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Volume 2010, Article ID 358986,13pages doi:10.1155/2010/358986

Research Article

On Carlitz’s Type q-Euler Numbers Associated with the Fermionic P -Adic Integral on Z

p

Min-Soo Kim,

1

Taekyun Kim,

2

and Cheon-Seoung Ryoo

3

1Department of Mathematics, Korea Advanced Institute of Science and Technology, 373-1 Guseong-dong, Yuseong-Gu, Daejeon 305-701, Republic of Korea

2Division of General Education-Mathematics, Kwangwoon University, Seoul 139-701, Republic of Korea

3Department of Mathematics, Hannam University, Daejeon 306-791, Republic of Korea

Correspondence should be addressed to Taekyun Kim,[email protected] Received 2 August 2010; Accepted 28 September 2010

Academic Editor: Jewgeni Dshalalow

Copyrightq2010 Min-Soo Kim 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.

We consider the following problem in the paper of Kim et al.2010: “Find Witt’s formula for Carlitz’s typeq-Euler numbers.” We give Witt’s formula for Carlitz’s typeq-Euler numbers, which is an answer to the above problem. Moreover, we obtain a new p-adic q-l-functionlp,qs, χfor Dirichlet’s characterχ, with the property thatlp,q−n, χ En,χn,qχnppnqEn,χn,qpforn0,1, . . . using the fermionic p-adic integral onZp.

1. Introduction

Throughout this paper, letpbe an odd prime number. The symbol,Zp,Qp,andCpdenote the rings ofp-adic integers, the field ofp-adic numbers, and the field ofp-adic completion of the algebraic closure ofQp,respectively. The p-adic absolute value inCpis normalized in such way that|p|pp−1.LetNbe the set of natural numbers andZN∪ {0}.

As the definition ofq-number, we use the following notations:

xq 1−qx

1−q, x−q 1−

−qx

1q . 1.1

Note that limq1xqxforx∈Zp,whereqtends to 1 in the region 0<|q−1|p<1.

When one talks of q-analogue, q is variously considered as an indeterminate, a complex numberq∈C,or ap-adic numberq∈Cp.Ifq1t∈Cp,one normally assumes

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|t|p<1.We will further suppose that ordpt>1/p−1,so thatqxexpxlogqfor|x|p≤1.

Ifq∈C,then we assume that|q|<1.

After Carlitz 1, 2 gave q-extensions of the classical Bernoulli numbers and polynomials, theq-extensions of Bernoulli and Euler numbers and polynomials have been studied by several authors cf. 1–21. The Euler numbers and polynomials have been studied by researchers in the field of number theory, mathematical physics, and so oncf.

1,2,9,11,13–16,22,23. Recently, variousq-extensions of these numbers and polynomials have been studied by many mathematicianscf.6–8,10,12,17,18,20. Also, some authors have studied in the several area ofq-theorycf.3,4,16,19,24.

It is known that the generating function of Euler numbersFtis given by

Ft 2

et1

n0

Entn

n!. 1.2

From1.2, we know the recurrence formula of Euler numbers is given by

E01, E1nEn0 ifn >0, 1.3

with the usual convention of replacingEnbyEnsee7,18.

In17, theq-extension of Euler numbersEn,qare defined as

E0,q1,

qE1n

En,q

⎧⎨

2 ifn0,

0 ifn >0, 1.4

with the usual convention of replacingEnbyEn,q.

As the same motivation of the construction in18, Carlitz’s typeq-Euler numbersEn,q

are defined as

E0,q 2

2q, q

qE1n

En,q

⎧⎨

2 ifn0,

0 ifn >0, 1.5

with the usual convention of replacingEnbyEn,q.It was shown that limq1En,q En,where En is thenth Euler number. In the complex case, the generating function of Carlitz’s type q-Euler numbersFqtis given by

Fqt

n0

En,qtn n! 2

n0

−qn

enqt, 1.6

whereqis a complex number with|q|< 1see18. The remark point is that the series on the right-hand side of1.6is uniformly convergent in the wider sense. Inp-adic case, Kim et al.18could not determine the generating function of Carlitz’s typeq-Euler numbers and Witt’s formula for Carlitz’s typeq-Euler numbers.

In this paper, we obtain the generating function of Carlitz’s type q-Euler numbers in thep-adic case. Also, we give Witt’s formula for Carlitz’s typeq-Euler numbers, which

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is a partial answer to the problem in 18. Moreover, we obtain a new p-adicq-l-function lp,qs, χfor Dirichlet’s characterχ,with the property that

lp,q

−n, χ

En,χn,qχn

p

p nqEn,χn,qp, 1.7

forn∈Zusing the fermionicp-adic integral onZp.

