeta functions. AN EXPERIMENTAL CONJECTURE ON SERIES ASSOCIATED WITH THE ZETA FUNCTIONS 977

COROLLARY 2. Each of the following formulas holds true. ∞ ζ( + ) ∑ 2k 1 = 1 (2k + 1) · 22k (2m − 1)! k=1 2m B2m 2m B2m H2m−1 · 1 + ln2 + 2 2 − 1 − lnD − m 2m 2m 1 (2.10) m−1 − + 1 ∑ 2m 1 (2m − 1)! 2k k=1 − γ B2(m−k) 2m−2k H2m−1 · H − − lnD − − 2 + (m ∈ N); 2(m − k) 2m 1 2m 2k 1 (2m)! ∞ ζ(2k) 1 ∑ = (lnπ − H − ) ( ) · 2k · ( − ) 2m 1 k=1 2k 2m 2 2 2m 1 ! (2.11) 1 m−1 (−1) j+1 ζ(2 j + 1) + ∑ (m ∈ N); ( − − ) π2 j 2 j=1 2m 2 j 1 ! ∞ ζ(2k) 1 1 ζ(2m+1) ∑ = [ln(2π)−H ]+(−1)m −1 ( ) · 2k · ( ) 2m 2m+1 π2m k=1 2k 2m+1 2 2 2m ! 2 (2.12) 1 m−1 (−1) j+1 ζ(2 j + 1) + ∑ (m ∈ N); ( − ) π2 j 2 j=1 2m 2 j ! ∞ ζ( + ) − γ m 2k 1 = ln2 + H2m + 1 2m ∑ 2k ∑ = (2k + 1)2m+1 · 2 (2m)! (2m + 1)! (2m)! = 2k − 1 k 1 k 1 (2.13) B2(m−k+1) 2m−2k+2 · H − lnD − + 2 (m ∈ N). 2(m − k + 1) 2m 2m 2k 1 We now further specialize our results (2.10) to (2.13) only in the case when m = 1 (see also [23, p. 128, Problem 3]).

COROLLARY 3. Each of the following formulas holds true. ∞ ζ(2k + 1) 7 ∑ = 2 − γ + ln2 − 12 lnA, (2.14) ( + )( + ) · 2k k=1 k 1 2k 1 2 3 where A is the Glaisher-Kinkelin constant defined by n n2 n 1 n2 lnA = lim ∑ k ln k − + + lnn + , (2.15) n→∞ k=1 2 2 12 4 the numerical value of A being given by A =∼ 1.282427130··· and D1 = A. ∞ ζ(2k) ∑ = lnπ − 1. (2.16) ( + ) · 2k k=1 k 2k 1 2 978 JUNESANG CHOI AND HARI M. SRIVASTAVA

∞ ζ(2k) 3 7ζ(3) ∑ = − + ln(2π)+ . (2.17) ( + )( + ) · 2k π2 k=1 k k 1 2k 1 2 2 2 ∞ ζ(2k + 1) 3 γ ∑ = − + ln2 − 8lnA. (2.18) ( + )( + )( + ) · 2k k=1 k 1 2k 1 2k 3 2 2 3

3. Concluding remarks and observations

We conclude this paper by giving the following comments and observations.

1. Equations (2.14), (2.16), and (2.18) are known identities recorded, for example, in [23, p. 223, Eq. (546)], [23, p. 223, Eq. (545)], and [23, p. 229, Eq. (581)], respectively.

2. Equation (2.17) can be verified by using such known formulas as, for example, [23, p. 162, Eq. (26)], [23, p. 212, Eq. (467)], [23, p. 217, Eq. (506)], and [23,p. 100, Eq. (29)].

3. The Glaisher-Kinkelin constant in (2.15) is a constant naturally arising in the theory of the multiple Gamma functions (see, for more general set of constants, [12]).

4. Equation (2.11) verifies the above-asserted correctness of the Lima’s experimen- tal conjecture (1.8) [16, Eq. (29)].

Many other interesting corollaries and consequences of our main results asserted by Theorems 1 and 2 (and Corollaries 1, 2 and 3) can be deduced in an analogous manner.

Acknowledgement. The first-named author was supported by the Basic Science Research Program through the National Research Foundation of Korea funded by the Ministry of Edu- cation, Science and Technology (2010-0011005). The second-named author was sup- ported, in part, by the Natural Sciences and Engineering Research Council of Canada under Grant OGP0007353.

