Abstract
Recently, extended r-central factorial numbers of the second kind and extended r-central Bell polynomials were introduced and various results of them were investigated. The purpose of this paper is to further derive properties, recurrence relations and identities related to these numbers and polynomials using umbral calculus techniques. Especially, we will represent the extended r-central Bell polynomials in terms of quite a few families of well-known special polynomials.
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1 Introduction and preliminaries
In [5], the extended r-central factorial numbers of the second kind and the extended r-central Bell polynomials were introduced and various properties and identities related to these numbers and polynomials were investigated by means of generating functions. The extended r-central factorial numbers of the second kind are an extended version of the central factorial numbers of the second kind and also a central analogue of the r-Stirling numbers of the second kind (see [2, 7, 10, 11, 14, 15, 17, 22]). The extended r-central Bell polynomials are an extended version of the central Bell polynomials and also a central analogue of r-Bell polynomials (see [3, 8, 11, 12, 15, 18]).
Here we study the extended r-central factorial numbers of the second kind and the extended r-central Bell polynomials by making use of umbral calculus techniques. In particular, we represent the extended r-central Bell polynomials in terms of many well-known special polynomials. Here the special polynomials are Bernoulli polynomials, Euler polynomials, falling factorial polynomials, Abel polynomials, ordered Bell polynomials, Laguerre polynomials, Daehee polynomials, Hermite polynomials, polynomials closely related to the reverse Bessel polynomials and studied by Carlitz, and Bernoulli polynomials of the second kind. The necessary facts about umbral calculus will be briefly reviewed in the next section.
The central factorials \(x^{[n]}\) (\(n \geq 0\)) are given by (see [1, 4,5,6, 10, 12, 20])
For nonnegative integers n, k, with \(n\geq k\), the central factorial numbers of the second kind \(T(n,k)\) are given by the coefficients in the expansion (see [1, 4,5,6, 10, 12, 20])
It is well known that \(T(2n, 2n-2k)\) enumerates the number of ways to pace k rooks on a 3 D-triangle board of size \((n-1)\) (see [1, 16]). The central factorial numbers of the second kind \(T(n,k)\) are given by the generating function
From (1.3), we can easily deduce that they are explicitly given by
Thus (1.4) yields
and that
where \(\bigtriangleup ^{k} ( -\frac{k}{2} )^{n}= \bigtriangleup ^{k} x^{n} |_{x=-\frac{k}{2}}\), \(\bigtriangleup f(x)=f(x+1)-f(x)\) is the forward difference operator, \(\delta ^{k} 0^{n}=\delta ^{k} x^{n} |_{x=0}\), and \(\delta f(x)=f ( x+\frac{1}{2} )-f ( x-\frac{1}{2} )\) is the central difference operator.
For these results, one may refer to [19, 20].
Let r be any nonnegative integer. The central factorial numbers of the second kind \(T(n,k)\) were generalized to the extended r-central factorial numbers of the second kind \(T_{r}(n+r,k+r)\) (see [5]). For nonnegative integers n, k, with \(n\geq k\), \(T_{r}(n+r,k+r)\) are given by the coefficients in the expansion
The extended r-central factorial numbers of the second kind, \(T_{r}(n+r,k+r)\), are also given by the generating function
An explicit expression for \(T_{r}(n+r,k+r)\) can be deduced from (1.8) as follows:
where \(\delta ^{k} r^{n}=\delta ^{k} x^{n} |_{x=r}\), and by induction we can show
For some details on these, one may refer to [4, 5, 20]. The central Bell polynomials \(B_{n}^{(c)}(x)\) are defined by (see [5, 10, 12, 13])
Then it is immediate from (1.11) that
and that (see [12])
where \(S_{2}(l,k)\) are the Stirling numbers of the second kind, given by
Further, the central Bell polynomials are given by the following Dobinski-like formula (see [12]):
On the other hand, the extended r-central Bell polynomials \(B_{n}^{(c,r)}(x)\) are defined by (see [5, 6, 21])
Then it is easy from (1.16) that
and that (see [5])
In addition, the extended r-central Bell polynomials are given by the following Dobinski-like formula:
which can be observed immediately from the proof of Theorem 2.3 in [12].
2 Quick review of umbral calculus
Here we will briefly recall some of the basic facts about umbral calculus. The reader is advised to refer to [20] for a complete treatment. Let \(\mathbb{C}\) be the field of complex numbers, and let \(\mathfrak{F}\) be the algebra of all formal power series in the variable t with the coefficients in \(\mathbb{C}\):
Let \(\mathbb{P}=\mathbb{C}[x]\) denote the ring of polynomials in x with the coefficients in \(\mathbb{C}\), and let \(\mathbb{P}^{*}\) be the vector space of all linear functionals on \(\mathbb{P}\). For \(L \in \mathbb{P}^{*}\) and \(p(x)\in \mathbb{P}\), the notation \(\langle L|p(x)\rangle \) will be used for the action of the linear functional L on \(p(x)\).
