A New Extension of Q-Euler Numbers and Polynomials Related to Their Interpolation Functions

A New Extension of Q-Euler Numbers and Polynomials Related to Their Interpolation Functions

CORE Metadata, citation and similar papers at core.ac.uk Provided by Elsevier - Publisher Connector Applied Mathematics Letters 21 (2008) 934–939 www.elsevier.com/locate/aml A new extension of q-Euler numbers and polynomials related to their interpolation functions Hacer Ozdena,∗, Yilmaz Simsekb a University of Uludag, Faculty of Arts and Science, Department of Mathematics, Bursa, Turkey b University of Akdeniz, Faculty of Arts and Science, Department of Mathematics, Antalya, Turkey Received 9 March 2007; received in revised form 30 July 2007; accepted 18 October 2007 Abstract In this work, by using a p-adic q-Volkenborn integral, we construct a new approach to generating functions of the (h, q)-Euler numbers and polynomials attached to a Dirichlet character χ. By applying the Mellin transformation and a derivative operator to these functions, we define (h, q)-extensions of zeta functions and l-functions, which interpolate (h, q)-extensions of Euler numbers at negative integers. c 2007 Elsevier Ltd. All rights reserved. Keywords: p-adic Volkenborn integral; Twisted q-Euler numbers and polynomials; Zeta and l-functions 1. Introduction, definitions and notation Let p be a fixed odd prime number. Throughout this work, Zp, Qp, C and Cp respectively denote the ring of p- adic rational integers, the field of p-adic rational numbers, the complex numbers field and the completion of algebraic | | = −vp(p) = 1 closure of Qp. Let vp be the normalized exponential valuation of Cp with p p p p . When one talks of q-extension, q is considered in many ways, e.g. as an indeterminate, a complex number q ∈ C, or a p-adic number − 1 p−1 x q ∈ Cp. If q ∈ C we assume that |q| < 1. If q ∈ Cp, we assume that |1 − q|p < p , so that q = exp(x log q) for |x|q 6 1; cf. [3,2,5–7,4,11,14,16,1]. We use the following notation: 1 − qx 1 − (−q)x [x] = , [x]− = , q 1 − q q 1 + q where limq→1 [x]q = x; cf. [5]. Let UD Zp be the set of uniformly differentiable functions on Zp. For f ∈ UD Zp , Kim [3] originally defined the p-adic invariant q-integral on Zp as follows: Z pN −1 1 X x Iq ( f ) = f (x)dµq (x) = lim f (x)q , N→∞ N Zp p q x=0 ∗ Corresponding author. E-mail addresses: [email protected] (H. Ozden), [email protected] (Y. Simsek). 0893-9659/$ - see front matter c 2007 Elsevier Ltd. All rights reserved. doi:10.1016/j.aml.2007.10.005 H. Ozden, Y. Simsek / Applied Mathematics Letters 21 (2008) 934–939 935 where N is a natural number and p is an odd prime number. The q-deformed p-adic invariant integral on Zp, in the fermionic sense, is defined by Z I−q ( f ) = lim Iq ( f ) = f (x)dµ−q (x), cf. [3,5,6,4]. q→−q Zp Recently, twisted (h, q)-Bernoulli and Euler numbers and polynomials were studied by several authors (see [10,2,15, 16,9,8,13,1]). By definition of µ−q (x), we see that I−1( f1) + I−1( f ) = 2 f (0), cf. [5], (1.1) where f1(x) = f (x + 1). In this study, we define new (h, q)-extension of Euler numbers and polynomials. By using a derivative operator on these functions, we derive (h, q)-extensions of zeta functions and l-functions, which interpolate (h, q)-extensions of Euler numbers at negative integers. 2. A new approach to q-Euler numbers In this section, we define (h, q)-extension of Euler numbers and polynomials. Substituting f (x) = qhx etx , with h ∈ Z, into (1.1) we have ∞ n h hx tx 2 X (h) t F (t) = I− (q e ) = = E , |h log q + t| < π, (2.1) q 1 qhet + 1 n,q n! n=0 (h) (h) where En,q is called the (h, q)-extension of Euler numbers. limq→1 En,q = En, where En is the classical Euler numbers. That is ∞ 2 X tn = En cf. [8,4,12,17]. et + 1 n! n=0 (h) (h, q)-extensions of Euler polynomials, En,q (x), are defined by the following generating function: ∞ 2etx X tn Fh(t, x) = Fh(t)etx = = E(h) (x) . (2.2) q q qhet + 1 n,q n! n=0 By using the Maclaurin series of etx in (2.1), we have Z ∞ n n ∞ n X hx t x X (h) t q dµ− (x) = E . n! 1 n,q n! Zp n=0 n=0 tn By comparing