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Volume 2009, Article ID 946569,17pages doi:10.1155/2009/946569

Research Article

On Interpolation Functions of the Generalized Twisted h, q -Euler Polynomials

Kyoung Ho Park

Department of Mathematics, Sogang University, Seoul 121-742, South Korea

Correspondence should be addressed to Kyoung Ho Park,[email protected] Received 5 November 2008; Accepted 14 January 2009

Recommended by Vijay Gupta

The aim of this paper is to constructp-adic twisted two-variable Euler-h,q-L-functions, which interpolate generalized twistedh,q-Euler polynomials at negative integers. In this paper, we treat twistedh,q-Euler numbers and polynomials associated withp-adic invariant integral onZp. We will construct two-variable twistedh,q-Euler-zeta function and two-variableh,q-L-function in Complexs-plane.

Copyrightq2009 Kyoung Ho Park. 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.

1. Introduction

Tsumura and Young treated the interpolation functions of the Bernoulli and Euler polynomials in 1,2. Kim and Simsek studied onp-adic interpolation functions of these numbers and polynomials3–48. In49, Carlitz originally constructedq-Bernoulli numbers and polynomials. Many authors studied these numbers and polynomials 4, 28, 38, 41, 50. After that, twistedh, q-Bernoulli and Euler numberspolynomials were studied by several authors 1–32, 32–65. In 62, Whashington constructed one-variable p-adic-L- function which interpolates generalized classical Bernoulli numbers at negative integers.

Fox introduced the two-variable p-adi L-functions 53. Young defined p-adic integral representation for the two-variable p-adicL-functions64. Furthermore, Kim constructed the two-variable p-adic q-L-function, which is interpolation function of the generalized q-Bernoulli polynomials 8. This function is the q-extension of the two-variable p-adic L-function. Kim constructed q-extension of the generalized formula for two-variable of Diamond and Ferrero and Greenberg formula for two-variablep-adicL-function in the terms of thep-adic gamma and log-gamma functions8. Kim and Rim introduced twistedq-Euler numbers and polynomials associated with basic twistedq--functions28. Also, Jang et al.

investigated thep-adic analogue twistedq--function, which interpolates generalized twisted

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q-Euler numbers En,q,ξ,χ attached to Dirichlet’s character χ 55. Kim et al. have studied two-variablep-adicL-functions, which interpolate the generalized Bernoulli polynomials at negative integers. In this paper, we will construct two-variale p-adic twisted Euler h, q- L-functions. This functions interpolation functions of the generalized twisted h, q-Euler polynomials.

Let p be a fixed odd prime number. Throughout this paper Z,Zp,Qp and Cp will respectively denote the ring of rational integers, the ring ofp-adic rational integers, the field ofp-adic rational numbers and the completion of the algebraic closure ofQp. Letvp be the normalized exponential valuation ofCp such that|p|p p−vpp p−1. Ifs ∈ C, then|q| <1.

If q ∈ Cp, we normally assume |1 −q|p < p−1/p−1, so that qx explogq for|x|p ≤ 1.

Throughout this paper we use the following notationscf.1–32,32–48,50,51,54–65:

xq x:q 1−qx

1−q, x−q 1−−qx

1q . 1.1

Hence, limq→1xqx, for anyxwith|x|p≤1 in the presentp-adic case.

Forda fixed positive integer withp, d 1, set

X Xd lim

N

Z

dpNZ, X1Zp,

X

0<a<dp, a,p1

adpZp

,

adpNZp

xX |xa

mod dpN ,

1.2

wherea∈Zsatisfies the condition 0≤a < dpN. The distribution is defined by

μq

adpNZp

qa

dpNq. 1.3 We say thatf is uniformly differential function at a pointa∈ Zp, and we writefUDZp, if the difference quotients, Ffx, y fx−fy/xyhave a limitfaas x, y → a, a.