2. Carlitz’s Type q -Euler Numbers in the p -Adic Case

Let UDZp be the space of uniformly differentiable functions on Zp. Then, the p-adic q- integral of a functionf∈UDZponZpis defined by

Iq

f

Zp

fadμqa lim

N→ ∞

1 pN q

pN−1 a0

faqa, 2.1

cf.5–17,19,20,22. The bosonicp-adic integral onZpis considered as the limitq → 1,that is,

I1

f

Zp

fadμ1a. 2.2

From2.1, we have the fermionicp-adic integral onZpas follows:

I−1 f

lim

q→ −1Iq

f

Zp

fadμ−1a. 2.3

Using2.3, we can readily derive the classical Euler polynomials,Enx,namely

2

Zp

exyt−1 y

2ext et1

n0

Enxtn

n!. 2.4

In particular, whenx0, En0 Enis the well-known the Euler numberscf.7,16,19.

By definition ofI−1f,we show that

I−1 f1

I−1 f

2f0, 2.5

wheref1x fx1 see7. By2.5and induction, we obtain

I−1 fn

−1n−1I−1 f

2 n−1

i0

−1n−i−1fi, 2.6

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wheren1,2, . . .andfnx fxn.From2.6, we note that

I−1 fn

I−1 f

2 n−1

i0

−1ifi ifnis odd

I−1 fn

I−1 f

2 n−1

i0

−1i1fi ifnis even.

2.7

Forx∈Zpand any integeri≥0,we define x

i

⎧⎪

⎪⎩

xx−1· · ·x−i1

i! ifi≥1,

1, ifi0.

2.8

It is easy to see thatxi∈Zpsee23, page 172. We putx ∈Cpwith ordpx > 1/p−1 and|1−q|p<1.We defineqxforx∈Zpby

qx

i0

x i

q−1i

, xq

i1

x i

q−1i−1

. 2.9

If we setfx qxin2.7, we have

I−1 qx

2 qn1

n−1

i0

−1iqi 2

q1 if nis odd

I−1 qx

2 qn−1

n−1

i0

−1i1qi 2

q1 ifnis even.

2.10

From2.10, we note that iffx qx,then I−1qx 2/q1,hence there is no need to consider bothodd and evencases. Thus, for eachl ∈ N,we obtainI−1qlx 2/ql1.

Therefore, we have

I−1

qxxnq 1

1−qn

n l0

n l

−1lI−1

ql1x

1 1−qn

n l0

n l

−1l 2 ql11.

2.11

Also, iffx qlxin2.5, then

I−1 qlx1

I−1 qlx

2f0 2. 2.12

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On the other hand, by2.12, we obtain that

I−1

qx1x1nq I−1

qxxnq 1

1−qnn

l0

n l

−1l

I−1

ql1x1

I−1

ql1x

2 1−qnn

l0

n l

−1l0

2.13

is equivalent to

0I−1

qx1x1nq I−1

qxxnq qI−1

qx

1qxn I−1

qxxnq qI−1

qx

n l0

n l

qlxl

I−1

qxxnq

q n

l0

n l

qlI−1

qxxl

I−1

qxxnq .

2.14

From the definition of fermionicp-adic integral onZpand2.11, we can derive

I−1

qxxnq

Zp

xnqqx−1x

lim

N→ ∞ pN−1

a0

1

1−qnn

i0

n i

−1iqia

−qa 1

1−qnn

i0

n i

−1i lim

N→ ∞ pN−1

a0

−1a qi1a

1 1−qnn

i0

n i

−1i 2 1qi1

2.15

is equivalent to n0

I−1

qxxnqtn n!

n0

1

1−qnn

i0

n i

−1i 2 1qi1

tn n!

2 n0

−qn enqt.

2.16

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From2.12,2.13,2.14,2.15, and2.16, it is easy to show that

q n

l0

n l

qlEl,qEn,q

⎧⎨

2 ifn0,

0 ifn >0, 2.17

whereEn,qare Carlitz’s typeq-Euler numbers defined bysee18

Fqt 2 n0

−qn

enqt

n0

En,qtn

n!. 2.18

Therefore, we obtain the recurrence formula for the Carlitz’s typeq-Euler numbers as follows:

q

qE1n

En,q

⎧⎨

2 ifn0,

0 ifn >0, 2.19

with the usual convention of replacingEnbyEn,q.Therefore, by2.16,2.18, and2.19, we obtain the following theorem, which is a partial answer to the problem in18.

Theorem 2.1Witt’s formula forEn,q. Forn∈Z, En,q 1

1−qnn

i0

n i

−1i 2 1qi1

Zp

xnqqx−1x. 2.20 Carlitz’s typeq-Euler numbersEnEn,qcan be determined inductively by

q

qE1n

En,q

⎧⎨

2 ifn0,

0 ifn >0, 2.21

with the usual convention of replacingEnbyEn,q.