coefficients of n! on either side of the above equation, we obtain the Witt formula, which is given by the following theorem. Theorem 1 (Witt Formula). For h ∈ Z, q ∈ Cp with |1 − q|p < 1, Z hx n (h) q x dµ−1(x) = En,q , (2.3) Zp and Z hy n (h) q (x + y) dµ−1(y) = En,q (x). Zp 936 H. Ozden, Y. Simsek / Applied Mathematics Letters 21 (2008) 934–939 From (2.2), we have ∞ ∞ ∞ X tn X tn X tn E(h) xn = E(h) (x) . n,q n! n! n,q n! n=0 n=0 n=0 By the Cauchy product, we see that ∞ n k n−k ∞ n X X h t t X t E( ) xn−k = E(h) (x) . k,q k! (n − k)! n,q n! n=0 k=0 n=0 tn By comparing coefficients of n! , we arrive at the following theorem: Theorem 2. Let n ∈ Z+ = Z ∪ {0}. Then we have n X n h E(h) (x) = xn−k E( ). (2.4) n,q k k,q k=0 Let d be a fixed integer. For any positive integer N, we set = = N = ∗ = [ + N X Xd lim←− Z/dp Z , X1 Zp, X a dp Zp , N 0<a<dp (a,p)=1 N n N o a + dp Zp = x ∈ X : x ≡ a mod dp , N where a ∈ Z with 0 6 a < dp (cf. [3]). It is known that Z Z f (x)dµ−1(x) = f (x)dµ−1(x), cf. [3]. Zp X From this we note that − Z d 1 Z k ht k ht k X a ha a + x d (x + t) q dµ− (t) = d (−1) q t + q dµ− (t), (2.5) 1 d 1 X a=0 Zp where d is an odd positive integer. From (2.2) and (2.5), we obtain the following theorem. Theorem 3 (Distribution Relation). For d an odd positive integer, k ∈ Z+, we have d−1 h X h x + a E( )(x) = dk (−1)aqha E( ) . k,q k,qd d a=0 By (1.1), Kim [5] defined the following integral equation: n−1 n−1 X n−1−l I−1( fn) + (−1) I−1( f ) = 2 (−1) f (l), (2.6) l=0 where n ∈ N, fn(x) = f (x + n). Let d be an odd positive integer and χ be the Dirichlet character with conductor d; substituting f (x) = qhx χ(x)etx , for h ∈ Z, into (2.6), we obtain d−1 P − a ta ha 2 ( 1) χ(a)e q ∞ n a=0 X t π Fh(t, χ) = = E(h) , |t + h log q| < , (2.7) q qhd etd + 1 n,χ,q n! d n=0 (h) where En,χ,q denote (h, q)-extensions of generalized Euler numbers. H. Ozden, Y. Simsek / Applied Mathematics Letters 21 (2008) 934–939 937 From (2.7), we see that − Z d 1 Z hx n hx n n X ha a d a χ(x)q x dµ− (x) = d χ(a)q (−1) q + x dµ− (x). (2.8) 1 d 1 X a=0 Zp By Theorem 1 and (2.8), we obtain the following theorem. Theorem 4. Let d be an odd positive integer and χ be Dirichlet’s character with conductor d. Then we have d−1 X h a E(h) = dn χ(a)qha(−1)a E( ) . n,χ,q n,qd d a=0 From (2.6), we also note that d−1 P − a t(a+x) ha 2 ( 1) χ(a)e q ∞ n a=0 X t Fh(t, x, χ) = = E(h) (x) , (2.9) q qhd etd + 1 n,χ,q n! n=0 (h) h where h ∈ Z, En,χ,q (x) are called generalized (h, q)-extensions of Euler polynomials attached to χ and Fq (t, x, χ) = h tx Fq (t, χ)e . By (2.9), we easily see that Z n hy (h) (x + y) χ(y)q dµ−1(y) = En,χ,q (x). (2.10) X By using (2.10), we arrive at the following theorem. Theorem 5. Let d be an odd integer. Then we have d−1 X h a + x E(h) (x) = dn (−1)aχ(a)qha E( ) . n,χ,q n,qd d a=0 3. A new approach to the (h, q)-Euler zeta function In this section, we assume that q ∈ C with |q| < 1. By using a geometric series in (2.2), we obtain ∞ ∞ X X tn 2ext qhnetn(−1)n = E(h) (x) . n,q n! n=0 n=0 k By applying the derivative operator d | to the above equation, we have dtk t=0 ∞ (h) = X − n hn + k Ek,q (x) 2 ( 1) q (x n) . (3.1) n=0 By (3.1), we define new extensions of Hurwitz type (h, q)-Euler zeta functions as follows: Definition 1.

View Full Text

Details

  • File Type
    pdf
  • Upload Time
    -
  • Content Languages
    English
  • Upload User
    Anonymous/Not logged-in
  • File Pages
    6 Page
  • File Size
    -

Download

Channel Download Status
Express Download Enable

Copyright

We respect the copyrights and intellectual property rights of all users. All uploaded documents are either original works of the uploader or authorized works of the rightful owners.

  • Not to be reproduced or distributed without explicit permission.
  • Not used for commercial purposes outside of approved use cases.
  • Not used to infringe on the rights of the original creators.
  • If you believe any content infringes your copyright, please contact us immediately.

Support

For help with questions, suggestions, or problems, please contact us