ForfUDZp, thep-adic invariantq-integral onZpis defined as4,18

Iqf

Zp

fxdμqx lim

N→ ∞

1 pNq

pN−1 x0

fxqx. 1.4

The fermionicp-adicq-measures onZpis defined ascf.14–16,18,22,28

μ−q

adpNZp

−qa

dpN−q, 1.5

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forfUDZp. ForfUDZp, the ferminoicp-adic invariantq-integral onZpis defined as

I−qf

Zp

fxdμ−qx lim

N→ ∞

1 pN−q

pN−1 x0

fx−qx, 1.6

which has a sense as we see readily that the limit is convergent. ForfUDZp,Cp, we note thatcf.14,16,18,22,28

Zp

fxdμ−1x

X

fxdμ−1x. 1.7

From the fermionic invariant integral onZp, we derive the following integral equation cf.14,35:

I−1 f1

I−1f 2f0, 1.8

wheref1x fx1.

2. Twisted h, q-Euler Numbers and Polynomials

In this section, we will treat some properties of twistedh, q-Euler numbers and polynomials associated withp-adic invariant integral onZp. From now on, we takeh∈Zandq∈Cpwith

|q−1|p< p−1/p−1. LetCpn be the space of primitivepnth root of unity, Cpn

w∈Cpn |wpn 1

. 2.1

Then, we denote

Tp lim

n→ ∞Cpn

n≥0

Cpn. 2.2

HenceTpis ap-adic locally constant space. ForξTp, we denote byφξ :Zp → Cpdefined by φξx ξx, the locally constant function. If we takefx ξxext, then we havecf.35

En,ξ

Zp

xnξn−1x. 2.3

By induction in1.8, Kim constructed the following useful identitycf.14,28:

I−1 fn

−1n−1I−1f 2

n−1

0

−1n−1−f, 2.4

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wheren∈N, fnfxn. From2.4, ifnis odd, then we have

I−1 fn

I−1f 2 n−1 0

−1f. 2.5

If we replacenbydoddinto2.5, we obtain

I−1 fd

I−1f 2

d−1

0

−1f. 2.6

LetξTp. Letχbe a Dirichlet’s character of conductord, whichdis any multiple ofp withp≡1mod 2. By substitutingfx χxξxextinto2.6, we have

I−1

χxξxext

n0

En,ξ,χtn

n!. 2.7

Remark 2.1. In complex case, the generating function of the Euler numbersEn,ξ,χ is given by cf.28

2 d−10−1χξet ξdedt1

n0

En,ξ,χtn

n!, |t|< π

d. 2.8

By using Taylor series ofext, then we can define the generalized twisted Euler numbersEn,ξ,χ

attached toχas followscf.55:

En,ξ,χ

X

ξnxnχxdμ−1x. 2.9

In8,h, q-Euler numbers were defined by

Eh,1n,q x

Zp

qh−1yxynq−qy, 2.10

whereh∈Zandx∈Zp. In particular, if we takex0, thenEn,qh,10 Eh,1n,q . These numbers are calledh, q-Euler numbers.

By using iterative method ofp-adic invariant integral onZpin the sense of fermionic, we define twistedh, q-Euler numbers as followscf.55:

Eh,1n,q,ξx

Zp

qh−1yφξyxynq−qy. 2.11

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Forh∈Zandn∈N, we have thatcf.55 Eh,1n,q,ξx 1q

1−qn n

i0

n i

−1iqxi 1

1ξqhi, 2.12

En,q,ξh,1x 1q 1qd

d−1

a0

−1aqhaξaEh,1n,ξd,qd

xa d

dnq, 2.13

whered∈Nwithd≡1mod 2.

LetFq,ξh,1t, xbe the generating function ofEn,q,ξh,1xin complex plane as followscf.

55:

Fq,ξh,1t, x 1q

n0

−1nqhnξnetnxq

n0

Eh,1n,q,ξxtn n!.

2.14

Letχbe the Dirichlet’s character with conductord∈Nwithd≡1 mod 2. Then the generalized twistedh, q-Euler polynomials attached toχis given by as follows:

Forn∈ZN∪ {0},

En,q,ξ,χh,1 x

X

χyqh−1yξyxynq−qy, 2.15 whereh∈Z, dis any multiple ofpwithp≡1mod 2andx∈Cp.

Then the distribution relation of the generalized twistedh, q-Euler polynomials is given by as followscf.14:

Eh,1n,q,ξ,χx 1q 1qd

d a1

χa−1aqhaξaEh,1n,qdd

xa d

dnq. 2.16

3. Two-Variable Twisted h, q-Euler-Zeta Function and h, q - L -Function

In this section, we will construct two-variable twisted h, q-Euler-zeta function and two- variableh, q-L-function in Complexs-plane. We assumeq∈Cwith|q|<1.

