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Zeta Functions of Higher Order and Their Applications (Diophantine Problems and Analytic Number Theory)

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(1)

Zeta

Functions

of Higher Order and Their

Applications

Nobushige

Kurokawa

(Tokyo

Institute of

Technology)

Shin-ya Koyama

(Keio

University)

1

Absolute

Tensor Product

In this note

we

present

our

results

on

multiple zeta functions with

some

applications. This is asurvey of

our

papers [KK1, KK2, KK3, KK4]. We

also refer to [KK5, KK6] for applications

more

recently proved.

Definition 1(regularized product) Let $m(\rho)\in \mathbb{Z}(\rho\in \mathbb{C})$ be the

multi-plicity of

zeros

(or poles) at $s$ $=\rho$ of

some

meromorphic function $Z(s)$

.

We

define the regularized product

as

follows:

$\coprod_{\rho\in \mathbb{C}}(s-\rho)^{m(\rho)}:=\exp(-\frac{\partial}{\partial w}|_{w=0}\sum_{\rho\in \mathrm{C}}\frac{m(\rho)}{(s-\rho)^{w}})$

in

case

the series in the right hand side converges in ${\rm Re}(w)\gg 0$ and has

an

analytic continuation to $w=0$

.

The absolute tensor product is defined

as

folows:

Definition

2(absolute

tensor

product) The absolute tensor product of

zeta functions

$Z_{j}(s)$

$=\coprod_{\rho\in \mathrm{C}}(s-\rho)^{m_{j}(\rho)}$ $(j=1, \ldots, r)$

is defined by

$(Z_{1}\otimes\cdots\otimes Z_{r})(s):=\coprod_{\rho\in \mathrm{C}}(s-(\rho_{1}+\cdots+\rho_{r}))^{m(\rho_{1\prime\cdots\prime}\rho_{r})}$,

数理解析研究所講究録 1319 巻 2003 年 1-13

(2)

$m(\rho_{1}, \ldots,\rho_{r})=m(\rho_{1})\cdots m(\rho_{r})\mathrm{x}\{\begin{array}{l}(-\mathrm{l})^{r-1}1\mathrm{i}\mathrm{f}\mathrm{i}\mathrm{f}\mathrm{I}\mathrm{m}(\rho_{j})\geq 0(\forall j)\mathrm{I}\mathrm{m}(\rho_{j})<0(\forall j)0\mathrm{o}\mathrm{t}\mathrm{h}\mathrm{e}\mathrm{r}\mathrm{w}\mathrm{i}\mathrm{s}\mathrm{e}\end{array}$

For the background and the motivation of this definition, we refer to the

ex-cellent surveyofManin [M], where thetensorproduct is named the Kurokawa

product by him.

We introduce theSelbergzetafunction for aRiemannian manifold. Let $M$

be aRiemannian manifold, and $P$ be the set of prime closed geodesies. The

Selberg zeta function of $M$ is defined

as

follows

as

long

as

$P$ is acountable

set and the following Euler product converges:

Definition 3(Selberg zeta function) We define

$\zeta_{M}(s):=\prod_{p\in P}(1-e^{-l(p)s})^{-1}$,

where $l(p)$ is the length of ageodesic$p$

.

Examples 4Let $M=S^{1}( \frac{l}{2\pi})$ be the circle with radius $\frac{l}{2\pi}$

.

Then $P$ consists

of

one

element which

we

denote by $p$

.

Then

$\zeta_{M}(s)=(1-e^{-l(p)s})^{-1}$

.

Especiallywhen $l(p)=\log q$ with $q$ apower of

some

prime number, it follows

that $\zeta_{M}(s)=(1-q^{-s})^{-1}=\zeta(s,\mathrm{F}_{q})$ which is the Hasse zeta function of the

finite field $\mathrm{F}_{q}$

.

In what folows

we

denote by $p$ either aprime number

or

aprime geodesic.