Carlitz type q-Euler polynomials En,qx are defined by means of the generating functionFqx, tas follows:

Fqx, t 2 k0

−1kqkekxqt

n0

En,qxtn

n!. 2.22

In the casesx0, En,q0 En,qwill be called Carlitz typeq-Euler numberscf.8,19. One also can see that the generating functionsFqx, tare determined as solutions of

Fqx, t 2exqtqetFq

x, qt

. 2.23

From2.22, one gets the following.

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Lemma 2.2. 1Fqx, t 2et/1−q

j01/q−1jqxj1/1qj1tj/j!.

2En,qx 2

k0−1kqkkxnq.

It is clear from1and2of Lemma2.2that

En,qx 2 1−qnn

k0

n k

−1k 1qk1qxk,

m−1

k0

−1kqkkxnq

k0

−1kqkkxnq

k0

−1kmqkmkmxnq 1

2

En,qx −1m1qmEn,qxm .

2.24

From2.24, we may state the following.

Proposition 2.3. Ifm∈Nandn∈Z,then (1)En,qx 2/1−qnn

k0nk−1k/1qk1qxk, (2)m−1

k0−1kqkkxnq 1/2En,qx −1m1qmEn,qxm.

Proposition 2.4. Forn∈Z,the value of

Zpxynqqy−1yisn! times the coefficient oftnin the formal expansion of 2

k0−1kqkekxqtin powers oft.That is,En,qx

Zpxynqqy−1y.

Proof. From2.3, we have

Zp

qkxyqy−1 y

qxk lim

N→ ∞ pN−1

a0

−qk1a

2qxk

1qk1, 2.25

which leads to

Zp

xy nqqy−1 y

2 n k0

n k

1

1−qn−1k

Zp

qkxyqy−1 y

2 1−qnn

k0

n k

−1k 1qk1qxk.

2.26

The result now follows by using1of Proposition2.3.

Corollary 2.5. Ifn∈Z,then

En,qx n

k0

n k

xn−kq qkxEk,q. 2.27

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Letd∈Nwithd≡1mod 2andpbe a fixed odd prime number. One sets

Xlim

N

Z dpNZ

, X

0<a<dp

a,p1

adpZp,

adpNZp

xX|xa

moddpN ,

2.28

wherea∈ Zwith 0 ≤ a < dpNcf. 7,9. Note that the natural mapZ/dpNZ → Z/pNZ induces

π:X−→Zp. 2.29

Hereafter, iffis a function onZp,one denotes by the samefthe functionfπonX.Namely one considersfas a function onX.

Let χ be the Dirichlet character with an odd conductor d dχ ∈ N. Then, the generalized Carlitz typeq-Euler polynomials attached toχare defined by

En,χ,qx

X

χa

xy nqqy−1 y

, 2.30

wheren∈Zandx∈Zp.Then, one has the generating function of generalized Carlitz type q-Euler polynomials attached toχ

Fq,χx, t 2 m0

χm−1mqmemxqt

n0

En,χ,qxtn

n!. 2.31

Now, fixed anyt∈Cpwith ordpt>1/p−1and|1−q|p<1.From2.31, one has

Fq,χx, t 2 m0

χm

−qm

n0

1 1−qn

n i0

n i

−1iqimxtn n!

2 n0

1

1−qnn

i0

n i

−1iqix

×d−1

j0

l0

χ

jdl

−qjdl

qijdltn n!

2 n0

1

1−qnd−1

j0

χ j

−qjn i0

n i

−1i qixj 1qdi1

tn n!,

2.32

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wherex∈Zpandd∈Nwithd≡1mod 2.By2.31and2.32, one can derive

En,χ,qx 1

1−qn

d−1 j0

χ j

−qjn

i0

n i

−1iqixj 2 1qdi1

1 1−qnd−1

j0

χ j

−qjn

i0

n i

−1iqixj× lim

N→ ∞ pN−1

l0

−1l qdi1l

lim

N→ ∞ d−1

j0 pN−1

l0

χ

jdl 1 1−qn

n i0

n i

−1iqijdlx×−1jdlqjdl

lim

N→ ∞ dpN−1

a0

χa 1

1−qnn

i0

n i

−1iqiax

−qa

X

χ y

xy nqqy−1 y

,

2.33

wherex∈Zpandd∈Nwithd≡1mod 2.Therefore, one obtains the following.

Theorem 2.6.

En,χ,qx 1

1−qnd−1

j0

χ j

−qjn i0

n i

−1iqixj 2

1qdi1, 2.34

wheren∈Zandx∈Zp.

Letωdenote the Teichm ¨uller character modp.ForxX,one sets

x xqω−1x xq

ωx. 2.35

Note that since|x −1|p< p−1/p−1,xsis defined by expslogpxfor|s|p ≤1cf.10,12, 21. One notes thatxsis analytic fors∈Zp.