For \(f(t)= \sum_{k=0}^{\infty }a_{k} \frac{t^{k}}{k!} \in \mathfrak{F}\), the linear functional \(\langle f(t)| \cdot \rangle \) on \(\mathbb{P}\) is defined by
In particular, from (2.2) we see that
where \(\delta _{n,k}\) is the Kronecker symbol.
For \(L\in \mathbb{P}^{*}\), let \(f_{L}(t)=\sum_{k=0}^{\infty }\langle L|x^{k}\rangle \frac{t ^{k}}{k!}\in \mathfrak{F}\). Then we note that \(\langle f_{L}(t)| x^{n}\rangle =\langle L|x ^{n}\rangle \), and the map \(L\rightarrow f_{L}(t)\) is a vector space isomorphism from \(\mathbb{P}^{*}\) to \(\mathfrak{F}\). Henceforth, \(\mathfrak{F}\) denotes both the algebra of all formal power series in t and the vector space of all linear functionals on \(\mathbb{P}\). Thus an element \(f(t)\) of \(\mathfrak{F}\) will be thought of as both a formal power series and a linear functional on \(\mathbb{P}\). \(\mathfrak{F}\) is called the umbral algebra, the study of which the umbral calculus is.
The order \(o(f(t))\) of \(0\neq f(t) \in \mathfrak{F} \) is the smallest integer k such that the coefficient of \(t^{k}\) does not vanish. In particular, for \(0\neq f(t)\in \mathfrak{F}\) it is called an invertible series if \(o(f(t))=0\) and a delta series if \(o(f(t))=1\). Let \(f(t), g(t) \in \mathfrak{F}\), with \(o(g(t))=0\), \(o(f(t))=1\). Then there exists a unique sequence of polynomials \(s_{n}(x) (\operatorname{deg} s _{n}(x)=n)\) such that
Such a sequence is called the Sheffer sequence for the Sheffer pair \((g(t), f(t))\), which we denote by \(s_{n}(x)\sim (g(t),f(t))\). Then \(s_{n}(x)\sim (g(t), f(t))\) if and only if
where \(\bar{f}(t)\) is the compositional inverse of \(f(t)\) satisfying \(f(\bar{f}(t))=\bar{f}(f(t))=t\).
Let \(s_{n}(x)\sim (g(t), f(t))\). Then we have the following: The Sheffer identity is given by
where \(p_{n}(x)=g(t) s_{n}(x)\sim (1,f(t))\). Then the conjugate representation says that
We also have the recurrence formula
The derivative of \(s_{n}(x)\) is given by
Assume that \(s_{n}(x)\sim (g(t), f(t))\), \(r_{n}(x)\sim (h(t), l(t))\). Then \(s_{n}(x)=\sum_{k=0}^{n} c_{n,k}r_{k}(x)\), where
Let \(p_{n}(x)\sim (1,f(t))\), \(q_{n}(x)\sim (1,l(t))\). Then the transfer formula says that
Finally, for \(h(t)\in \mathfrak{F}\), \(p(x)\in \mathbb{P}\),
3 Main results
Here we will derive some properties, identities and recurrence relations for the extended r-central Bell polynomials by making use of umbral calculus techniques and the formulas in Sect. 2. In addition, we will express those polynomials as linear combinations of quite a few well-known special polynomials. Here the special polynomials are Bernoulli polynomials, Euler polynomials, falling factorial polynomials, Abel polynomials, ordered Bell polynomials, Laguerre polynomials, Daehee polynomials, Hermite polynomials, polynomials closely related to the reverse Bessel polynomials and studied by Carlitz, and Bernoulli polynomials of the second kind.
We first note from (1.16) and (2.4) that
Using (2.14) for \(n\geq 1\), we have
Thus by replacing n by \(n+1\), we obtained the following theorem.
Theorem 3.1
For any nonnegative integer n, we have
For \(n\geq 1\) and from (2.11), we get
Again, by replacing n by \(n+1\), we have shown the next result.
Theorem 3.2
For any nonnegative integer n, we have the following expression
From (3.2), we first observe that
Then, by using (2.8) and (2.9), we obtain
This does not give us a new result. In fact, combining (3.3) and (3.6) yields Eq. (3.4).