The

norm

of$p$ is defined by

$N(p)=\{e^{l(p)}p(p.\in P)(p\cdot \mathrm{a}\mathrm{p}\mathrm{r}\mathrm{i}\mathrm{m}\mathrm{e} \mathrm{n}\mathrm{u}\mathrm{m}\mathrm{b}\mathrm{e}\mathrm{r})$

Here

we

introduce the notion of generic for real numbers.

Definition 5(generic) Areal number $\alpha$ is called generic if and only if

$\lim_{marrow\infty}||m\alpha||^{\frac{1}{m}}=1$,

where $||x||:= \min\{|x-n| : n \in \mathbb{Z}\}$ for $x$ $\in \mathrm{R}$

.

(3)

Examples 6

(1) If $\alpha\in \mathbb{Q}$, then $\alpha$ is not generic.

(2) If $\alpha\in(\overline{\mathbb{Q}}\cap \mathbb{R})\backslash \mathbb{Q}$, then $\alpha$ is generic.

(3) Let $x$,$y\in\overline{\mathbb{Q}}\cap \mathrm{R}_{>0}$, $y\neq 1$

.

If $\alpha=\frac{1\mathrm{o}\mathrm{g}x}{1\mathrm{o}\mathrm{g}y}\not\in \mathbb{Q}$, then $\alpha$ is generic.

The last example

was

proved by Baker in his famous work

on

transcendental

numbers. We recall it

as

follows:

Baker’s Theorem, Let $x,y\in\overline{\mathbb{Q}}$ and

assume

that $\mathrm{g}\mathrm{l}\mathrm{g}_{\frac{x}{y}}1\mathrm{o}\mathrm{g}\not\in \mathrm{Q}$

.

Then for any

$m$, $n\in \mathbb{Z}$, $m$ $>0$,

$|m \frac{1\mathrm{o}\mathrm{g}x}{1\mathrm{o}\mathrm{g}y}-n|>m^{-c}$

with $c$ depending only

on

$x$ and $y$

.

Here

we

calculate the absolute tensor product for Selberg zeta functions for

circles.

Theorem 7The absolute tensor product

of

$Z_{j}(s)=(1-e^{-l_{j}s})^{-1}$ $(j=1,2)$

is expressed

as

follows

in ${\rm Re}(\mathrm{s})>0$ with

some

polynomials $Q(s)$:

(1) When both $\frac{l_{1}}{l_{2}}$ and $\frac{l_{1}}{l_{2}}$

are

generic,

$(Z_{1}\otimes Z_{2})(s)=e^{Q(s)}(1-e^{-\cdot l_{1}})^{\frac{1}{2}}(1-e^{-\epsilon l_{2}})^{\frac{1}{2}}$

$\mathrm{x}\exp(\frac{1}{2i}\sum_{k=1}^{\infty}\frac{\cot(\pi k\frac{l_{1}}{l_{2}})}{k}e^{-l_{1}ks}+\frac{1}{2i}\sum_{n=1}^{\infty}\frac{\cot(\pi n\frac{l}{l}1)1}{n}e^{-l_{2}ns)}$

(2) When $l_{1}=l_{2}=l$,

$(Z_{1} \otimes Z_{2})(s)=e^{Q(s)}(1-e^{-ls})^{1-\frac{l\epsilon}{2\pi}}.\cdot\exp(\frac{-1}{2\pi i}\sum_{n=1}^{\infty}\frac{e^{-nls}}{n^{2}})$

.

(4)

In particular when $l_{1}=\log p$ and $l_{2}=1o\mathrm{g}q$ with

some

prime powers $p$

and q, the following theorem holds:

Theorem 8([KK2]) Let $\zeta(s, \mathrm{F}_{p})=(1-p^{-}’)$

-1.

We have the following

expressions in ${\rm Re}(s)>0$ with

some

polynomials $Q(s)$

.

