Continued fraction expansions of the generating functions of Bernoulli and related numbers

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Abstract

We give continued fraction expansions of the generating functions of Bernoulli numbers, Cauchy numbers, Euler numbers, harmonic numbers, and their generalized or related numbers. In particular, we focus on explicit forms of the convergents of these continued fraction expansions. Linear fractional transformations of such continued fractions are also discussed. We show more continued fraction expansions for different numbers and types, in particular, on Cauchy numbers.

Section snippets

Continued fractions

Given an analytic function f(x), several types of general continued fractions have been known and studied. J.H. Lambert expanded log(1x), arctanx and tanx in continued fractions in 1768. Some special types are known as J-fractions, C-fractions, T-fractions, M-fractions and Hankel continued fractions (see, e.g., [7], [9], [16], [19]). Lando [14] discusses other similar continued fractions from the aspect of Combinatorics and generating functions. Loya [15, Chapter 8] exhibits intriguing ideas

Bernoulli numbers

Bernoulli numbers Bn are defined by n=1Bnxnn!.Many kinds of continued fraction expansions of the generating functions of Bernoulli numbers have been known and studied (see, e.g., [1, Appendix],[6]). However, those of generalized Bernoulli numbers seem to be few, though there exist several generalizations of the original Bernoulli numbers. In particular, direct generalizations from the continued fraction expansions seem to be hard.

Hypergeometric degenerate Bernoulli numbers βN,n(λ) are defined

Cauchy numbers

Cauchy numbers are defined by xlog(1+x)=n=0cnxnn!.Note that these numbers are also called Gregory coefficients, reciprocal logarithmic numbers, Bernoulli numbers of the second kind, or Cauchy numbers of the first kind. In [4], new identities are found by using the continued fraction

(see, e.g., [19, (90.1)]). In this section, we find a different type of continued fraction expansion related to Cauchy numbers.

Define the hypergeometric degenerate Cauchy numbers γN,n(λ) by the generating

Euler numbers

Hypergeometric Euler numbers EN,n [13] are defined by 11F2(1;N+1,(2N+1)2;x24)=n=0EN,nxnn!,where 1F2(a;b,c;z) is the hypergeometric function defined by 1F2(a;b,c;z)=n=0(a)(n)(b)(n)(c)(n)znn!.When N=0, then En=E0,n are the classical Euler numbers, defined by 1coshx=n=0Enxnn!.Since by (9) 1F2(1;N+1,(2N+1)2;x24)=n=0(2N)!x2n(2N+2n)!,consider the convergents Pm(x)Qm(x) with Pm(x)=(2N+2m)!(2N)!andQm(x)=(2N+2m)!n=0mx2n(2N+2n)!.Now, P0(x)Q0(x)=11=1,P1(x)Q1(x)=(2N+1)(2N+2)(2N+1)(2N+2)+x2=1x

Harmonic numbers

There are several generalizations of harmonic numbers Hn, defined by Hn=k=1n1k(n1)withH0=0.In [20], the generalized harmonic numbers of order m (m1) are defined by hn(m)(a,b)=k=1n1((k1)a+b)m(n1)withh0(m)(a,b)=0,where a and b are positive real numbers. When a=b=1, Hn(m)=hn(m)(1,1) are the m-order harmonic numbers. When m=a=b=1, Hn=hn(1)(1,1) are the original harmonic numbers.

Let (x|r)(n)=x(x+r)(x+2r)(x+(n1)r) (n1) be the generalized rising factorial with (x|r)(0)=1. When r=1, (x)(n)=(x

Functions associated with the Riemann zeta function

Let μ(n) be Möbius function. From the property d|nμ(d)=1if n=1,0if n2,the Dirichlet series that generates the Möbius function is the multiplicative inverse of the Riemann zeta function: n=1μ(n)ns=1ζ(s),where s is a complex number with real part larger than 1. Then we consider the convergents Pm(x)Qm(x) as Pm(x)=(m!)s,Qm(x)=(m!)sk=1mxkks(m1).Now,

and Pn(x) and Qn(x) (n3) satisfy the recurrence relations Pn(x)=ns+(n1)sxPn1(x)(n1)2sxPn2(x),Qn(x)=ns+(n1)sxQn1(x)(n1)2sxQn2(x).

Transforms of continued fractions

Raney [18] established a method to yield the simple continued fraction expansions of β(x)=ax+bcx+d with adbc0 from the simple continued fraction expansion

where a0 is an integer and a1,a2, are positive integers. In this section, we shall consider the linear fractional transformation β(x) for the continued fraction expansion in (1). Since the convergents Pn(x)Qn(x) (n0) are given in (2) in our case, we have P̃n(x)Q̃n(x)βPn(x)Qn(x)=g1gn(a+b)+bj=1nh1hjg1gjxjg1gn(c+d)+dj=1nh1hjg1gjx

Continued fractions of the ordinary generating functions

A continued fraction expansion of the ordinary generating function of Bernoulli numbers is given by

([1, A.5]). However, any beautiful continued fraction expansion for Cauchy numbers has not been known yet. Nevertheless, in order to satisfy the approximation property (3), we have the following expansion.

Theorem 8

Concluding remarks

In this paper, we deal with continued fraction in the aspects of convergents. Such techniques and ideas can be applied to more different types. For example, we can have a more complicated continued fraction expansion than that in Corollary 4.

Theorem 9

For N1,

When N=1, this is a direct generalization of the continued fraction expansion

(see, e.g., [19, (90.1)]).

Similarly, the nth convergent and the generating function of cn coincide up to the nth term in their Taylor expansions. However, the structure

Acknowledgment

The author thanks the anonymous referee for his/her detailed comments and suggestions, which improved the quality of the paper.

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