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23 11

Article 08.1.7

Journal of Integer Sequences, Vol. 11 (2008), 2

3 6 1 47

Some Properties of Associated Stirling Numbers

Feng-Zhen Zhao

Department of Applied Mathematics Dalian University of Technology

Dalian 116024 China

fengzhenzhao@yahoo.com.cn

Abstract

In this paper, we discuss the properties of associated Stirling numbers. By means of the method of coefficients, we establish a series of identities involving associated Stirling numbers, Bernoulli numbers, harmonic numbers, and the Cauchy numbers of the first kind. In addition, we give the asymptotic expansion of certain sums involving 2-associated Stirling numbers of the second kind by Darboux’s method.

1

Introduction

Stirling numbers are generalized by many forms. See for instance [1,2,3,4,5] and [9]. In this paper, we are interested in associated Stirling numbers. The associated Stirling numbers of the first kind s2(n, k) [3] are given by

∞ X

n=k

s2(n, k)t

n

n! =

[ln(1 +t)−t]k

k!

and ther-associated Stirling numbers of the second kind Sr(n, k) [3] are given by

∞ X

n=k

Sr(n, k)

tn

n! = 1

k!

et r−1 X

j=0

tj

j! k

,

where k and r are positive integers. It is clear that

∞ X

n=k

S2(n, k)t

n

n! =

(et1t)k

k! , ∞

X

n=k

S3(n, k)t

n

n! =

(et1tt2/2)k

k! .

(2)

(|N|=n), withk orbits, andSr(n, k) is the number of partitions of the setN (|N|=n), into

k blocks, all of cardinality ≥r. It is clear that S1(n, k) is the Stirling number of the second kindS(n, k). Therefore, associated Stirling numbers deserve to be investigated. The aim of this paper is to investigate the properties of associated Stirling numbers by making use of the method of coefficients [7]. We establish a series of identities relating associated Stirling numbers with Bernoulli, harmonic, and Cauchy numbers of the first kind. In addition, we give the asymptotic expansion of certain sums involving r-associated Stirling numbers by Darboux’s method.

The paper is organized as follows. In Section 2, we establish a series of identities involving associated Stirling, Bernoulli, harmonic and Cauchy numbers of the first kind. In Section 3, we give the asymptotic expansion of certain sums involving r-associated Stirling numbers by Darboux’s method.

For convenience, we recall some definitions of combinatorial numbers involved in the paper. Throughout, we denote Stirling numbers of the first kind bys(n, k), and letBn,Bn(k),

and En stand for Bernoulli, generalized Bernoulli, and Euler numbers respectively. That is,

∞ X

n=k

s(n, k)t

n

n! =

lnk(1 +t)

k! ,

∞ X

n=0

Bn

tn

n! =

t et1,

∞ X

n=0

B(k)

n

tn

n! =

tk

(et1)k (k ≥1),

∞ X

n=0

En

tn

n! = 2

et+e−t.

The Cauchy numbers of the first kind an are given by

∞ X

n=0

an

tn

n! =

t

ln(1 +t).

The harmonic numbers Hn are given by

∞ X

n=1

Hntn =−

ln(1−t) 1−t .

In this paper, [tn]f(t) denotes the coefficient oftn inf(t), where

f(t) = ∞ X

n=0

fntn.

The expression [tn] is called the “coefficient of ” functionals [7]. If f(t) and g(t) are formal

power series, the following relations hold [7]:

[tn](αf(t) +βg(t)) =α[tn]f(t) +β[tn]g(t), (1.1)

[tn]tf(t) = [tn−1]f(t), (1.2) [tn]f′

(t) = (n+ 1)[tn+1]f(t), (1.3)

[tn]f(t)g(t) =

n

X

k=0

([yk]f(y))[tn−k

]g(t). (1.4)

(3)

2

Identities involving associated Stirling, Bernoulli, and

harmonic numbers

(4)

Then (2.1) holds.