Firstly, we consider twisted q-Euler numbers and polynomials in C as followscf.

55:

Fq,ξh,1t, x 1q

n0

−1nqhnξnetnxq

n0

Eh,1n,q,ξxtn n!,

3.1

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whereq, x ∈ C, r ∈ Z N∪ {0}andξ isrth root of unity. In particular, if we takex 0, then we haveEh,1n,q,ξ0 Eh,1n,q,ξ. These numbers are called twisted Euler numbers. By using derivative operator, we havedk/dtkFq,ξt, x|t0Eh,1n,q,ξx.

From3.1, we can define Hurwitz-type twistedh, q-Euler-zeta function as follows cf.55:

ζh,1E,q,ξs, x 1q

k0

−1kqhkξk

xksq , 3.2 whereq∈C,|q|<1, s∈C, h∈Zandx∈R,0< x≤1. Note that ifx1 in3.2, then we see that the twistedh, q-Euler-zeta function is defined bycf.28,55

ζh,1E,q,ξs 1q

k1

−1kqhkξk

ksq , s∈C,Res>1. 3.3

Forn∈N, we knowcf.28

ζh,1E,q,ξ−n, x Eh,1n,q,ξx. 3.4

From now on, we will define the two-variableh, q-L-functionsLh,1E,q,ξs, x :χwhich interpolates the generalizedh, q-Euler polynomials.

Definition 3.1. Let χbe the Dirichlet’s character with conductor dwith d ≡ 1 mod 2. For s∈C, h∈Zandx∈R,0< x≤1, we define

Lh,1E,q,ξs, x:χ 1q

n0

χn−1nqhnξn

nxsq . 3.5 By substitutingnajd, d≡1mod 2,1≤adandn0,1,2, . . .into3.5, then using3.2, we have

Lh,1E,q,ξs, x:χ1qd

a1

j0

χajd−1ajdqhajdξajd ajdxsq

1qd

a1

χa−1aqhaξa dsq

j0

−1jdqhjd j ax/dsqd

1q 1qd

d a1

χa−1aqhaξaζh,1E,qdd

s,ax

d

d−sq .

3.6

Thus, we see the functionLh,1E,q,ξs, x:χwhich interpolates the generalizedh, q-Euler polynomials as follows.

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Theorem 3.2. For s ∈ C, h ∈ Z, letχ be the Dirichlet’s character with conductor dwith d ≡ 1mod 2. Then one has

Lh,1E,q,ξs, x:χ 1q 1qd

d a1

χa−1aqhaξaζE,qh,1dd

s,ax

d

d−sq . 3.7

By substitutings−nwithn >0, into3.7, we obtain

Lh,1E,q,ξ−n, x:χ 1q 1qd

d a1

χa−1aqhaξaζE,qh,1dd

n,ax d

dnq 1q

1qd d a1

χa−1aqhaξaEh,1n,qdd

ax d

dnq En,q,ξ,χh,1 x,

3.8

whered≡1 mod 2, d∈N.

Thus, we have the following theorem.

Theorem 3.3. Forn ∈N, letχbe the Dirichlet’s character with conductordwithd ≡ 1mod 2.

Then one has

Lh,1E,q,ξ−n, x:χ Eh,1n,q,ξ,χx. 3.9

Remark 3.4. If we takex1 in3.5, then we havecf.28,55

Lh,1E,q,ξs, χ 1q

n1

χn−1nqhnξn

nsq , fors∈C. 3.10 From3.9and3.10, we have the following corollary.

Corollary 3.5. Letχbe the Dirichlet’s character with conductordwithd ≡ 1mod 2. Then one has

Eh,1n,q,ξ,χx 1q 1qd

d a1

χa−1aqhaξaEh,1n,qdd

ax d

dnq. 3.11

Secondly, we will define two-variable twisted Eulerh, q-L-function as follows.

Definition 3.6. Letχbe the Dirichlet’s character with conductordwithd≡1 mod 2, d∈N.

