Volume 2013, Issue 1 871512
Research Article
Open Access

Umbral Calculus and the Frobenius-Euler Polynomials

Dae San Kim

Dae San Kim

Department of Mathematics, Sogang University, Seoul 121-742, Republic of Korea sogang.ac.kr

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Taekyun Kim

Corresponding Author

Taekyun Kim

Department of Mathematics, Kwangwoon University, Seoul 139-701, Republic of Korea kw.ac.kr

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Sang-Hun Lee

Sang-Hun Lee

Division of General Education, Kwangwoon University, Seoul 139-701, Republic of Korea kw.ac.kr

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First published: 07 February 2013
Citations: 1
Academic Editor: Juan J. Trujillo

Abstract

We study some properties of umbral calculus related to the Appell sequence. From those properties, we derive new and interesting identities of the Frobenius-Euler polynomials.

1. Introduction

Let C be the complex number field. For λC with λ ≠ 1, the Frobenius-Euler polynomials are defined by the generating function to be
(1)
(see [15]) with the usual convention about replacing Hn(xλ) by Hn(xλ).
In the special case, x = 0,  Hn(0∣λ) = Hn(λ) are called the nth Frobenius-Euler numbers. By (1), we get
(2)
(see [69]) with the usual convention about replacing Hn(λ) by Hn(λ).
Thus, from (1) and (2), we note that
(3)
where δn,k is the kronecker symbol (see [1, 10, 11]).
For rZ+, the Frobenius-Euler polynomials of order r are defined by the generating function to be
(4)
In the special case, are called the nth Frobenius-Euler numbers of order r (see [1, 10]).
From (4), we can derive the following equation:
(5)
By (5), we see that is a monic polynomial of degree n with coefficients in Q(λ).
Let be the algebra of polynomials in the single variable x over C and let * be the vector space of all linear functionals on . As is known, 〈Lp(x)〉 denotes the action of the linear functional L on a polynomial p(x) and we remind that the addition and scalar multiplication on * are, respectively, defined by
(6)
where c is a complex constant (see [3, 12]).
Let F denote the algebra of formal power series:
(7)
(see [3, 12]). The formal power series define a linear functional on by setting
(8)
Indeed, by (7) and (8), we get
(9)
(see [3, 12]). This kind of algebra is called an umbral algebra.
The order O(f(t)) of a nonzero power series f(t) is the smallest integer k for which the coefficient of tk does not vanish. A series f(t) for which O(f(t)) = 1 is said to be an invertible series (see [2, 12]). For f(t), g(t) ∈ F, and p(x) ∈ , we have
(10)
(see [12]). One should keep in mind that each f(t) ∈ F plays three roles in the umbral calculus: a formal power series, a linear functional, and a linear operator. To illustrate this, let p(x) ∈ and f(t) = eytF. As a linear functional, eyt satisfies 〈eytp(x)〉 = p(y). As a linear operator, eyt satisfies eytp(x) = p(x + y) (see [12]). Let sn(x) denote a polynomial in x with degree n. Let us assume that f(t) is a delta series and g(t) is an invertible series. Then there exists a unique sequence sn(x) of polynomials such that 〈g(t)f(t) ksn(x)〉 = n! δn,k for all n, k ≥ 0 (see [3, 12]). This sequence sn(x) is called the Sheffer sequence for (g(t), f(t)) which is denoted by sn(x)~(g(t), f(t)). If sn(x)~(1, f(t)), then sn(x) is called the associated sequence for f(t). If sn(x)~(g(t), t), then sn(x) is called the Appell sequence.
Let sn(x)~(g(t), f(t)). Then we see that
(11)
(12)
where is the compositional inverse of f(t) (see [3]). In this paper, we study some properties of umbral calculus related to the Appell sequence. For those properties, we derive new and interesting identities of the Frobenius-Euler polynomials.

2. The Frobenius-Euler Polynomials and Umbral Calculus

By (4) and (12), we see that
(13)
Thus, by (13), we get
(14)
Let
(15)
Then it is an (n + 1)-dimensional vector space over Q(λ).
So we see that is a basis for n(λ). For p(x) ∈ n(λ), let
(16)
Then, by (13), (14), and (16), we get
(17)
From (17), we have
(18)
Therefore, by (16) and (18), we obtain the following theorem.

Theorem 1. For p(x) ∈ n(λ), let

(19)
Then one has
(20)
where Dp(x) = dp(x)/dx.

From Theorem 1, we note that
(21)
Let us consider the operator with and let . Then we have
(22)
Thus, by (22), we get
(23)
From (4), we can derive
(24)
By (23) and (24), we get
(25)
From (25), we have
(26)
For sZ+, from (25), we have
(27)
On the other hand, by (12), (13), and (25),
(28)
Thus, by (28), we get
(29)
Therefore, by (27) and (29), we obtain the following theorem.

Theorem 2. For any r, s ≥ 0, one has

(30)

Let us take s = r − 1  (r ≥ 1) in Theorem 2. Then we obtain the following corollary.

Corollary 3. For n ≥ 0,   r ≥ 1, one has

(31)

Let us take s = r  (r ≥ 1) in Theorem 2. Then we obtain the following corollary.

Corollary 4. For n ≥ 0, r ≥ 1, one has

(32)

Now, we define the analogue of Stirling numbers of the second kind as follows:
(33)
Note that S1(n, k) = S(n, k) is the Stirling number of the second kind.
From the definition of , we have
(34)
By (33) and (34), we get
(35)
Let us take s = 2r. Then we have
(36)
By (36), we get
(37)
Let us take x = 0 in (37). Then we obtain the following theorem.

Theorem 5. We have

(38)

Let us consider s = 2r − 1 in the identity of Theorem 2. Then we have
(39)
Let us take x = 0 in (39). Then we obtain the following theorem.

Theorem 6. For n ≥ 0 and r ≥ 1, one has

(40)

Remark 7. Note that

(41)

Acknowledgment

The authors would like to express their gratitude to the referees for their valuable suggestions.

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