Hindawi Publishing Corporation Abstract and Applied Analysis Volume 2012, Article ID 865721, 12 pages doi:10.1155/2012/865721 Research Article Applications of Umbral Calculus Associated with p-Adic Invariant Integrals on Zp Dae San Kim1 and Taekyun Kim2 1 2 Department of Mathematics, Sogang University, Seoul 121-742, Republic of Korea Department of Mathematics, Kwangwoon University, Seoul 139-701, Republic of Korea Correspondence should be addressed to Taekyun Kim, tkkim@kw.ac.kr Received 8 November 2012; Accepted 22 November 2012 Academic Editor: Gaston N’Guerekata Copyright q 2012 D. S. Kim and T. Kim. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Recently, Dere and Simsek 2012 have studied the applications of umbral algebra to some special functions. In this paper, we investigate some properties of umbral calculus associated with p-adic invariant integrals on Zp . From our properties, we can also derive some interesting identities of Bernoulli polynomials. 1. Introduction Let p be a fixed prime number. Throughout this paper, Zp , Qp , and Cp denote the ring of padic integers, the field of p-adic rational numbers, and the completion of algebraic closure of Qp , respectively. Let N ∪ {0}. Let UDZp be space of uniformly differentiable functions on Zp . For f ∈ UDZp , the p-adic invariant integral on Zp is defined by p −1 1 fxdμx lim N fx, N →∞p Zp x0 N 1.1 see 1, 2. From 1.1, we have Zp fx ndμx − Zp fxdμx n l0 f l, n ∈ N, 1.2 2 Abstract and Applied Analysis where f l dfx/dx|xl see 1–6. Let F be the set of all formal power series in the variable t over Cp with F ft ∞ ak k0 k! t | ak ∈ Cp . k 1.3 Let P Cp x and let P∗ denote the vector space of all linear functional on P. The formal power series, ft ∞ ak k! k0 tk ∈ F, 1.4 defines a linear functional on P by setting ft | xn an , ∀n ≥ 0, 1.5 see 7, 8. In particular, by 1.4 and 1.5, we get tk | xn n!δn,k , 1.6 where δn,k is the Kronecker symbol see 7. Here, F denotes both the algebra of formal power series in t and the vector space of all linear functional on P, so an element ft of F will be thought of as both a formal power series and a linear functional. We shall call F the umbral algebra. The umbral calculus is the study of umbral algebra. The order oft of power series ft / 0 is the smallest integer k for which ak does not vanish. We define oft ∞ if ft 0. From the definition of order, we note that oftgt oft ogt and oft gt ≥ min{oft, ogt}. The series ft has a multiplicative inverse, denoted by ft−1 or 1/ft, if and only if oft 0. Such a series is called invertible series. A series ft for which oft 1 is called a delta series see 7, 8. Let ft, gt ∈ F. Then, we have ftgt | px ft | gtpx gt | ftpx . 1.7 By 1.5 and 1.6, we get eyt | xn yn , eyt | px p y , 1.8 see 7. Notice that for all ft in F, ∞ ft | xk ft tk , k! k0 1.9 Abstract and Applied Analysis 3 and for all polynomials px, tk | px xk , px k! k≥0 1.10 see 7, 8. Let f1 t, f2 t, . . . , fm t ∈ F. Then, we have f1 tf2 t · · · fm t | xn n f1 t | xi1 · · · fm t | xim , i 1 , . . . , im 1.11 where the sum is over all nonnegative integers i1 , i2 , . . . , im such that i1 · · · im n see 8. By 1.10, we get pk x n tl | px dk px ll − 1 · · · l − k 1xl−k . l! dxk lk 1.12 Thus, from 1.12, we have pk 0 tk | px 1 | pk x , 1.13 see 7. By 1.13, we get t px p k k x dk px dxk . 