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On the Symmetric Properties of Higher-Order Twisted q-Euler Numbers and Polynomials

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doi:10.1155/2010/765259

Research Article

On the Symmetric Properties of Higher-Order Twisted q-Euler Numbers and Polynomials

Eun-Jung Moon,

1

Seog-Hoon Rim,

2

Jeong-Hee Jin,

1

and Sun-Jung Lee

1

1Department of Mathematics, Kyungpook National University, Daegu 702-701, South Korea

2Department of Mathematics Education, Kyungpook National University, Daegu 702-701, South Korea

Correspondence should be addressed to Seog-Hoon Rim,[email protected] Received 14 December 2009; Accepted 19 March 2010

Academic Editor: Panayiotis Siafarikas

Copyrightq2010 Eun-Jung Moon et al. 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.

In 2009, Kim et al. gave some identities of symmetry for the twisted Euler polynomials of higher- order, recently. In this paper, we extend our result to the higher-order twistedq-Euler numbers and polynomials. The purpose of this paper is to establish various identities concerning higher- order twistedq-Euler numbers and polynomials by the properties ofp-adic invariant integral on Zp. Especially, ifq1, we derive the result of Kim et al.2009.

1. Introduction

Letp be a fixed odd prime number. Throughout this paper, the symbolsZ, Zp,Qp,C,and Cp will denote the ring of rational integers, the ring of p-adic integers, the field of p-adic rational numbers, the complex number field, and the completion of the algebraic closure of Qp, respectively. Let Nbe the set of natural numbers and Z N

{0}. Letvp be the normalized exponential valuation ofCpwith|p|pp−vpp1/p.

When one talks of q-extension, q is variously considered as an indeterminate, a complex q ∈ C, or a p-adic number q ∈ Cp. Ifq ∈ C,one normally assumes that |q| < 1.

Ifq∈Cp, then we assume that|q−1|p< p−1/p−1so thatqxexpxlogqfor eachx∈Zp.We use the following notation:

xq 1−qx

1−q , x−q 1−

−qx

1q ∀x∈Zp. 1.1

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For a fixed positive integerdwithp, d 1, set

X Xd limnZ

dpnZ , X1Zp, X

0<a<dp, a,p1

adpZp

,

adpnZp

xX|xa

moddpn ,

1.2

wherea∈Zsatisfies the condition 0≤a < dpn.For anyn∈N,

μq

adpnZp

qa

dpn q 1.3

see1–13is known to be a distribution onX.

We say thatfis a uniformly differentiable function ata∈Zpand denote this property byfUDZpif the difference quotients

Ff

x, y

fxf y

xy 1.4

have a limitfaasx, y → a, a.

ForfUDZp,the fermionicp-adic invariantq-integral onZpis defined as

I−q f

Zp

fxdμ−qx lim

n→ ∞

1 pn −q

pn−1 x0

fx

−qx

1.5

see14. Let us define the fermionicp-adic invariant integral onZpas follows:

I−1 f

lim

q→1I−q f

Zp

fxdμ−1x lim

n→ ∞ pn−1

x0

fx−1x 1.6

see1–12,14–20. From the definition ofq-integral, we have I−1

f1

I−1 f

2f0, wheref1x fx1. 1.7

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Forn∈N, letTpbe thep-adic locally constant space defined by

Tp

n≥1

Cpn lim

n→ ∞Cpn Cp, 1.8

whereCpn {ζ∈Cp|ζpn 1 for somen≥0}is the cyclic group of orderpn.

It is well known that the twistedq-Euler polynomials of orderkare defined as

ext 2

etζq1 k

n0

En,ζ,qk xtn

n!, ζTp, 1.9

and Ekn,ζ,q Ekn,ζ,q0 are called the twisted q-Euler numbers of order k. When k 1, the polynomials and numbers are called the twisted q-Euler polynomials and numbers, respectively. When k 1 and q 1, the polynomials and numbers are called the twisted Euler polynomials and numbers, respectively. Whenk1,q1,andζ1, the polynomials and numbers are called the ordinary Euler polynomials and numbers, respectively.

In15, Kim et al. gave some identities of symmetry for the twisted Euler polynomials of higher order, recently. In this paper, we extend our result to the higher-order twisted q-Euler numbers and polynomials.