REFERENCES

[1] V.S.ADAMCHIK, Polygamma functions of negative order, J. Comput. Appl. Math. 100 (1998), 191– 199. [2] E.W.BARNES, The theory of the G-function, Quart. J. Math. 31 (1899), 264–314. [3] E. W. BARNES, The genesis of the double Gamma function, Proc. London Math. Soc. (Ser. 1) 31 (1900), 358–381. [4]E.W.BARNES, The theory of the double Gamma function, Philos. Trans. Roy. Soc. London Ser. A 196 (1901), 265–388. [5]E.W.BARNES, On the theory of the multiple Gamma functions, Trans. Cambridge Philos. Soc. 19 (1904), 374–439. [6] L. BENDERSKY, Sur la fonction Gamma g´en´eralis´ee, Acta Math. 61 (1933), 263–322. AN EXPERIMENTAL CONJECTURE ON SERIES ASSOCIATED WITH THE ZETA FUNCTIONS 979

[7] J. CHOI, Determinant of Laplacian on S3 , Math. Japon. 40 (1994), 155–166. [8] J. CHOI,Y.J.CHO AND H. M. SRIVASTAVA, Series involving the Zeta function and multiple Gamma functions, Appl. Math. Comput. 159 (2004), 509–537. [9] J. CHOI AND H. M. SR I VA S TAVA,An application of the theory of the double Gamma function, Kyushu J. Math. 53 (1999), 209–222. [10] J. CHOI AND H. M. SRIVASTAVA, Certain classes of series associated with the Zeta function and multiple Gamma functions, J. Comput. Appl. Math. 118 (2000), 87–109. [11] J. CHOI AND H. M. SR I VA S TAVA, A certain family of series associated with the Zeta and related functions, Hiroshima Math. J. 32 (2002), 417–429. [12] J. CHOI AND H. M. SR I VA S TAVA, A family of log-Gamma integrals and associated results,J.Math. Anal. Appl. 303 (2005), 436–449. [13] J. CHOI AND H. M. SR I VA S TAVA, Certain families of series associated with the Hurwitz-, Appl. Math. Comput. 170 (2005), 399–409. [14] E. D’HOKER AND D. H. PHONG, On determinant of Laplacians on Riemann surface, Comm. Math. Phys. 104 (1986), 537–545. [15] H. KUMAGAI, The determinant of the Laplacian on the n-sphere, Acta Arith. 91 (1999), 199–208. [16] F. M. S. LIMA, An Euler-type formula for β(2n) and closed-form expressions for a class of zeta series, Integral Transforms Spec. Funct. 23 (2012), 649–657. [17] B. OSGOOD,R.PHILLIPS AND P. S ARNAK, Extremals of determinants of Laplacians, J. Funct. Anal. 80 (1988), 148–211. [18] J. R. QUINE AND J. CHOI, Zeta regularized products and functional determinants on spheres,Rocky Mountain J. Math. 26 (1996), 719–729. [19] P. SARNAK, Determinants of Laplacians, Comm. Math. Phys. 110 (1987), 113–120. [20] J. D. SHALLIT AND K. ZIKAN, A theorem of Goldbach, Amer. Math. Monthly 93 (1986), 402–403. [21] H. M. SR I VA S TAVA, A unified presentation of certain classes of series of the Riemann Zeta function, Riv. Mat. Univ. Parma (Ser. 4) 14 (1988), 1–23. [22] H. M. SR I VA S TAVA, Sums of certain series of the Riemann Zeta function, J. Math. Anal. Appl. 134 (1988), 129–140. [23] H. M. SR I VA S TAVA A N D J. CHOI, Series Associated with the Zeta and Related Functions,Kluwer Academic Publishers, Dordrecht, Boston and London, 2001. [24] H. M. SR I VA S TAVA A N D J. CHOI, Zeta and q-Zeta Functions and Associated Series and Integrals, Elsevier Science Publishers, Amsterdam, London and New York, 2012. [25] I. VARDI, Determinants of Laplacians and multiple Gamma functions, SIAM J. Math. Anal. 19 (1988), 493–507. [26] A. VOROS, Special functions, spectral functions and the Selberg Zeta function, Comm. Math. Phys. 110 (1987), 439–465.

(Received September 3, 2012) J. Choi Department of Mathematics Dongguk University Gyeongju, Korea e-mail: [email protected] H. M. Srivastava Department of Mathematics and Statistics University of Victoria Victoria, British Columbia V8W 3R4 Canada e-mail: [email protected]

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