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
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
x∈X |x≡a
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 writef ∈ UDZp, if the difference quotients, Ffx, y fx−fy/x−yhave a limitfaas x, y → a, a.
Forf∈UDZp, 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
forf ∈UDZp. Forf ∈UDZp, 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. Forf ∈UDZp,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. Forξ∈Tp, we denote byφξ :Zp → Cpdefined by φξx ξx, the locally constant function. If we takefx ξxext, then we havecf.35
En,ξ
Zp
xnξndμ−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
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
Letξ∈Tp. 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−1yxynqdμ−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−1yφξyxynqdμ−qy. 2.11
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−1yξyxynqdμ−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,qd,ξd
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
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≤a≤dandn0,1,2, . . .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,qd,ξd
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.
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,1d,ξd
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,1d,ξd
−n,ax d
dnq 1q
1qd d a1
χa−1aqhaξaEh,1n,qd,ξd
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,qd,ξd
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
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 1q1−qs∞
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,qd,ξd
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,1d,ξd
−n,ax d
dnq 1q
1qd d a1
χa−1aqhaξaEh,1n,qd,ξd
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.
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,qF,ξF
s,ax
F
.
3.20
By substituting3.2, fors−n, we get
HE,q,ξh,1s, a, x|F Fnq−1aqhaξa 1qF Eh,1n,qF,ξF
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< x≤1, 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,qF,ξF
ax F
.
3.23
From2.12, if we takes0, then we have the following corollary.
Corollary 3.11. Fors∈C, ξr 1 withξ /1, letχbe the Dirichlet’s character with conductord∈N withd≡1 mod 2andx∈R,0< x≤1,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 subsetDofC∗pbycf.62
D{s∈Cp:|s|p≤p1−1/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,j → an,0asj → ∞for alln, jand
2for eachs∈Dandε >0, there existsn0n0s, εsuch that
n≥n0
an,jsn p
< ε, for∀j. 4.4
Then limj→ ∞Ajs A0sfor alls∈Dcf.2,22,50,51,60,62.
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,qF,ξFqjapt F
apt j
qapt
.
4.5
ThenLh,1E,p,q,ξs, x:χis analytic fort∈Cpwith|t|p ≤1, whens∈D. Fort∈Cpwith|t|p ≤1, we have
∞ j0
−s j
Ej,qh,1F,ξFqjapt F
apt j
qapt
4.6
is analytic fors∈D. It readily follows that
aptsω−saaptsqas∞
m0
s
m qaa−1q ptqm
4.7
is analytic fors∈Cpwith|t|p≤1 whens∈D. Thus we see that
Lh,1E,p,q,ξ0, x:χ 1q 2
F a1
−1aχnaξa. 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,qF,ξF
apt F
. 4.9
Ifχnp/0, thenp, dχn 1, soF/pis a multiple ofdχn. Therefore, we have χnppnqEh,1n,qF,ξF,χnt
χnppnq F p
n
qp
1qp 1qpF/p
F/p−1
a0
χna−1aξaEh,1n,qpF/p,ξpF/p
at F/p
Fnq1qp 1qF
F a0pa
χna−1aξaEh,1n,qF,ξF
apt F
.
4.10
Then we note that 1q
1qpχnppnqEn,qh,1F,ξF,χnt 1q
1qFFnqF
a0p|a
χna−1aξaEn,qh,1F,ξF
apt F
. 4.11
The difference of these equations yields
Eh,1n,q,ξ,χ
npt− 1q
1qpχnppnqEh,1n,qF,ξF,χnt 1q
1qFFnqF
a0pa
χna−1aξaEh,1n,qF,ξF
apt F
. 4.12
Using distribution forh, q-Euler polynomials, we easily see that
En,qh,1F,ξF
apt F
F−nq aptnqn
k0
n k
qaptkξa F
apt k
qapt
Eh,1k,qF,ξF. 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,1F,ξF,χnt 1q
1qF
F−1
a0
χna−1aξaEn,qh,1F,ξF
apt F
1q 1qp
F−1
a0,pa
χna−1aξaaptnn
k0
n k
qaptk F
apt k
qapt
Ek,qh,1F,ξF.
4.14
From4.5–4.14, we can derive that
Eh,1n,q,ξ,χnpt− 1q
1qpχnppnqEh,1n,qp,ξp,χnt 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,qF,ξF. 4.16
ThenLh,1E,p,q,ξs, t : χis analytic for t ∈ Cp,|t|p ≤ 1, provides s ∈ D 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,1p,ξp,χnt. 4.17
Thus we note thatLh,1E,p,q,ξs,0 : χ Lh,1E,p,q,ξs, χfor alls ∈ D, 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,qF,ξF,
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,qF,ξF
−1a
1qFqhaξaω−naFnqEn,qF,ξF
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, whens ∈ D. 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
Thep-adic logarithmic function, logp, is the unique functionC∗p → Cpthat satisfies
logp1x ∞
n1
−1n
n xn, |x|p<1, logpxy logpx logpy, ∀x, y∈C∗p,
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,qF,ξF.
4.23
Thus, we have
∂
∂sLh,1E,p,q,ξs, t:χ|s0 1q 1qF
F a1,pa
χa−1aξa
·
−logaptE0,qh,1F,ξF∞
m1
−1m m qaptm
F apt
m qapt
Eh,1m,qF,ξF
. 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,qF,ξF
−1q 2
F a1pa
χa−1aξalogapt.
4.26
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