Now we give the proof of (2.2).

n

X

j=0

n+k−1

j

S2(n−j+k, k)Bj = (n+k−1)! n

X

j=0

S2(n−j +k, k) (n−j +k−1)!·

Bj

j!

= (n+k−1)!

n

X

j=0

(n−j +k)S2(n−j+k, k) (n−j+k)! ·

Bj

j!

= (n+k−1)!

n

X

j=0

(n−j+k)[tn−j+k](et−1−t)k

k! [t

j] t

et1

= (n+k−1)!

n

X

j=0

[tn−j+k−1](et−1−t)k−1(et−1) (k−1)! [t

j

] t

et1

= (n+k−1)!

n

X

j=0 [tn−j

]k(e

t1t)k−1(et1)

tk−1k! [t

j

] t

et1

= (n+k−1)![tn](e

t1t)k−1

tk−2(k1)!

= (n+k−1)![tn+k−2](et−1−t)k−1 (k−1)! = (n+k−1)S2(n+k−2, k−1).

This completes the proof.

Formula (2.1) relates associated Stirling, Bernoulli, and Stirling numbers of the second kind.

The generating functions of generalized Bernoulli numbers Bn(k) implies that they are

related to associated Stirling numbers. For S2(n, k) and Bn(k), we get

Corollary 2.1. For n≥1 andk≥1, 2-associated Stirling numbersS2(n, k)and generalized

Bernoulli numbers Bn(k) satisfy

n

X

j=0

S2(n−j+k, k)

n+k j

Bj(k) =

n+k k

k

X

j=0

(−1)k−j

k j

B(k−j)

(5)

Proof.

n

X

j=0

S2(n−j +k, k)

n+k j

Bj(k) = (n+k)!

n

X

j=0

S2(n−j +k, k) (n−j+k)! ·

Bj(k) j!

= (n+k)!

n

X

j=0

[tn−j+k](et−1−t)k

k! [t

j] tk

(et1)k

= (n+k)!

k!

n

X

j=0

[tn−j](et−1−t)k

tk [t

j] tk

(et1)k

= (n+k)!

k! [t

n](et−1−t)k

(et1)k

= (n+k)!

k!

k

X

j=0

(−1)k−j

k j

Bn(k−j)

n! .

Hence (2.3) holds.

For S3(n, k) and Bernoulli numbersBn, we have

Theorem 2.2. For n ≥k and k≥1, S3(n, k) and Bn satisfy

n

X

j=0

n+k j+k

S3(j+k, k)Bn−j = (n+k)! k

X

j=1

(−1)k−j

j(k−j)!

k−j

X

j1=0

k−j j1

S(n−j1+j −1, j−1) 2j1(n−j

1+j−1)!

+(−1)

k(n+k)!

k!

k

X

j=0

Bn−j

2j(nj)!

k j

(6)

Proof. From the generating functions of S3(n, k) andBn, we have

Then (2.4) holds.

There are many identities relating Stirling numbers of the first kind and harmonic num-bers in [3]. For example,

(−1)n+1s(n+ 1,2) = n!H

(7)

Theorem 2.3. For n ≥1 and k≥1, we have

Proof. By integrating the generating function forHn we have

One can verify that

[ln(1−t) +t]kln2(1t)

Hence (2.5) holds.

There are some identities involving Stirling numbers and Cauchy numbers of the first kind. For example

n

See [3,6] for more details. For associated Stirling numbers of the first kind and the Cauchy numbers of the first kind, we have

Theorem 2.4. For n ≥1 and k≥1, s2(n, k) and an satisfy

The proof of (2.6) is similar to that of (2.1) and is omitted here.

