Research article Special Issues

New approach to λ-Stirling numbers

  • The aim of this paper is to study the λ-Stirling numbers of both kinds, which are λ-analogues of Stirling numbers of both kinds. These numbers have nice combinatorial interpretations when λ are positive integers. If λ=1, then the λ-Stirling numbers of both kinds reduce to the Stirling numbers of both kinds. We derive new types of generating functions of the λ-Stirling numbers of both kinds which are related to the reciprocals of the generalized rising factorials. Furthermore, some related identities are also derived from those generating functions. In addition, all the corresponding results to the λ-Stirling numbers of both kinds are obtained for the λ-analogues of r-Stirling numbers of both kinds, which are generalizations of those numbers.

    Citation: Dae San Kim, Hye Kyung Kim, Taekyun Kim. New approach to λ-Stirling numbers[J]. AIMS Mathematics, 2023, 8(12): 28322-28333. doi: 10.3934/math.20231449

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  • The aim of this paper is to study the λ-Stirling numbers of both kinds, which are λ-analogues of Stirling numbers of both kinds. These numbers have nice combinatorial interpretations when λ are positive integers. If λ=1, then the λ-Stirling numbers of both kinds reduce to the Stirling numbers of both kinds. We derive new types of generating functions of the λ-Stirling numbers of both kinds which are related to the reciprocals of the generalized rising factorials. Furthermore, some related identities are also derived from those generating functions. In addition, all the corresponding results to the λ-Stirling numbers of both kinds are obtained for the λ-analogues of r-Stirling numbers of both kinds, which are generalizations of those numbers.



    It is remarkable that explorations for degenerate versions of quite a few special numbers and polynomials, which began with the study of degenerate Bernoulli and degenerate Euler polynomials by Carlitz, have led to the discoveries of many interesting results (see [10,12,13,14,15] and references therein). Specially, the degenerate Stirling numbers of both kinds are degenerate versions of the usual Stirling numbers of both kinds and occur frequently when we study degenerate versions of many special numbers and polynomials. In addition, λ-analogues, which are different from degenerate versions, of some special numbers and polynomials, have also been studied (see [5,6,9,11]). Here, we consider the λ-analogues of Stirling numbers of both kinds.

    The Stirling number of the second kind {nk} enumerates the number of partitions of the set [n]={1,2,,n} into k nonempty disjoint sets, while the unsigned Stirling number of the first kind [nk]=(1)nkS1(n,k) counts the number of permutations of n elements with k disjoint cycles. Here, we consider the λ-analogues of the Stirling numbers of both kinds. The λ-analogues of {nk} are called the λ-Stirling numbers of the second kind and denoted by {nk}λ, while those of [nk] are called the λ-Stirling numbers of the first kind and denoted by [nk]λ. Here, λ is any real number and we note that [nk]1=[nk]and{nk}1={nk}. Now, let λ be any positive integer, then it is possible to give combinatorial interpretations of {nk}λ and [nk]λ. Indeed, {nk}λ, called the translated Whitney numbers of the second kind [2,16], enumerates the number of partitions of the set [n] into k subsets such that each element of each subset can mutate in λ ways, except the dominant one. Meanwhile, [nk]λ, called the translated Whitney numbers of the first kind [2,16], counts the number of permutations of n elements with k cycles, such that the element of each cycle can mutate in λ ways except the dominant one. We also consider generalizations of the λ-Stirling numbers of both kinds, namely the λ-analogues of r-Stirling numbers of the second kind {n+rk+r}r,λ and those of (unsigned) r-Stirling numbers of the first kind [n+rk+r]r,λ. Here, we note that {nk}0,λ={nk}λ and [nk]0,λ=[nk]λ.