(i) When $p\neq q$,

$\zeta(s, \mathrm{F}_{p})\otimes\zeta(s,\mathrm{F}_{q})=e^{Q(s)}(1-p^{-\epsilon})^{\frac{1}{2}}(1-q^{-s})^{\frac{1}{2}}$

$\mathrm{x}\exp(\frac{1}{2i}\sum_{k=1}^{\infty}\frac{\cot(\pi k\frac{1\mathrm{o}\mathrm{g}p}{1\mathrm{o}\mathrm{g}q})}{k}p^{-ks}+\frac{1}{2i}\sum_{n=1}^{\infty}\frac{\cot(\pi n_{\mathrm{g}p}\frac{10}{10}\mathrm{g}\mathrm{g})}{n}q^{-ns})$

(2) When$p=q$,

$\zeta(s, \mathrm{F}_{p})\otimes\zeta(s, \mathrm{F}_{p})=e^{Q(s)}(1-p^{-s})^{1--_{2\pi}}.\cdot\exp*\mathrm{p}1\mathrm{o}_{R}(\frac{-1}{2\pi i}\sum_{n=1}^{\infty}p^{-n}\mathrm{i}_{2})n$

.

Remark 9(Convergence) Theconvergenceofthe powerseries in the right

hand side of Theorems $7(1)$ and $8(1)$ is subtle. When $\alpha\in \mathrm{R}$ is generic,

we

deduce from the definition that $|m\alpha-n|>e^{-\epsilon m}$ for any $m\geq 1$ and any

$n\in \mathrm{Z}$

.

Thus it holds that $\cot(\pi m\alpha)=O(e^{\epsilon m})$ for any $\epsilon>0$

.

Hence the

series

$\sum_{m=1}^{\infty}\cot(\pi m\alpha)x^{m}$

absolutely converges in $|x|<1$. This is the

reason

why

we

need the

as-sumption of genericity. In Theorem 8we do not need the assumption with

help of the Baker’s theorem. When $\alpha=\mathrm{g}1\log q\epsilon$, the Baker’s theorem leads to

$|m\alpha-n|>m^{-\mathrm{c}}$ for any $m\geq 1$ and $n\in \mathrm{Z}$

.

Then $\cot(\pi m\alpha)=O(m^{\epsilon})$ and

hence the series again absolutely converges in $|x|$ $<1$

.

Remark 10 (Euler product) Assume $Z_{j}$ has

an

analytic continuation,

a

functional

equation and

an

Euler product expressi $0$

$Z_{j}(s)= \prod_{p}H_{p}^{(j)}(N(p)^{-s})$

(5)

in ${\rm Re}(s)>\sigma_{j}$ with $H_{p}^{(j)}(T)$ $\in 1+T\mathbb{C}[[T]]$

.

Then $Z_{1}\otimes\cdots\otimes Z_{r}$ would have

an

Euler product

$(Z_{1} \otimes\cdots\otimes Z_{r})(s)=e^{Q(s)}\prod_{p_{1,\ldots\prime}p_{r}}H_{p_{1,\ldots\prime}p_{r}}(N(p_{1})^{-}’, \ldots, N(p_{r})^{-s})$

with $H_{p_{1}},\ldots$

,$\mathrm{P}r(T_{1}, \ldots, T_{r})\in 1$ $+(T_{1}, \ldots, T_{r})\mathbb{C}[[T_{1}, \ldots, T_{r}]]$ and

some

polynomial

$Q(s)$

.

Theorem 8gives

an

example of this fact where we put $H_{p}^{(1)}(p^{-}’)$ $=$ $(1-p^{-s})^{-1}$, $H_{q}^{(2)}(q^{-}’)=(1-q^{-s})^{-1}$ and the right hand side of Theorem 8

gives the explicit form of $H_{p,q}(p^{-s}, q^{-s})$

.

The following Theorem deals with the remaining

cases.

Theorem 11 ([KK4]) Let$N_{1}$ and$N_{2}$ be pisitive integers and$N_{0}=(N_{1}, N_{2})$

.