(8)

3

Asymptotic Expansion of Certain Sums Involving

2

-associated Stirling numbers of the second kind,

Bernoulli numbers, and Euler Numbers

We know that it is difficult to compute the accurate values of certain sums involving r -associated Stirling numbers. However, sometimes we can give their asymptotic expansion. In this section, we give asymptotic expansion of certain sums for 2-associated Stirling numbers of the second kind, Bernoulli numbers, and Euler numbers by Darboux’s method. We first recall a lemma (see [8]):

Lemma: Assume thatf(t) =P

n≥0antn is an analytic function for |t|< rand with a finite

number of algebraic singularities on the circle |t| = r. α1, α2, · · ·, αl are singularities of

order ω, where ω is the highest order of all singularities. Then

an = (nω−1/Γ(ω))×

l

X

k=1

gk(αk)α−kn+ o(r−n)

, (3.1)

where Γ(ω) is the gamma function, and

gk(αk) = lim t→αk

(1−(t/αk))ωf(t).

By using (3.1), we obtain

Theorem 3.1. Suppose that n≥1 and k≥1, where k is fixed. When n → ∞, we have

X

p+q=2n

S2(p+k, k)Bq

(p+k)!q! ∼

2(−1)n+k+1

(2π)2nk! , (3.2)

X

p+q=n

S2(p+k, k)Eq

(p+k)!q! ∼

2n+1[(2 + 2iπ)ki−n+ (22iπ)k(−i)−n]

πn+k+1k! . (3.3)

Proof. Because the proof of (3.3) is similar to that of (3.2), we only prove that (3.2) holds. It is clear that

∞ X

p=0

S2(p+k, k)

tp

(p+k)! ∞ X

q=0

Bq

tq

q! =

(et1t)k

k!tk−1(et1).

Let

f(t) = (e

t1t)k

k!tk−1(et1).

Then f(t) is analytic for|t|<2π and with two algebraic singularities on the circle |t|= 2π.

α1 = 2πiand α2 =−2πiare singularities of order 1. One can compute that

lim

t→2πi

1− t

2πi

f(t) = lim

t→−2πi

1 + t

2πi

f(t)

= (−1)

k+1

(9)

It follows from (3.1) that

X

p+q=n

S2(p+k, k)Bq

(p+k)!q! = 1 Γ(1)

(−1)k+1[(2πi)−n+ (−2πi)−n]

k! + o((2π)

−n)

.

Then we have

X

p+q=2n

S2(p+k, k)Bq

(p+k)!q! ∼

(−1)k+1[i2n+ (−i)2n]

(2π)2nk!

Hence (3.2) holds.

4

Acknowledgments

The author would like to thank the anonymous referee for his criticism and useful suggestions.

References

[1] A. Z. Broder, Ther-Stirling numbers, Discrete Math. 49 (1984), 241–259.

[2] L. Carlitz, On some polynomials of Tricomi, Boll Un. M. Ital.13 (1958), 58–64.

[3] L. Comtet, Advanced Combinatorics, Reidel, 1974.

[4] R. Ehrenborg, Determinants involving q-Stirling numbers, Adv. App. Math. 31 (2003), 630–642.

[5] H. W. Gould, The q-Stirling numbers of the first and second kinds, Duke Math. J. 28

(1961), 281–289.

[6] D. Merlini, R. Sprugnoli, and M. C. Verri, The Cauchy numbers, Discrete Math. 306

(2006), 1906–1920.

[7] D. Merlini, R. Sprugnoli, and M. C. Verri, The method of coefficients, Amer. Math. Monthly 114 (2007), 40–57.

[8] G. Szeg¨o,Orthogonal polynomials, Amer. Math. Soc. Coll. Pub., Vol. 23, rev. ed., 1959.

[9] M. Wachs, D. White,p, q-Stirling numbers and set partion statistics,J. Combin. Theory Ser. A 56 (1990), 27–46.

2000 Mathematics Subject Classification: Primary 05A15; Secondary 05A16, 05A19.

Keywords: Stirling numbers, Bernoulli numbers, harmonic numbers, asymptotic expansion, Darboux’s method.

Received December 8 2007; revised version received May 2 2008. Published in Journal of Integer Sequences, May 6 2008. Minor revisions, June 11 2008, June 20 2008, July 5 2008.

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