    The aim of this paper is to derive new types of generating functions of the λ-Stirling numbers of both kinds (see Theorem 3, Corollary 4, Remark 5). We note that the new type of generating function of the λ-Stirling numbers of the second kind is equivalent to the ordinary generating function of those numbers (see Theorem 3, Remark 5). The generating function of the λ-Stirling numbers of the first kind follows from that of the second kind by inversion (see Corollary 4). In Theorem 6, we find expressions of the integral over (a,) of the reciprocals of the generalized rising factorials as finite sums by using an identity in (2.5), and the fact that the limit as b tends to of a certain finite sum is zero (see (2.13)). Also, we derive an expression of 1kak as an infinite sum by integrating the generating function of the λ-Stirling numbers of the second kind in Corollary 4. In section three, we derive the corresponding results to those in section two for the λ-analogues of r-Stirling numbers of both kinds by using similar methods. We are indebted to [3] for many ideas in this paper.

    The outline of this paper is as follows. We first recall the generalized falling factorial sequence, the Stirling numbers of the first kind, the Stirling numbers of the second kind and the unsigned Stirling numbers of the first kind. We remind the reader of the λ-Stirling numbers of the first kind, the λ-Stirling numbers of the second kind and the unsigned λ-Stirling numbers of the first kind. We recall the λ-analogues of (unsigned) r-Stirling numbers of the first kind and the λ-analogues of r-Stirling numbers of the second kind as well as an explicit expression of the λ-analogues of r-Stirling numbers of the second kind and the λ-analogues of binomial coefficients. Then we remind the reader of orthogonality and inverse relations for the λ-analogues of r-Stirling numbers. Section two is the main result of this paper. In Theorem 3, we obtain an expression of the reciprocal of the generalized rising factorial as an infinite series involving the λ-Stirling numbers of the second kind, which is equivalent to the ordinary generating function of those numbers. It is noted in Corollary 4 that we get, by inversion, a generating function of the unsigned λ-Stirling numbers of the first kind in terms of the reciprocals of the generalized rising factorials. By applying a Frullani's integral in (2.10), we show that the limit b tending to of a certain finite sum is equal to zero (see (2.13)). By using this fact and an expression of the reciprocals of the generalized rising factorials in (2.5), we get explicit expressions as finite sums of the integral of those reciprocals over (a,) in Theorem 6 and those as infinite sums of 1kak in Corollary 7. In section three, all the results in section two are extended to the λ-analogues of r-Stirling numbers and similar results to those in section two are obtained. In the rest of this section, we recall the necessary facts that will be used throughout this paper.

    For any λR, the generalized falling factorial sequence is defined by

    (x)0,λ=1, (x)n,λ=x(xλ)(x2λ)  (x(n1)λ),(n1). (1.1)

    For n0, it is known that the Stirling numbers of the first kind are defined by

    (x)n=nk=0S1(n,l)xl, (1.2)

    see [2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,18].

    As the inversion formula of (1.2), the Stirling numbers of the second kind are defined by

    xn=nk=0{nk}(x)k,(n0), (1.3)

    see [2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,18,19,20].

    The unsigned Stirling numbers of the first kind are defined by [nk]=(1)nkS1(n,k),(n,k0). In [9,11], the λ-Stirling numbers of the first kind are given by

    (x)n,λ=nk=0S1,λ(n,k)xk,  (n0). (1.4)

    The unsigned λ-Stirling numbers of the first kind are defined by

    <x>n,λ=(1)n(x)n,λ=nk=0[nk]λxk, (1.5)

    where the generalized rising factorial sequence is given by

    <x>0,λ=1, <x>n,λ=x(x+λ)  (x+(n1)λ),(n1). (1.6)

    From (1.4) and (1.5), we note that [nk]λ=(1)nkS1,λ(n,k).

    The λ-Stirling numbers of the second kind are defined by

    xn=nk=0{nk}λ(x)k,λ,(n0),  [9,11]. (1.7)

    For rN{0}, the λ-analogues of (unsigned) r-Stirling numbers of the first kind are defined by

    <x+r>n,λ=nk=0[n+rk+r]r,λxk,  [9,11], (1.8)

    where we note that [nk]0,λ=[nk]λ, for r=0, (see (1.5), (1.8)).