In order to apply Eq. (2.10), we first note from (3.5) and \(\bar{f}(t)=e^{\frac{t}{2}} - e^{-\frac{t}{2}}\) that
Then, by (2.10), we have
Here \(E_{n}^{*}\) are the type 2 Euler numbers, which are given by
Thus we have shown the following theorem.
Theorem 3.3
For \(n\geq 0\), we have the following identity:
where \(E_{n}^{*} \) are the type 2 Euler numbers given in (3.8).
Noting that \(B_{n}^{(c)} (x)=g(t) B_{n}^{(c,r)} (x)\), from the Sheffer identity in (2.6), we have
Noting that the Bernoulli polynomials \(B_{n}(x)\) is Sheffer for the pair \((\frac{e^{t}-1}{t}, t )\), we write \(B_{n}^{(c,r)} (x) = \sum_{k=0}^{n} C_{n,k} B_{k}(x)\). Then
Before proceeding, let us recall that \(B_{n}^{*}\) are the type 2 Bernoulli numbers, which are defined by
From (3.10) and (3.12), we have
Here \(B_{n}^{(c)}\) are the central Bell numbers, given by
Finally, from (3.12) we obtain
This completes the proof for the next theorem.
Theorem 3.4
For \(n\geq 0\), we have the following representation of \(B_{n}^{(c,r)}(x)\) in terms of \(B_{k}(x)\):
where \(B_{n}^{*} \) are the type 2 Bernoulli numbers in (3.11) and \(B_{n}^{(c)}\) are the central Bell numbers in (3.13).
Let us write \(B_{n}^{(c,r)}(x)=\sum_{k=0}^{n} C_{n,k} E_{k}(x)\). Here \(E_{n}(x)\) are the Euler polynomials with \(E_{n}(x) \sim ( \frac{e ^{t}+1}{2}, t )\). Then
This shows the next result.
Theorem 3.5
For \(n\geq 0\), we have the following representation of \(B_{n}^{(c,r)}(x)\) in terms of \(E_{k}(x)\):
We let \(B_{n}^{(c,r)}(x)=\sum_{k=0}^{n} C_{n,k}(x)_{k}\). Here \((x)_{n}\) is the falling factorial sequence with \((x)_{n} \sim (1, e ^{t}-1)\). Then
Here \(S_{2,r} (l+r,k+r)\) are the r-Stirling numbers of the second kind, given by
This gives the next result.
Theorem 3.6
For \(n\geq 0\), we have the following representation of \(B_{n}^{(c,r)}(x)\) in terms of \((x)_{k}\):
To obtain another expression, we compute \(C_{n,k}\) in (3.16) in a different way as follows:
This finishes the proof of the next theorem.
Theorem 3.7
For \(n\geq 0\), we have the following representation of \(B_{n}^{(c,r)}(x)\) in terms of \((x)_{k}\):
Let \(B_{n}^{(c,r)} (x)= \sum_{k=0}^{n} C_{n,k}A_{k}(x;a)\). Here \(A_{n}(x;a)\) are the Abel polynomials with \(A_{n}(x;a)\sim (1,te^{at})\), \((a\neq 0)\). Then
Thus the following has been verified.
Theorem 3.8
For \(n\geq 0\), we have the following representation of \(B_{n}^{(c,r)}(x)\) in terms of \(A_{k}(x;a)\):
Let us write \(B_{n}^{(c,r)}(x)= \sum_{k=0}^{n} C_{n,k}Ob_{k}(x)\). Here \(Oh_{n}(x)\) are the ordered Bell polynomials with \(Ob_{n}(x)\sim (2-e ^{t}, t)\). Then
This shows the following result.
Theorem 3.9
For \(n\geq 0\), we have the following representation of \(B_{n}^{(c,r)}(x)\) in terms of \(Ob_{k}(x)\):
We write \(B_{n}^{(c,r)}(x)= \sum_{k=0}^{n} C_{n,k}L_{k}^{(\alpha )}(x)\), where \(L_{k}^{(\alpha )}(x)\) are the Laguerre polynomials with \(L_{k}^{(\alpha )}(x)\sim ((1-t)^{-\alpha -1}, \frac{t}{t-1})\). Then
Before proceeding, we recall several definitions. The central Fubini polynomials \(F_{n}^{(c)}(x)\) are defined by (see [9])
For \(x=1\), \(F_{n}^{(c)}=F_{n}^{(c)}(1)\) are called the central Fubini numbers.
More generally, for any real number α, the central Fubini polynomials \(F_{n}^{(c,x)}(x)\) of order α are given by
For \(x=1\), \(F_{n}^{(c,\alpha )}=F_{n}^{(c,\alpha )}(1)\) are called the central Fubini numbers of order α. Now, from (3.21) and (3.23) we have
This verifies the following theorem.