Fors∈C, h∈Z, x∈R,0< x≤1 andξr 1 withξ /1, we define

Lh,1E,q,ξs, x:χ 1q

k0

χk−1kqhkξk

kxsq . 3.12

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We consider the well-known identitycf.44,65 1

1−xs

j0

sj−1 j

xj. 3.13

By using3.12, we define two-variable twisted Eulerh, q-L-function as follows:

Lh,1E,q,ξs, x:χ 1q1qs

j0

k0

sj−1 j

χk−1kξkqhkjkx. 3.14

We will investigate the relations betweenLh,1E,q,ξs, x:χandLh,1E,q,ξs, χas follows.

Substitutingk ajd, a 1,2, . . . , dwithd ≡1 mod 2, j 0,1,2, . . . ,into3.12, we have

Lh,1E,q,ξs, x:χ 1qd

a1

j0

χajd−1ajdqhajdξajd

ajdxsq , 3.15

Thus we obtain the following theorem.

Theorem 3.7. Fors ∈ Cwithh ∈ Z, letχbe the Dirichlet character with conductordwithd ≡ 1mod 2andx∈R,0< x≤1, ξr 1 withξ /1. Then one has

Lh,1E,q,ξs, x:χ 1q 1qd

d a1

χa−1aqhaξaζh,1E,qdd

s,ax

d

d−sq . 3.16

By substitutings−nwithn∈Ninto3.16and using3.4, we can obtain

Lh,1E,q,ξ−n, x:χ 1q 1qd

d a1

χa−1aqhaξaζE,qh,1dd

n,ax d

dnq 1q

1qd d a1

χa−1aqhaξaEh,1n,qdd

ax d

dnq En,q,ξ,χh,1 x.

3.17

Thus, we see that the functionLh,1E,q,ws, x:χinterpolates generalizedh, q-Euler polynomi- als attached toχat negative integer values ofsas followings.

Theorem 3.8. Forn∈N, letχbe the Dirichlet’s character with odd conductord. Then one has

Lh,1E,q,ξ−n, x:χ Eh,1n,q,ξ,χx. 3.18

Note that if we takex1, thenTheorem 3.8reduces toTheorem 3.3.

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LetaandFbe integers withF≡1mod 2and 0< a < F. Fors∈C, we define partial h, q-Hurwitz type zeta functionHE,q,ξh,1s, a, x|Fas follows:

HE,q,ξh,1s, a, x|F

m≡amodF, m>0

−1mqhmξm

mxsq . 3.19

By substitutingmajF, we have

HE,q,ξh,1s, a, x|F

j0

−1ajFqhajFξajF ajFxsq

−1aqhaξaF−sq

j0

−1jFqFhjξFj ax/F jsqF

F−sq −1aqhaξa 1 1qF

j0

−1jFqFhjξFj ax/F jsqF

F−sq −1aqhaξa 1qF ζh,1E,qFF

s,ax

F

.

3.20

By substituting3.2, fors−n, we get

HE,q,ξh,1s, a, x|F Fnq−1aqhaξa 1qF Eh,1n,qFF

ax F

. 3.21

Equation 3.20 means that the function HE,q,ξh,1s, a, x | F interpolates En,q,ξh,1s, a, x | F polynomials at negative integers.

From3.16and3.20, we have the following theorem.

Theorem 3.9. Fors∈C, ξr 1 withξ /1, letχbe the Dirichlet’s character with conductord∈N withd≡1mod 2andx∈R,0< x1, Fis any multiple ofd. Then one has

Lh,1E,q,ξs, x:χ 1qF

a1

χa−1aHE,q,ξh,1s, a, x|F. 3.22

Remark 3.10. If we takes0 in3.22, then we have

Lh,1E,q,ξ0, x:χ 1qF

a1

χaHE,q,ξh,10, a, x|F 1q

1qF F a1

χa−1aqhaξaEh,10,qFF

ax F

.

3.23

From2.12, if we takes0, then we have the following corollary.