    Thus, by (1.8), we get

    (x)n,λ=nk=0(1)nk[n+rk+r]r,λ(x+r)k,(n0). (1.9)

    The λ-analogues of r-Stirling numbers of the second kind are defined by

    (x+r)n=nk=0{n+rk+r}r,λ(x)k,λ,(n0),  [9,11]. (1.10)

    Note that

    {n+rk+r}r,λ=1λk1k!kl=0(kl)(1)kl(lλ+r)n. (1.11)

    This follows easily from Theorem 1 [9]. As a special case of (1.11), we observe that

    {nk}λ={nk}0,λ=1k!kl=0(kl)(1)klλnkln,see(1.7)and(1.10). (1.12)

    For n0, the λ-analogues of binomial coefficients are defined by

    (xn)λ=(x)n,λn!=x(xλ)  (x(n1)λ))n!, [15]. (1.13)

    We are going to use the next theorem and its corollary several times in the sequel. Both (a) and (b) follow from (1.9) and (1.10), while (c)–(e) can be derived from (a) and (b).

    Theorem 1. The λ-analogues of r-Stirling numbers enjoy the following orthogonality and inverse relations:

    (a)nk=l(1)nk[n+rk+r]r,λ{k+rl+r}r,λ=δn,l,(b)nk=l(1)kl[k+rl+r]r,λ{n+rk+r}r,λ=δn,l,(c)an=nk=0{n+rk+r}r,λckcn=nk=0(1)nk[n+rk+r]r,λak,(d)an=mk=n{k+rn+r}r,λckcn=mk=n(1)kn[k+rn+r]r,λak,(e)an=k=n{k+rn+r}r,λckcn=k=n(1)kn[k+rn+r]r,λak.

    In the special case of r=0, we obtain the next orthogonality and inverse relations for the λ-Stirling numbers.

    Corollary 2. The λ-Stirling numbers enjoy the following orthogonality and inverse relations:

    (a)nk=l(1)nk[nk]λ{kl}λ=δn,l,(b)nk=l(1)kl[kl]λ{nk}λ=δn,l,(c)an=nk=0{nk}λckcn=nk=0(1)nk[nk]λak,(d)an=mk=n{kn}λckcn=mk=n(1)kn[kn]λak,(e)an=k=n{kn}λckcn=k=n(1)kn[kn]λak.

    Let

    1x(x+λ)(x+2λ)  (x+kλ)=kl=0Al,λx+lλ. (2.1)

    Then, for 0mk, we have

    limxmλ(x+mλ)1x(x+λ)(x+2λ)  (x+kλ)=limxmλ(x+mλ)kl=0Al,λx+lλ=Am,λ. (2.2)

    On the other hand, by (2.2), we get

    limxmλx+mλx(x+λ)  (x+(m1)λ)(x+mλ)(x+(m+1)λ)  (x+kλ)=1(mλ)(m+1)λ  (λ)  λ  2λ  (km)λ=(1)mλmm!λkm(km)!=(1)mλk1k!(km). (2.3)

    From (2.2) and (2.3), we note that

    Am,λ=1λk(1)mk!(km). (2.4)

    By (2.1) and (2.4), we get

    1x(x+λ)  (x+kλ)=kl=01λk(1)lk!(kl)1x+lλ=λkk!kl=0(1)l(kl)n=0(1)nlnλn(1x)n+1=n=0((1)nk!kl=0(1)l(kl)λnkln)(1x)n+1=n=0(1)nkk!(kl=0(1)kl(kl)λnkln)(1x)n+1=n=k(1)nk{nk}λ(1x)n+1, (2.5)

    where we used (1.12).

    Therefore, by (2.5), we obtain the following theorem.

    Theorem 3. For k0, we have

    1x(x+λ)  (x+kλ)=n=k(1)nk{nk}λ(1x)n+1. (2.6)

    Then, from Corollary 2 (e), we obtain the following result, which is the generating function of the unsigned λ-Stirling numbers of the first kind in terms of the inverses of the generalized rising factorials.