Theorem 3.10
For \(n\geq 0\), we have the following representation of \(B_{n}^{(c,r)}(x)\) in terms of \(L_{k}^{(\alpha )}(x)\).
Let us write \(B_{n}^{(c,r)}(x)= \sum_{k=0}^{n} C_{n,k}D_{k}(x)\). Here \(D_{n}(x)\) are the Daehee polynomials with \(D_{n} (x)\sim (\frac{e ^{t}-1}{t}, e^{t}-1)\). Then
This completes the proof for the next result.
Theorem 3.11
For \(n\geq 0\), we have the following representation of \(B_{n}^{(c,r)}(x)\) in terms of \(D_{k}(x)\).
Let us put \(B_{n}^{(c,r)}(x)= \sum_{k=0}^{n} C_{n,k}H_{k}^{(\nu )}(x)\). Here \(H_{k}^{(\nu )}(x)\) are the Hermite polynomials with \(H_{k}^{( \nu )}(x)\sim (e^{\frac{\nu t^{2}}{2}}, t)\). Then
This shows the following theorem.
Theorem 3.12
For \(n\geq 0\), we have the following representation of \(B_{n}^{(c,r)}(x)\) in terms of \(H_{k}^{(\nu )}(x)\).
The Bessel polynomials \(y_{n}(x)\) are given by
which satisfies the differential equation
The reverse Bessel polynomials are known to be
which obey
On the other hand, Carlitz defined a related set of polynomials,
Then we can show that \(P_{n}(x)\sim (1, t-\frac{1}{2} t^{2} )\) (see [20]). Let us write \(B_{n}^{(c,r)}(x)=\sum_{k=0}^{n} C _{n,k}P_{k}(x)\). Then
This completes the proof for the next theorem.
Theorem 3.13
For \(n\geq 0\), we have the following representation of \(B_{n}^{(c,r)}(x)\) in terms of \(P_{k}(x)\):
We write \(B_{n}^{(c,r)}(x)=\sum_{k=0}^{n} C_{n,k}b_{k}(x)\). Here \(b_{n}(x)\) are the Bernoulli polynomials of the second kind with \(b_{n} (x)\sim (\frac{t}{e^{t}-1}, e^{t}-1 )\). Then
where \(S_{2}(l,k)\) are the Stirling numbers of the second and \(B_{s}\) are the Bernoulli numbers, given by
Thus we have shown the next theorem.
Theorem 3.14
For \(n\geq 0\), we have the following representation of \(B_{n}^{(c,r)}(x)\) in terms of \(b_{k}(x)\).
From (3.2), \(B_{n}^{(c,r)}(x)= ( \frac{t+\sqrt{t^{2}+4}}{2} )^{2r} B_{n}^{(c)}(x)\), and hence
In particular, for \(s=1\) we have
Thus we have shown the following theorem.
Theorem 3.15
The following identity holds true.
4 Conclusions
In this paper, we studied the extended r-central factorial numbers of the second kind and the extended r-central Bell polynomials by making use of umbral calculus techniques. We noted that the extended r-central factorial numbers of the second kind are an extended version of the central factorial numbers of the second kind and also a central analog of the r-Stirling numbers of the second kind. Also, the extended r-central Bell polynomials are an extended version of the central Bell polynomials and also a central analogue of r-Bell polynomials.
We derived some properties, identities and recurrence relations. In addition, we represented the extended r-central Bell polynomials in terms of many well-known special polynomials. Here the special polynomials are Bernoulli polynomials, Euler polynomials, falling factorial polynomials, Abel polynomials, ordered Bell polynomials, Laguerre polynomials, Daehee polynomials, Hermite polynomials, polynomials closely related to the reverse Bessel polynomials and studied by Carlitz, and Bernoulli polynomials of the second kind.
Finally, along the same line as this paper, we will continue to investigate some special numbers and polynomials from the umbral calculus viewpoint.
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Acknowledgements
This paper was supported by Konkuk University in 2017. We would like to thank the referees for their valuable comments and suggestions that improved the original manuscript to its present form.
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Each of the authors, L-CJ, TK, DSK, and HYK, contributed to each part of this study equally and read and approved the final version of the manuscript.
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Jang, LC., Kim, T., Kim, D.S. et al. Extended r-central Bell polynopmials with umbral calculus viewpoint. Adv Differ Equ 2019, 202 (2019). https://doi.org/10.1186/s13662-019-2141-1
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DOI: https://doi.org/10.1186/s13662-019-2141-1