1.14 Thus, by 1.14, we see that eyt px p x y . 1.15 Let us assume that sn x is a polynomial of degree n. Suppose that ft, gt ∈ F with oft 1 and ogt 0. Then, there exists a unique sequence sn x of polynomials satisfying gtftk | sn x n!δn,k for all n, k ≥ 0. The sequence sn x is called the Sheffer sequence for gt, ft, which is denoted by sn x ∼ gt, ft. The Sheffer sequence for gt, t is called the Appell sequence for gt, or sn x is Appell for gt, which is indicated by sn x ∼ gt, t. 4 Abstract and Applied Analysis For px ∈ P, it is known that ft | xpx ∂t ft | px f t | px , yt e − 1 | px p y − p0, 1.16 see 7, 8. Let sn x ∼ gt, ft. Then, we have ht ∞ ht | sk x k! k0 px ∞ gtftk | px k! k0 1 gtftk , e g ft yft ∞ s y k tk , k! k0 ht ∈ F, 1.17 px ∈ P, 1.18 for any y ∈ Cp , 1.19 sk x, where ft is the compositional inverse of ft, and ftsn x nsn−1 x, 1.20 see 7, 8. We recall that the Bernoulli polynomials are defined by the generating function to be ∞ tn t xt Bxt e e Bn x , t n! e −1 n0 1.21 with the usual convention about replacing Bn x by Bn x see 1–16. In the special case, x 0, Bn 0 Bn are called the nth Bernoulli numbers. By 1.21, we easily get Bn x B xn n n l l0 Bl xn−l n n l0 l Bn−l xl . 1.22 Thus, by 1.22, we see that Bn x is a monic polynomial of degree n. It is easy to show that B0 1, Bn 1 − Bn δ1,n , 1.23 see 13–15. From 1.2, we can derive the following equation: Zp fx 1dμx − Zp fxdμx f 0. 1.24 Abstract and Applied Analysis 5 Let us take fx etx ∈ UDZp . Then, from 1.21, 1.22, 1.23, and 1.24, we have x dμx Bn , Zp n x y dμ y Bn x, n Zp 1.25 where n ≥ 0 see 1, 2. Recently, Dere and simsek have studied applications of umbral algebra to some special functions see 7. In this paper, we investigate some properties of umbral calculus associated with p-adic invariant integrals on Zp . From our properties, we can derive some interesting identities of Bernoulli polynomials. 2. Applications of Umbral Calculus Associated with p-Adic Invariant Integrals on Zp Let sn x be an Appell sequence for gt. By 1.19, we get 1 n x sn x, gt iff xn gtsn x. 2.1 Let us take gt et − 1/t ∈ F. Then, gt is clearly invertible series. From 1.21 and 2.1, we have ∞ Bk x k! k0 tk 1 xt e . gt 2.2 Thus, by 2.2, we get 1 n x Bn x, gt tBn x Bn x nBn−1 x, n ≥ 0. 2.3 From 1.21, 2.1, and 2.3, we note that Bn x is an Appell sequence for gt et − 1/t. Let us take the derivative with respect to t on both sides of 2.2. Then, we have ∞ Bk x k1 k! ktk−1 xgtext − ext g t gt2 ∞ k0 xk xk g t x − gt gt gt tk . k! 2.4 Thus, by 2.4, we get xk g t xk Bk1 x x − gt gt gt g t x− gt Bk x, 2.5 6 Abstract and Applied Analysis where k ≥ 0. Zp e xy1t dμ y − Zp exyt dμ y text . 2.6 Thus, by 2.6, we get Zp n x y 1 dμ y − n x y μ y nxn−1 , Zp n ≥ 0. 2.7 From 1.25 and 2.7, we have Bn x 1 − Bn x nxn−1 , 2.8 n ≥ 0. By 2.5, we see that gtBk1 x gtxBk x − g tBk x, 2.9 Thus, by 2.9, we have et − 1 Bk1 x et − 1 xBk x − et − gt Bk x, k ≥ 0, 2.10 and we can derive the following equation. From 2.3 and 2.10, Bk1 x 1 − Bk1 x x 1Bk x 1 − xBk x − Bk x 1 xk , k ≥ 0. 2.11 By 2.8 and 2.11, we see that Bk1 x 1 Bk1 x k 1xk . 2.12 Therefore, by 2.5, we obtain the following theorem. Theorem 2.1. For k ∈ Z , one has Bk1 x x− g t Bk , gt 2.13 where g t dgt/dt. Corollary 2.2. For ≥ 0, one has Bk1 x 1 Bk1 x k 1xk . 