    Corollary 4. For k0, we have

    (1x)k+1=n=k(1)nkS1,λ(n,k)1x(x+λ)  (x+nλ)=n=k[nk]λ1x(x+λ)  (x+nλ). (2.7)

    Remark 5. It is immediate to see that (2.6) is equivalent to the ordinary generating function of the λ-Stirling numbers of the second kind given by

    xk(1λx)(12λx)(1kλx)=n=k{nk}λxn.

    On the other hand, the exponential generating function of the λ-Stirling numbers of the second kind is shown in Eq (11) of [9] to be equal to

    1λk1k!(eλt1)k=n=k{nk}λtnn!.

    Let f be a nonnegative real valued function that has value at , which is denoted by f().

    Then, for a,b>0, we have

    0f(ax)f(bx)xdx=0abtf(xt)dtdx=ab0tf(xt)dxdt=abf()f(0)tdt=(f()f(0))logab. (2.8)

    The integral in (2.8) is the Frullani's integral, and its evaluation in (2.9) was first published by Cauchy in 1823. The Eq (2.8) is valid for 'nice' functions f [1,4,17].

    Thus, by (2.8), we get

    0f(ax)f(bx)xdx=(f()f(0))logab,   [4]. (2.9)

    Let us take f(x)=ex and a=1, then we have

    0exebxxdx=log1b=logb,(b>0). (2.10)

    Let k be any positive integer, and let b,λ>0. Then, from (2.10), we note that

    kl=0(kl)(1)llog(b+lλ)=kl=0(kl)(1)l0exe(b+lλ)xxdx=0{kl=0(kl)(1)lexxkl=0(kl)(1)le(b+lλ)xx}dx=0{(11)kexxkl=0(kl)(1)le(b+lλ)xx}dx=0ebxxkl=0(kl)(1)lelλxdx=0ebxx(1eλx)kdx. (2.11)

    As (1eλx)kx is bounded on [0,), say by M, we have

    |0ebxx(1eλx)kdx|M0ebxdx=Mb, (2.12)

    and hence the integral 0ebxx(1eλx)kdx is convergent for any b,λ>0 and any positive integer k.

    Moreover, for any positive integer k and any λ>0, by (2.12) we get

    limbkl=0(kl)(1)llog(b+lλ)=limb0ebxx(1eλx)kdx=0. (2.13)

    From (2.13) and (2.5), for any λ,a>0 and any positive integer k, we note that

    a1x(x+λ)  (x+kλ)dx=limbba1x(x+λ)  (x+kλ)dx=λkk!kl=0(kl)(1)llimbba1x+lλdx=λkk!limbkl=0(kl)(1)l(log(b+lλ)log(a+lλ))=λkk!kl=0(kl)(1)l+1log(a+lλ). (2.14)

    Thus, by (2.13), we get the following theorem.

    Theorem 6. For any λ,a>0 and any positive integer k, the following identity holds.

    a1x(x+λ)  (x+kλ)dx=λkk!kl=0(kl)(1)l+1log(a+lλ). (2.15)

    From Corollary 4 and (2.15), for any positive integer k and any λ,a>0, we have

    1kak=a1xk+1dx=n=k[nk]λa1x(x+λ)  (x+nλ)dx=n=k[nk]λ1n!λnnl=0(nl)(1)l+1log(a+lλ). (2.16)

    We state this as a corollary.

    Corollary 7. For any positive integer k and any λ,a>0, the following holds true.

    1kak=n=k[nk]λ1n!λnnl=0(nl)(1)l+1log(a+lλ).

    By Theorem 3, we get

    (1x)k=n=k[nk]λ1(x+λ)(x+2λ)  (x+nλ). (2.17)

    Replacing x by xλ and n by n+1, we get

    (1xλ)k=n=k1[n+1k]λ1x(x+λ)  (x+nλ). (2.18)

    In particular, for k=1, we have

    1xλ=n=0λnn!x(x+λ)  (x+nλ)=n=0λn(x+(n1)λn)λ(x+nλ). (2.19)

    Let

    1(x+r)(x+r+λ)  (x+r+kλ)=kl=0Kl,λx+r+lλ. (3.1)