The purpose of this paper is to establish various identities concerning higher-order twistedq-Euler numbers and polynomials by the properties ofp-adic invariant integral on Zp. Especially, ifq1, we derive the result of15.

2. Some Identities of the Higher-Order Twisted q -Euler Numbers and Polynomials

Letw1, w2∈Nwithw1≡1mod 2andw2 ≡1mod 2.

ForζTpandm∈N, we set

Rmq w1, w2:ζ

Zmp emi1xiw2xw1tζmi1xiw1qmi1xiw1−1x1· · ·−1xm

Zpew1w2xtζw1w2xqw1w2x−1x

×

Zmp

emi1xiw1yw2tζmi1xiw2qmi1xiw2−1x1· · ·−1xm,

2.1

where

Zmp

fx1, . . . , xm−1x1· · ·−1xm

Zp

· · ·

Zp

m-times

fx1, . . . , xm−1x1· · ·−1xm. 2.2 In2.1, we note thatRmq w1, w2:ζis symmetric inw1andw2.

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From2.1, we derive that

Rmq w1, w2:ζ ew1w2xt

Zmp

emi1xiw1tζmi1xiw1qmi1xiw1−1x1· · ·−1xm

×

Zpew2xmtζw2xmqw2xm−1xm

Zpew1w2xtζw1w2xqw1w2x−1x

×ew1w2yt

Zpm−1

em−1i1 xiw2tζm−1i1 xiw2qm−1i1 xiw2−1x1· · ·−1xm−1. 2.3 From the definition ofq-integral, we also see that

Zpm

emi1xiw1tζmi1xiw1qmi1xiw1−1x1· · ·−1xmew1w2xt

2 ew1tζw1qw11

m

ew1w2xt

n0

Emn,ζw1,qw1w2xw1ntn n! .

2.4

It is easy to see that

Zpextζxqxdμx

Zpew1xtζw1xqw1xdμx w1−1

l0

−1lζlqlelt

k0

Tk,qw1−1 :ζtk

k!, 2.5

whereTk,qw1−1 :ζ w1−1

l0 −1lζlqllk.

From2.3,2.4, and2.5, we can derive Rmq w1, w2:ζ

l0

Eml,ζw1,qw1w2xwl1tl l!

k0

Tk,qw2w1−1 :ζw2 wk2tk k!

i0

Ei,ζm−1w2,qw2

w1yw2iti i!

n0

⎧⎨

n

j0

n j

w2jwn−j1 En−j,ζm w1,qw1w2x j k0

Tk,qw2w1−1 :ζw2 j

k

Em−1j−k,ζw2,qw2

w1y

tn n!.

2.6

From the symmetry ofRmq w1, w2:ζinw1andw2, we also see that Rmq w1, w2:ζ

n0

⎧⎨

n

j0

n j

w1jwn−j2 En−j,ζm w2,qw2w1x j k0

Tk,qw1w2−1 :ζw1 j

k

Em−1j−k,ζw1,qw1

w2y

tn n!.

2.7

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Comparing the coefficients on the both sides of2.6and2.7, we obtain an identity for the twistedq-Euler polynomials of higher order as follows.

Theorem 2.1. Letw1, w2∈Nwithw1≡1mod 2andw2≡1mod 2.

Forn∈Zandm∈N,we have

n j0

n j

wj2wn−j1 Emn−j,ζw1,qw1w2x j k0

Tk,qw2w1−1 :ζw2 j

k

Ej−k,ζm−1w2,qw2

w1y

n

j0

n j

wj1w2n−jEmn−j,ζw2,qw2w1x j k0

Tk,qw1w2−1 :ζw1 j

k

Em−1j−k,ζw1,qw1

w2y .

2.8

Remark 2.2. Takingm1 andy0 inTheorem 2.1, we can derive the following identity:

n j0

n j

wj2w1n−jEn−j,ζw1,qw1w2x j k0

Tk,qw2w1−1 :ζw2 j

k

n

j0

n j

wj1w2n−jEn−j,ζw2,qw2w1x j k0

Tk,qw1w2−1 :ζw1 j

k

.