The follouring expression holds in ${\rm Re}(s)>0$:

$\zeta(s, \mathrm{F}_{p^{N_{1}}})\otimes\zeta(s, \mathrm{F}_{p^{N_{2}}})$

$= \exp(-\frac{1}{2\pi i}\frac{N_{0}^{2}}{N_{1}N_{2}}\sum_{n=1}^{\infty}\frac{p^{-snN_{1}N_{2}/N_{0}}}{n^{2}}+(\frac{isN_{0}\log p}{2\pi}-1)$ $\sum_{n=1}^{\infty}\frac{p^{-\cdot nN_{1}N_{2}/N_{0}}}{n}$

$+ \sum_{n=1}^{\infty}\frac{p^{-s\mathfrak{n}N_{1}}f_{1}(n)+p^{-snN_{2}}f_{2}(n)}{n}+Q_{p}(s))$ ,

where $Q_{p}(s)$ is a quadratic polynomial in $s$ and

$f_{1}(n)=\{(e_{N\simeq_{2\overline{N}_{\mathrm{O}}}^{-A}N}^{2\pi|nN_{1}/N_{2}}.-\mathrm{l})^{-1}(\frac{}{(}\parallel n)\frac{NN\mathrm{g}\theta_{2}}{N\mathrm{o}}|n)’$

$f_{2}(n)=\{(e^{2\pi\cdot nN_{2}/N_{1}}.-1)^{-1}rightarrow N-N2N\mathrm{o}^{\mathrm{A}}(\frac{N_{1}}{(\frac{N\theta}{N}}\int_{1,\mathrm{o}’|n}n))$

Ageneralzation of theprecedingtheorems to the

case

ofthree zeta functions

was

recently done by Akatsuka

as

follows

(6)

Theorem 12 ([A]) Let$p$, $q$, $r$ be distinct primes. In ${\rm Re}(s)>0$

we

have

$\zeta(s, \mathrm{F}_{p})\otimes\zeta(s, \mathrm{F}_{q})\otimes\zeta(s, \mathrm{F}_{r})$

$=e^{Q(s)}(1-p^{-s})^{-\frac{1}{4}}(1-q^{-s})^{-\frac{1}{4}}(1-r^{-s})^{-\frac{1}{4}}$

$\exp(-\frac{1}{4}\sum_{n_{1}=1}^{\infty}\frac{\cot(\pi n_{1_{\mathrm{o}\mathrm{g}q}^{\frac{1}{1}\mathrm{E})\cot(\pi n_{1}\frac{1\mathrm{o}\mathrm{g}p}{1\mathrm{o}\mathrm{g}r})}}^{\mathrm{o}}}{n_{1}p^{n_{1}s}}$

$- \frac{1}{4}\sum_{n_{2}=1}^{\infty}\frac{\cot(\pi n_{2_{\mathrm{o}\mathrm{g}p}^{\frac{1}{1}BA)\cot(\pi n_{2}\frac{1\mathrm{o}\mathrm{g}q}{1\mathrm{o}\mathrm{g}r})}}^{\mathrm{o}}}{n_{2}q^{n_{2^{S}}}}$

$- \frac{1}{4}\sum_{n_{3}=1}^{\infty}\frac{\cot(\pi n_{3}\frac{1\mathrm{o}\mathrm{g}r}{\overline{10}\mathrm{g}p})\cot(\pi n_{3_{\mathrm{g}}^{\frac{1\circ}{10}\epsilon}}\frac{r}{q})}{n_{3}r^{-n_{3^{\theta}}}}$

$+ \frac{i}{4}\sum_{n_{1}=1}^{\infty}\frac{\cot(\pi n_{1_{\mathrm{g}q}^{\frac{10}{10}\mathrm{g}\mathrm{g})+\cot(\pi n_{1_{\mathrm{o}\mathrm{g}r}^{\frac{1}{1}}}^{\mathrm{o}\mathrm{g}\mathrm{g})}}}}{n_{1}p^{n_{1^{\mathrm{S}}}}}$

$+ \frac{i}{4}.\sum_{n\mathrm{z}=1}^{\infty}\frac{\cot(\pi n_{2}\frac{1\mathrm{o}\mathrm{g}q}{1\mathrm{o}\mathrm{g}p})+\cot(\pi n_{2_{1\mathrm{o}\mathrm{g}r}^{\mathrm{l}}}^{\mathrm{E}\Xi 4)}}{n_{2}q^{n_{2}s}}$