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Corollary 3.11. Fors∈C, ξr 1 withξ /1, letχbe the Dirichlet’s character with conductord∈N withd≡1 mod 2andx∈R,0< x1,Fis any multiple ofd. Then one has

Lh,1E,q,ξ0, x:χ 1q2 1qF1ξqh

F a1

χa−1aqhaξa. 3.24

4. p -Adic Twisted Two-Variable Euler h, q-L-Functions

In 62, Washington constructed one-variable p-adic-L-function which interpolates gen- eralized classical Bernoulli numbers negative integers. Kim 22 investigated the p-adic analogues of two-variables Euler q-L-function. In this section, we will construct p-adic twisted two-variable Euler-h, q-L-functions, which interpolate generalized twisted h, q- Euler polynomials at negative integers. Our notations and methods are essentially due to Kim and Washingtoncf.22,62.

We assume thatq ∈ Cpwith |1−q|p < p−1/p−1, so thatqx expxlogq. Letpbe an odd prime number. Let ωdenote the Teichm ¨uller character having conductorp. For an arbitrary character χ, we define χn χω−n, wheren ∈ Z, in the sense of the product of characters. Let a a : q ω−1aaq aq/ωa. Thena ≡ 1modp11/p−1. Hence we see that

aptω−1aptaptq ω−1aaqω−1aqaptq

≡1

mod p11/p−1

,

4.1

wheret∈Cpwith|t|p≤1,a, p 1.

We denote the subsetDofCpbycf.62

D{s∈Cp:|s|pp1−1/p−1}. 4.2

Let

Ajx

j0

an,jxn, an,j ∈Cp, j0,1,2, . . . , 4.3

be a sequence of power series, each of which converges in a fixed subsetDsuch that 1an,jan,0asj → ∞for alln, jand

2for eachsDandε >0, there existsn0n0s, εsuch that

n≥n0

an,jsn p

< ε, for∀j. 4.4

Then limj→ ∞Ajs A0sfor allsDcf.2,22,50,51,60,62.

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Letχbe the Dirichlet’s character with conductordwithd≡1 mod 2and letF be a positive multiple ofpandd.

Now we set

Lh,1E,p,q,ξs, x:χ 1q 1qF

F a1,pa

χa−1aξaapt−s

·

j0

−s j

Eh,1j,qFFqjapt F

apt j

qapt

.

4.5

ThenLh,1E,p,q,ξs, x:χis analytic fort∈Cpwith|t|p ≤1, whensD. Fort∈Cpwith|t|p ≤1, we have

j0

−s j

Ej,qh,1FFqjapt F

apt j

qapt

4.6

is analytic forsD. It readily follows that

aptsω−saaptsqas

m0

s

m qaa−1q ptqm

4.7

is analytic fors∈Cpwith|t|p≤1 whensD. Thus we see that

Lh,1E,p,q,ξ0, x:χ 1q 2

F a1

−1aχna. 4.8

Letn∈Zand fixedt∈Cpwith|t|p≤1. Then we have that

Eh,1n,q,ξ,χ

npt Fnq 1q 1qF

F a0

χna−1aξaEh,1n,qFF

apt F

. 4.9

Ifχnp/0, thenp, dχn 1, soF/pis a multiple ofdχn. Therefore, we have χnppnqEh,1n,qFFnt

χnppnq F p

n

qp

1qp 1qpF/p

F/p−1

a0

χna−1aξaEh,1n,qpF/ppF/p

at F/p

Fnq1qp 1qF

F a0pa

χna−1aξaEh,1n,qFF

apt F

.

4.10

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Then we note that 1q

1qpχnppnqEn,qh,1FFnt 1q

1qFFnqF

a0p|a

χna−1aξaEn,qh,1FF

apt F

. 4.11

The difference of these equations yields

Eh,1n,q,ξ,χ

npt− 1q

1qpχnppnqEh,1n,qFFnt 1q

1qFFnqF

a0pa

χna−1aξaEh,1n,qFF

apt F

. 4.12

Using distribution forh, q-Euler polynomials, we easily see that

En,qh,1FF

apt F

F−nq aptnqn

k0

n k

qaptkξa F

apt k

qapt

Eh,1k,qFF. 4.13

Sinceχna χaω−na, fora, p 1, andt∈Cp, with|t|p≤1, we have

Eh,1n,q,ξ,χ

npt− 1q

1qpχnppnqEn,qh,1FFnt 1q

1qF

F−1

a0

χna−1aξaEn,qh,1FF

apt F

1q 1qp

F−1

a0,pa

χna−1aξaaptnn

k0

n k

qaptk F

apt k

qapt

Ek,qh,1FF.