One defines an interpolation function for Carlitz typeq-Euler numbers. Fors∈Zp,

lp,q

s, χ

X

x−sχxqx−1x. 2.36

Then,lp,qs, χis analytic fors∈Zp.

The values of this function at nonpositive integers are given by the following.

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Theorem 2.7. For integersn≥0,

lp,q

−n, χ

En,χn,qχn

p

p nqEn,χn,qp, 2.37

whereχnχω−n.In particular, ifχωn,thenlp,q−n, ωn En,q−pnqEn,qp. Proof.

lp,q

−n, χ

X

xnχxqx−1x

X

xnqχnxqx−1x−

X

px nqχn

px

qpx−1 px

X

xnqχnxqx−1x− p nqχn

p

X

xnqpχnxqpx−1x.

2.38

Therefore by2.30, the theorem is proved.

Letχbe the Dirichlet character with an odd conductorddχ ∈N.LetFbe a positive integer multiple ofpandd.Then, by2.22and2.31, we have

Fq,χx, t 2 m0

χm−1mqmemxqt 2

F−1

a0

χa

−qa

k0

−qFk

eFqkxa/FqFt

n0

FnqF−1

a0

χa

−qa En,qF

xa F

tn n!.

2.39

Therefore, we obtain the following

En,χ,qx FnqF−1

a0

χa

−qa En,qF

xa F

. 2.40

Ifχnp/0,thenp, dχn 1,so thatF/pis a multiple ofdχn.From2.40, we derive

χn

p

p nqEn,χn,qp χn

p p nq

F p

n qp

F/p−1

a0

χna

−qpa

En,qpF/p a

F/p

FnqF

a0p|a

χna

−qa En,qF

a F

.

2.41

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Thus, we have

En,χn,qχn

p

p nqEn,χn,qp Fnq F−1

a0pa

χna

−qa En,qF

a F

. 2.42

By Corollary2.5, we easily see that

En,qF

a F

n

k0

n k

a F

n−k

qF qkaEk,qF

F−nq anqn

k0

n k

F a

k

qa

qkaEk,qF.

2.43

From2.42and2.43, we have

En,χn,qχn

p

p nqEn,χn,qp Fnq F−1

a0pa

χna

−qa En,qF

a F

F−1

a0pa

χaan

−qa

k0

n k

F a

k qa

qkaEk,qF,

2.44

sinceχna χaω−na.From Theorem2.7and2.44, we have

lp,q

−n, χ F−1

a0pa

χaan

−qa k0

n k

F a

k

qa

qkaEk,qF, 2.45

forn∈Z.Therefore, we have the following theorem.

Theorem 2.8. LetFbe a positive integer multiple ofpandddχ,and let lp,q

s, χ

X

x−sχxqx−1x, s∈Zp. 2.46 Then,lp,qs, χis analytic fors∈Zpand

lp,q

s, χ F−1

a0pa

χaa−s

−qa k0

−s k

F a

k

qa

qkaEk,qF. 2.47

Furthermore, forn∈Z

lp,q

−n, χ

En,χn,qχn

p

p nqEn,χn,qp. 2.48

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Acknowledgments

The first author was supported by the Basic Science Research Program through the National Research Foundation of Korea NRF funded by the Ministry of Education, Science, and Technology 2010-0001654. The second author was supported by the research grant of Kwangwoon University in 2010.

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2 L. Carlitz, “q-Bernoulli and Eulerian numbers,” Transactions of the American Mathematical Society, vol.

76, pp. 332–350, 1954.

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10 T. Kim, “On p-adic q-l-functions and sums of powers,” Journal of Mathematical Analysis and Applications, vol. 329, no. 2, pp. 1472–1481, 2007.

11 T. Kim, “On the multiple q-Genocchi and Euler numbers,” Russian Journal of Mathematical Physics, vol.

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13 T. Kim, “On a p-adic interpolation function for the q-extension of the generalized Bernoulli polynomials and its derivative,” Discrete Mathematics, vol. 309, no. 6, pp. 1593–1602, 2009.

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19 H. Ozden, I. N. Cangul, and Y. Simsek, “Multivariate interpolation functions of higher-order q-Euler numbers and their applications,” Abstract and Applied Analysis, vol. 2008, Article ID 390857, 16 pages, 2008.

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23 A. M. Robert, A Course in p-Adic Analysis, vol. 198 of Graduate Texts in Mathematics, Springer, New York, NY, USA, 2000.

24 N. K. Govil and V. Gupta, “Convergence of q-Meyer-K ¨onig-Zeller-Durrmeyer operators,” Advanced Studies in Contemporary Mathematics, vol. 19, no. 1, pp. 97–108, 2009.

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