$+ \frac{i}{4}\sum_{n\mathrm{s}=1}^{\infty}\frac{\cot(\pi n_{3}\frac{1\mathrm{o}\mathrm{g}r}{1\mathrm{o}\mathrm{g}p})+\cot(\pi n_{3}\frac{1\mathrm{o}\mathrm{g}_{l}}{1\mathrm{o}\mathrm{g}q})}{n_{3}r^{n\mathrm{s}^{\mathrm{g}}}})$

Here

we

present the outline of

our

proof of Theorem 7. We

use

the

multiple sine function defined in [KK1]. We recall the definitions

as

follows:

The multiple Hurwitz zeta function is defined by Barnes [B]

as

$\zeta_{r}(s, z,\underline{\omega})=\sum_{n_{1,\ldots\prime}n_{r}=0}^{\infty}(n_{1}\omega_{1}+\cdots+n_{r}\omega_{f}+z)^{-s}$

for$\underline{\omega}=$ $(\omega_{1}, \ldots, \omega_{r})$ with$\omega_{j}>0$and ${\rm Re}(s)>r$

.

The multiple gamma function

is also defined

as

$\Gamma_{r}(z,\underline{\omega})=\exp(\frac{\partial}{\partial s}\zeta_{r}(s, z,\underline{\omega})|_{s=0})$

.

We define the multiple sine function [KK1]

as

$S_{r}(z,\underline{\omega})=\Gamma_{r}(z,\underline{\omega})^{-1}\Gamma_{r}(\omega_{1}+\cdots+\omega_{r}-z,\underline{\omega})^{(-1)^{r}}$

(7)

We put for simplicity

as

$Sr(z):=Sr(z)$ (1, \ldots , 1)), Fr(z) $:=\mathrm{F}\mathrm{r}(\mathrm{z})$ (1, \ldots , 1)),

$\Gamma_{1}(z)=\Gamma_{1}(z, 1)=\Gamma(z)/\sqrt{2\pi}$ and $S_{1}(z)=S_{1}(z, 1)=2\sin(\pi z)$.

Lemma 13 The absolute tensor product in Theorem 7is expressed as

fol-lows:

$(Z_{1}\otimes Z_{2})(s)=e^{Q(\epsilon)}S_{2}(is$,

(

$\frac{2\pi}{l_{1}}$, $\frac{2\pi}{l_{2}}$

)

$)$ ,

where $Q(s)$ is a polynomial

of

degree at most two, which depends on $l_{1}$ and

$l_{2}$

.

Proof.

The definitions of the absolute tensor product and the multiple sine

functions easily lead

us

to the identity.s

Next

we

obtain the “Euler product” expression of the double sine

func-tion:

Lemma 14 ([KK2])

If

both $\frac{\omega_{1}}{\omega_{2}}$ and $\frac{\omega_{2}}{\omega_{1}}$

are

generic and ${\rm Im}(z)>0$,

$S_{2}(z, (\omega_{1},\omega_{2}))$

$= \exp(\frac{1}{2i}\sum_{k=1}^{\infty}\frac{1}{k}\cot(\pi k\frac{\omega_{2}}{\omega_{1}})e^{2\pi\dot{l}k\frac{l}{w_{1}}}+\frac{1}{2i}\sum_{n=1}^{\infty}\frac{1}{n}\cot(\pi n\frac{\omega_{1}}{\omega_{2}})e^{2\pi\cdot n\frac{z}{2}}..$

$+ \frac{1}{2}\log(1-e^{2\pi}:.\frac{z}{1})+\frac{1}{2}\log(1-e^{2\pi}:.\frac{l}{2})$

$+ \frac{\pi iz^{2}}{2\omega_{1}\omega_{2}}-\frac{\pi i}{2}(\frac{1}{\omega_{1}}+\frac{1}{\omega_{2}})z+\frac{\pi i}{12}(\frac{\omega_{2}}{\omega_{1}}+\frac{\omega_{1}}{\omega_{2}}+3))$

Proof.

