Elsevier

Applied Mathematics and Computation

Volume 265, 15 August 2015, Pages 557-567
Applied Mathematics and Computation

Accurate double inequalities for generalized harmonic numbers

https://doi.org/10.1016/j.amc.2015.04.128Get rights and content

Abstract

For nN and pR the nth harmonic number of order p H(n,p):=k=1n1kpis expressed in the form H(n,p)=H˜q(m,n,p)+Rq(m,n,p)where m,qN are parameters controlling the magnitude of the error term. The function H˜q(m,n,p) consists of m+2q+1 simple summands and the remainder Rq(m, n, p) is estimated, for p ≥ 0, as 0(1)q+1Rq(m,n,p)<1π(12·4q)(p2+q1)πm)2q1·1mp.Similar result is obtained also for p < 0 and for real zeta function (n=, p > 1) as well.

Introduction

The infinite convergent p-series, noted as Riemann zeta function, is well known, at least from the numerical stand point. However, the finite p-series, known also as the (generalized) nth harmonic number of order p, was studied less intensively. Only a few of authors, Abalo [1] and Hansheng [5], for example, have estimated this series. Recently, Chlebus [3] published the paper approximating the sequence of partial sums H(n,p):=k=1n1kp,pR.Using the probability techniques, Chlebus [3, rel. (33), (25, (26))] derived the following estimates: C1(n,p):=1+n1p11p<H(n,p)<1+(n+1)1p11p=:C2(n,p)for p < 0, C1+(n,p):=(n+1)1p11p<H(n,p)<1+n1p11p=:C2+(n,p)for p > 0, p ≠ 1, ln(n+1)<H(n,1)<1+ln(n).

Our aim is to present more accurate approximations to harmonic numbers of order p than those given above. Indeed, we will improve the estimates (2)–(4), see Figs. 4 and 5, using the Euler–Maclaurin summation formula, the subject of the next section (see [4]).

Section snippets

Euler–Maclaurin summation formula

The sequence of Bernoulli polynomials Bn(x) is unambiguously defined inductively as (i)B0(x)=1,forxR(ii)Bn(x)=nBn1(x),fornNandxR(iii)01Bn(x)dx=0,fornN.This way, for example, we obtain B1(x)x1/2,B2(x)x2x+1/6,B3(x)x33x2/2+x/2 and B4(x)x42x3+x21/30.

The sequences of weighted Bernoulli polynomials Vn(x) and weighted Bernoulli 1-periodic functions Wn(x) are defined inductively as follows: (i)V0(x)=1,forxR,(ii)Vn(x)=Vn1(x),fornNandxR,(iii)Vn(0):=Vn(1),fornN{1},and (iv)W0(x)=1forx

Approximating the p-series

For xR and kN0, the upper (rising) Pochhammer [7] product x(k) is defined as x(0):=1andx(k):=i=0k1(x+i)=x(x+1)··(x+k1)(kN).

For pR,qN and xR+ we define the auxiliary sums σ1(x,p):=0andσq(x,p)=i=1q1B2i·p(2i1)xp+2i1·(2i)!(qN{1}).

The approximation of the nth harmonic number (1) is given in the following two theorems where the parameters m and q control the error Rq(m, n, p).

Theorem 1

Bounding harmonic numbers Hn

For positive integers m, n and q, where m < n, we have Hn:=H(n,1)=Aq(m,1)+Bq(n,1)+Rq(m,n,1),where4

References (10)

  • R.L. Graham et al.

    Concrete Mathematics

    A foundation for computer science, Advanced Book Program

    (1989)
  • E.K. Abalo et al.

    Convergence of p-series revisited with applications

    Int. J. Math. Math. Sci.

    (2006)
  • M. Abramowitz et al.

    Handbook of Mathematical Functions

    (1972)
  • E. Chlebus

    An approximate formula for a partial sum of the divergent p-series

    Appl. Math. Lett.

    (2009)
  • Y. Hansheng et al.

    Another proof for the p-series test

    College Math. J.

    (2005)
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