2.14 Abstract and Applied Analysis 7 Let us consider the linear functional ft that satisfies ft | px pudμu, Zp 2.15 for all polynomials px. It can be determined from 1.9 that ∞ ft | xk ∞ tk k ft t uk dμu k! k! k0 k0 Zp eut dμu. 2.16 Zp By 1.24 and 2.16, we get ft Zp eut dμu et t . −1 2.17 Therefore, by 2.17, we obtain the following theorem. Theorem 2.3. For px ∈ P, one has Zp e dμu | px ut Zp pudμu. 2.18 That is t | px et − 1 Zp pudμu. 2.19 In particular, one has Bn e dμu | x ut Zp n . 2.20 From 1.24, one has n0 n tn x y dμ y n! Zp Zp exyt dμ y ∞ n0 tn e dμ y xn . n! Zp yt 2.21 8 Abstract and Applied Analysis By 1.25 and 2.21, we get Bn x n x y dμ y Zp Zp eyt dμ y xn , 2.22 where n ≥ 0. Therefore, by 2.22, we obtain the following theorem. Theorem 2.4. For px ∈ P, we have Zp p x y dμ y Zp eyt dμ y px 2.23 t px. t e −1 In particular, one obtains Bn x x y dμ y Zp n Zp eyt dμ y xn 2.24 t xn . t e −1 r The higher order Bernoulli polynomials Bn x are defined by ··· Zp Zp ex1 x2 ···xr xt dμx1 · · · dμxr t t e −1 r ext ∞ tn r Bn x . n! n0 r 2.25 r In the special case, x 0, Bn 0 Bn are called the nth Bernoulli numbers of order r ∈ N. From 2.25, we note that Zp ··· Zp x1 · · · xr n dμx1 · · · dμxr i1 ···ir n i1 ···ir n n i 1 , . . . , ir Zp x1i1 dμx1 Zp n r B · · · Bir Bn . i1 , . . . , ir i1 x2i2 dμx2 · · · Zp xrir dμxr 2.26 Abstract and Applied Analysis 9 By 2.25 and 2.26, we get r Bn x n n l l0 r Bn−l xl . 2.27 r From 2.26 and 2.27, we note that Bn x is a monic polynomial of degree n with coefficients in Q. For r ∈ N, let us assume that g r t −1 Zp ··· e Zp x1 ···xr t dμx1 · · · dμxr et − 1 t r . 2.28 By 2.28, we easily see that g r t is an invertible series. From 2.25 and 2.28, we have ext g r t r Zp ··· Zp ex1 ···xr xt dμx1 · · · dμxr ∞ tn r Bn x , n! n0 2.29 r tBn x nBn−1 x. r From 2.29, we note that Bn is an Appell sequence for g r t. Therefore, by 2.29, we obtain the following theorem. Theorem 2.5. For px ∈ P and r ∈ N, one has Zp ··· Zp px1 · · · xr xdμx1 · · · dμxr t et − 1 r px. 2.30 ex1 ···xr t dμx1 · · · dμxr xn . 2.31 In particular, the Bernoulli polynomials of order r are given by r Bn x t et − 1 r xn Zp ··· Zp That is r Bn x ∼ et − 1 t r ,t . 2.32 Let us consider the linear functional f r t that satisfies f r t | px Zp ··· Zp px1 · · · xr dμx1 · · · dμxr , 2.33 10 Abstract and Applied Analysis for all polynomials px. It can be determined from 1.9 that ∞ f r t | xk k r t f t k! k0 ∞ Zp k0 tk k! 2.34 ex1 ···xr t dμx1 · · · dμxr Zp t t e −1 x1 · · · xr k dμx1 · · · dμxr Zp ··· Zp ··· r . Therefore, by 2.34, we obtain the following theorem. Theorem 2.6. For px ∈ P, one has Zp ··· That is t et − 1 r e Zp x1 ···xr t dμx1 · · · dμxr | px 2.35 Zp ··· Zp | px px1 · · · xr dμx1 · · · dμxr . Zp ··· Zp px1 · · · xr dμx1 · · · dμxr . 2.36 In particular, one gets r Bn Zp ··· Zp e x1 ···xr t dμx1 · · · dμxr | x n 2.37 . Remark 2.7. From 1.11, we note that x1 ···xr t n ··· e dμx1 · · · dμxr | x Zp Zp ni1 ···ir n i 1 , . . . , ir Zp e x1 t dμx1 | x i1 ··· 2.38 e dμxr | x xr t Zp ir . By Theorems 2.3 and 2.6 and 2.38, we get r Bn ni1 ···ir n B · · · Bir . i1 , . . . , ir i1 Let sn x be the Sheffer sequence for gt, ft. 2.39 Abstract and Applied Analysis 11 Then the Sheffer identity is given by n n sn x y pk y sn−k x, k k0 2.40 see 7, 8, where pk y gtsk y. 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