4.14

From4.5–4.14, we can derive that

Eh,1n,q,ξ,χnpt− 1q

1qpχnppnqEh,1n,qppnt Lh,1E,p,q,ξ−n, t:χ. 4.15 Therefore we obtain the following theorem.

Theorem 4.1. LetFbe a positive integral multiple ofpandddχwithF≡1mod 2, and let

Lh,1E,p,q,ξs, t:χ 1q 1qd

F a1,pa

χa−1aξaapt−s

m0

−s m

qaptm F

apt m

qapt

Eh,1m,qFF. 4.16

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ThenLh,1E,p,q,ξs, t : χis analytic for t ∈ Cp,|t|p ≤ 1, provides sD when χ 1.

Furthermore, for eachn∈Z, we have

Lh,1E,p,q,ξ−n, t:χ Eh,1n,q,ξ,χnpt− 1q

1qpχnppnqEn,qh,1ppnt. 4.17

Thus we note thatLh,1E,p,q,ξs,0 : χ Lh,1E,p,q,ξs, χfor allsD, whereLh,1E,p,q,ξs, χis twisted p-adic Eulerh, q-L-function,cf.15,22.

We now generalized to two-variable p-adic Euler h, q-L-function, Lh,1E,p,q,ξs, t : χ which is first defined by the interpolation function

HE,p,q,ξh,1 s, a, x|F −1a

1qFqhaξaapt−s

·

j0

−s j

qjapt

Fq aptq

j Eh,1j,qFF,

4.18

fors∈Zp.

From4.18, we have that

HE,p,q,ξh,1 −n, a, x|F −1a

1qFξaqhaaptna

j0

n j

qaptj

Fq aq

j Eh,1j,qFF

−1a

1qFqhaξaω−naFnqEn,qFF

a F

ω−naHE,q,ξh,1−n, a, x|F.

4.19

By using the definition of HE,p,q,ξh,1 s, a, x | F, we can express Lh,1E,p,q,ξs, t : χ for all a ∈ Z,a, p 1 andt∈Cpwith|t| ≤1 as follows:

Lh,1E,p,q,ξs, t:χ F

a1,pa

χaHE,p,q,ξh,1 s, apt|F. 4.20

We know thatHE,p,q,ξh,1 s, apt |Fis analytic fort ∈ Cp,|t| ≤1, whensD. The value of

∂/∂sLh,1E,p,q,ξs, t:χis the coefficients ofsin the expansion ofLh,1E,p,q,ξs, t:χats0. Using the Taylor expansion ats0, we see that

apt−s1−slogapt· · ·,

−s m

−1m

m s· · ·. 4.21

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Thep-adic logarithmic function, logp, is the unique functionCp → Cpthat satisfies

logp1x

n1

−1n

n xn, |x|p<1, logpxy logpx logpy, ∀x, y∈Cp,

logpp 0.

4.22

By employing these expansion and some algebraic manipulations, we evaluate the derivative

∂/∂sLh,1E,p,q,ξ0, t:χ. It follows from the definition ofLE,p,q,ξs, t:χthat

Lh,1E,p,q,ξs, t:χ 1q 1qF

F a1,pa

χa−1aξaapt−s

·

m0

−s m

qaptm F

apt m

qapt

Eh,1m,qFF.

4.23

Thus, we have

∂sLh,1E,p,q,ξs, t:χ|s0 1q 1qF

F a1,pa

χa−1aξa

·

−logaptE0,qh,1FF

m1

−1m m qaptm

F apt

m qapt

Eh,1m,qFF

. 4.24

Sinceωais a root of unity fora, p 1, we have

logpaptlogpapt logpω−1a logpapt. 4.25 Thus we have the following theorem.

Theorem 4.2. Letχbe a primitive Dirichlet’s character with odd conductord, d∈Nand letFbe a odd positive integral multiple ofpandd. Then for anyt∈Cpwith|t| ≤1, one has

∂sLh,1E,p,q,ξs, t:χ 1q 1qF

F a1,pa

χa−1aξa m1

−1m m qaptm

Fq aptq

m

Eh,1m,qFF

−1q 2

F a1pa

χa−1aξalogapt.

4.26

(15)

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