2.9

Moreover, if we takex 0 andy 0 in Theorem 2.1, then we have the following identity for the twistedq-Euler numbers of higher order.

Corollary 2.3. Letw1, w2 ∈Nwithw1≡1mod 2andw2 ≡1mod 2. Forn∈Zandm∈N, we have

n j0

n j

wj2wn−j1 Emn−j,ζw1,qw1

j k0

Tk,qw2w1−1 :ζw2 j

k

Em−1j−k,ζw2,qw2

n

j0

n j

wj1w2n−jEmn−j,ζw2,qw2

j k0

Tk,qw1w2−1 :ζw1 j

k

Ej−k,ζm−1w1,qw1.

2.10

We also note that takingm1 in Corollary 1 shows the following identity:

n j0

n j

w2jwn−j1 En−j,ζw1,qw1

j k0

Tk,qw2w1−1 :ζw2 j

k

n

j0

n j

wj1wn−j2 En−j,ζw2,qw2

j k0

Tk,qw1w2−1 :ζw1 j

k

.

2.11

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Now we will derive another interesting identities for the twistedq-Euler numbers and polynomials of higher order. From2.3, we can derive that

Rmq w1, w2:ζ

w

1−1

i0

−1iqw2iζw2i

k0

Emk,ζw1,qw1

w2

w1iw2x

w1ktk k!

l0

El,ζm−1w2,qw2

w1y w2ltl

l!

n0

n

k0

n k

w1kwn−k2 En−k,ζm−1w2,qw2

w1yw1−1

i0

−1iζw2iqw2iEmk,ζw1,qw1

w2xw2

w1i tn

n!. 2.12

From the symmetry ofRmq w1, w2:ζinw1andw2, we see that

Rmq w1, w2:ζ

n0

n

k0

n k

wk2w1n−kEm−1n−k,ζw1,qw1

w2yw2−1

i0

−1iζw1iqw1iEk,ζmw2,qw2

w1xw1

w2i tn

n!. 2.13 Comparing the coefficients on the both sides of2.12and 2.13, we obtain the following theorem which shows the relationship between the power sums and the twisted q-Euler polynomials.

Theorem 2.4. Letw1, w2 ∈Nwithw1 ≡1mod 2andw2 ≡1mod 2.Forn∈Z andm∈N, we have

n k0

n k

wk1wn−k2 Em−1n−k,ζw2,qw2

w1yw1−1

i0

−1iζw2iqw2iEmk,ζw1,qw1

w2x w2

w1i

n

k0

n k

wk2w1n−kEn−k,ζm−1w1,qw1

w2yw2−1

i0

−1iζw1iqw1iEmk,ζw2,qw2

w1xw1

w2i

.

2.14

Remark 2.5. Letm1 andy0 in Theorem 2.Then it follows that

n k0

n k

wk1w2n−k

w1−1 i0

−1iζw2iqw2iEk,ζw1,qw1

w2xw2

w1i

n

k0

n k

wk2w1n−k

w2−1 i0

−1iζw1iqw1iEk,ζw2,qw2

w1xw1

w2i

.

2.15

Moreover, if we takex0 andy0 inTheorem 2.4, then we have the following identity for the twistedq-Euler numbers of higher order.

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Corollary 2.6. Letw1, w2 ∈Nwithw1 ≡1mod 2, w2 ≡ 1mod 2.Forn∈Z andm∈N,we have

n k0

n k

w1kwn−k2 Em−1n−k,ζw2,qw2 w1−1

i0

−1iζw2iqw2iEmk,ζw1,qw1

w2

w1i

n

k0

n k

wk2w1n−kEm−1n−k,ζw1,qw1 w2−1

i0

−1iζw1iqw1iEmk,ζw2,qw2

w1

w2i

.

2.16

If we takem1 inCorollary 2.3, we derive the following identity for the twistedq-Euler polynomials:

forw1, w2∈Nwithw1≡1mod 2, w2≡1mod 2,andn∈Z,

n k0

n k

w1kwn−k2

w1−1 i0

−1iζw2iqw2iEk,ζw1,qw1

w2

w1i

n

k0

n k

w2kwn−k1

w2−1 i0

−1iζw1iqw1iEk,ζw2,qw2

w1

w2i

.