    For 0mk, we have

    Km,λ=limxrmλkl=0Kl,λx+r+lλ(x+r+mλ)=limxrmλx+r+mλ(x+r)(x+r+λ)  (x+r+kλ)=(1)mλkk!m!(km)!1k!=(1)mλk1k!(km). (3.2)

    By (3.1) and (3.2), we get

    1(x+r)(x+r+λ)  (x+r+kλ)=kl=0(1)lλkk!(kl)1x+r+lλ=1λkk!kl=0(1)l(kl)1x11+r+lλx=n=0(1)n1λkk!kl=0(1)l(kl)(r+lλ)n(1x)n+1=n=0(1)nk(1λk1k!kl=0(1)kl(kl)(r+lλ)n)(1x)n+1=n=k(1)nk{n+rk+r}r,λ(1x)n+1, (3.3)

    where we used (1.11).

    Therefore, by (3.3), we obtain the following theorem.

    Theorem 8. For k0, we have

    1(x+r)(x+r+λ)  (x+r+kλ)=n=k(1)nk{n+rk+r}r,λ(1x)n+1. (3.4)

    Now, from Corollary 2 (e) and using the notation in (1.13), we obtain the following result.

    Corollary 9. For k0, we have

    (1x)k+1=n=k[n+rk+r]r,λ1(x+r)(x+r+λ)  (x+r+nλ)=n=k[n+rk+r]r,λ1n!(x+r+(n1)λn)λ(x+r+nλ).

    Remark 10. The Eq (3.4) is equivalent to the ordinary generating function of the λ-analogues of r-Stirling numbers of the second kind given by

    xk(1rx)(1(r+λ)x)(1(r+kλ)x)=n=k{n+rk+r}r,λxn.

    On the other hand, it is shown in Theorem 1 of [9] that the exponential generating function of the λ-analogues of r-Stirling numbers of the second kind is given by

    1λk1k!(eλt1)kert=n=k{n+rk+r}r,λtnn!,(k0).

    Let k be any positive integer and let λ,a>0. By using (2.13) and (3.3), we obtain

    a1(x+r)(x+r+λ)  (x+r+kλ)dx=1k!1λkkl=0(kl)(1)l+1log(a+r+lλ). (3.5)

    From (3.5) and Corollary 6, we have

    1kak=a1xk+1dx=n=k[n+rk+r]r,λ1n!a1n!(x+r+(n1)λn)λ(x+r+nλ)dx=n=k[n+rk+r]r,λ1n!λnnl=0(nl)(1)l+1log(a+r+lλ). (3.6)

    Thus we have shown the following theorem.

    Theorem 11. For any positive integer k and any λ,a>0, the following hold true.

    a1(x+r)(x+r+λ)  (x+r+kλ)dx=1k!1λkkl=0(kl)(1)l+1log(a+r+lλ),1kak=n=k[n+rk+r]r,λ1n!λnnl=0(nl)(1)l+1log(a+r+lλ).

    We have witnessed that studying both degenerate versions and λ-analogues of some special numbers and polynomials yielded many fascinating results. Here, we note that these two are different in nature. Indeed, the degenerate versions tend to the non-degenerate ones as λ tends to zero, while the λ-analogues as λ tends to one. In this paper, we studied the λ-Stirling numbers of both kinds, which are λ-analogues of the usual Stirling numbers. We derived new types of generating functions for those numbers as well as for the λ-analogues of r-Stirling numbers of both kinds. All of these generating functions are related to reciprocals of the generalized rising factorials. Furthermore, from those new types of generating functions we obtained expressions of the integral over (a,) of the reciprocals of the generalized rising factorials as finite sums and an expression of 1kak as an infinite sum, involving the λ-Stirling numbers of the first kind or the λ-analogues of r-Stirling numbers of the first kind.

    It is one of our future projects to continue to study various λ-analogues of many special numbers and polynomials and to find their applications to physics, science and engineering as well as to mathematics.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    We would like to thank the Jangjeon Institute for Mathematical Sciences for supporting this research. This article was supported by the Basic Science Research Program, the National Research Foundation of Korea, (NRF-2021R1F1A1050151).

    The authors declare that there is no conflict of interest.



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