2.17

Remark 2.7. Ifq1,we can observe the result of15.

References

1 T. Kim, “q-Bernoulli numbers and polynomials associated with Gaussian binomial coefficients,”

Russian Journal of Mathematical Physics, vol. 15, no. 1, pp. 51–57, 2008.

2 T. Kim, J. Y. Choi, and J. Y. Sug, “Extended q-Euler numbers and polynomials associated with fermionicp-adicq-integral onZp,” Russian Journal of Mathematical Physics, vol. 14, no. 2, pp. 160–163, 2007.

3 T. Kim, “Symmetry of power sum polynomials and multivariate fermionicp-adic invariant integral onZp,” Russian Journal of Mathematical Physics, vol. 16, no. 1, pp. 93–96, 2009.

4 T. Kim, “Onp -adic interpolating function for q-Euler numbers and its derivatives,” Journal of Mathematical Analysis and Applications, vol. 339, no. 1, pp. 598–608, 2008.

5 R. P. Agarwal and C. S. Ryoo, “Numerical computations of the roots of the generalized twistedq- Bernoulli polynomials,” Neural, Parallel & Scientific Computations, vol. 15, no. 2, pp. 193–206, 2007.

6 M. Cenkci, M. Can, and V. Kurt, “p-adic interpolation functions and Kummer-type congruences for q-twisted andq-generalized twisted Euler numbers,” Advanced Studies in Contemporary Mathematics, vol. 9, no. 2, pp. 203–216, 2004.

7 F. T. Howard, “Applications of a recurrence for the Bernoulli numbers,” Journal of Number Theory, vol.

52, no. 1, pp. 157–172, 1995.

8 B. A. Kupershmidt, “Reflection symmetries of q-Bernoulli polynomials,” Journal of Nonlinear Mathematical Physics, vol. 12, supplement 1, pp. 412–422, 2005.

9 H. Ozden and Y. Simsek, “Interpolation function of theh, q-extension of twisted Euler numbers,”

Computers & Mathematics with Applications, vol. 56, no. 4, pp. 898–908, 2008.

10 L.-C. Jang, “A study on the distribution of twisted q-Genocchi polynomials,” Advanced Studies in Contemporary Mathematics, vol. 18, no. 2, pp. 181–189, 2009.

11 M. Schork, “Ward’s “calculus of sequences”, q-calculus and the limitq1,” Advanced Studies in Contemporary Mathematics, vol. 13, no. 2, pp. 131–141, 2006.

12 H. J. H. Tuenter, “A symmetry of power sum polynomials and Bernoulli numbers,” The American Mathematical Monthly, vol. 108, no. 3, pp. 258–261, 2001.

13 T. Kim, “Note on the Eulerq-zeta functions,” Journal of Number Theory, vol. 129, no. 7, pp. 1798–1804, 2009.

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14 T. Kim, “Symmetryp-adic invariant integral onZpfor Bernoulli and Euler polynomials,” Journal of Difference Equations and Applications, vol. 14, no. 12, pp. 1267–1277, 2008.

15 T. Kim, K. H. Park, and K.-W. Hwang, “On the identities of symmetry for theζ-Euler polynomials of higher order,” Advances in Difference Equations, vol. 2009, Article ID 273545, 9 pages, 2009.

16 T. Kim, “Note on the Euler numbers and polynomials,” Advanced Studies in Contemporary Mathematics, vol. 17, no. 2, pp. 131–136, 2008.

17 T. Kim, “Note on q-Genocchi numbers and polynomials,” Advanced Studies in Contemporary Mathematics, vol. 17, no. 1, pp. 9–15, 2008.

18 T. Kim, “The modified q-Euler numbers and polynomials,” Advanced Studies in Contemporary Mathematics, vol. 16, no. 2, pp. 161–170, 2008.

19 T. Kim, “On aq-analogue of thep-adic log gamma functions and related integrals,” Journal of Number Theory, vol. 76, no. 2, pp. 320–329, 1999.

20 T. Kim, “q-Volkenborn integration,” Russian Journal of Mathematical Physics, vol. 9, no. 3, pp. 288–299, 2002.

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