First

we

establish the “signatured” Poisson summation formula,

counting only

zeros

in the upper halfplane, with the test function

$H(t):=(t-z)^{-2}-(t +z)^{-2}$

.

By Cauchy’s theorem

we

have

$H(k \omega_{1}+n\omega_{2})=\frac{1}{(2\pi i)^{2}}\int_{C}\int_{C}h(s_{1}+s_{2})\frac{\xi_{1}’}{\xi_{1}}(s_{1})\frac{\xi_{2}’}{\xi_{2}}(s_{2})ds_{1}ds_{2}$ (1)

with $\xi_{1}(s)=\sinh(\frac{\pi s}{\omega_{1}})$ and $\xi_{2}(s)=\mathrm{s}\dot{\mathrm{m}}\mathrm{h}(\frac{\pi s}{\omega_{2}})$, and where $C=\partial\{s\in \mathbb{C}||{\rm Re}(s)|<\alpha, |s| >\alpha, {\rm Im}(s)>0\}$

.

(8)

Calculating the integrals in the right hand side of (1) leads to the signatured Poisson summation formula:

$\sum_{k,n>0}H(k\omega_{1}+n\omega_{2})$ $=$

$- \frac{1}{2}(\sum_{k>0}H(k\omega_{1})+\sum_{n>0}H(n\omega_{2}))$

$- \frac{i}{2\omega_{1}}\sum_{k>0}\cot(\pi\frac{k\omega_{2}}{\omega_{1}})\tilde{H}(\frac{2\pi k}{\omega_{1}})$

$- \frac{i}{2\omega_{2}}\sum_{n>0}\cot(\pi\frac{n\omega_{1}}{\omega_{2}})\overline{H}(\frac{2\pi n}{\omega_{2}})-\frac{i}{2}\overline{H}’(0)$

.

(2)

Then the left hand side of (2) is equal to

$\frac{d^{2}}{ds^{2}}\log S_{2}(z,\omega_{1},\omega_{2})$.

Thus

$S_{2}(z,\omega_{1},\omega_{2})$ $= \exp(\iint(2)dzdz)$ ,

where

we

substitute (2) with its right hand side, 1

2Application

to

Special

Values

By using the multiple sine function appeared in the proof of

our

theorems

in the preceding section,

we

express

some

unknown special values for the

Riemann zeta and Dirichlet L-functions.

Theorem 15 ([KK3]) Let $0<n$, $k\in \mathbb{Z}$ and put

$a(2n+1, k)= \sum_{l=1}^{k}(-1)^{k-l}l^{2n}$ $(\begin{array}{ll}2n +\mathrm{l}k -l\end{array})$,

then

we

have

$\zeta(2n+1)=\frac{2^{2n+1}\pi^{2n}}{(-1)^{n-1}(2n)!}\log\prod_{k=1}^{n}S_{2n+1}(k)^{a(2n+1.k)}$

.

(9)

Examples.

$\zeta(3)$ $=$ $4\pi^{2}\log S_{3}(1)$,

$\zeta(5)$ $=$ $- \frac{4\pi^{4}}{3}\log(S_{5}(1)S_{5}(2)^{11})$,

$\zeta(7)$ $=$ $\frac{8\pi^{6}}{45}\log(S_{7}(1)S_{7}(2)^{57}S_{7}(3)^{302})$.

Theorem 16 ([KK3]) Let$\chi$ be

a

primitive oddDirichlet character $(\mathrm{m}\mathrm{o}\mathrm{d} N)$

.

Then $L(2, \chi)=\frac{2\pi i\tau(\chi)}{N^{2}}\log\prod_{k=1}^{N-1}(S_{2}(\frac{k}{N})^{N}S_{1}(\frac{k}{N})^{k})^{\overline{\chi}(k)}$ Examples. $L(2, (_{*}^{\underline{-4}}))$ $=$ $\frac{-\pi}{4}\log(S_{2}(\frac{1}{4})^{4}S_{1}(\frac{1}{4})S_{2}(\frac{3}{4})^{-4}S_{1}(\frac{3}{4})^{-3})$ $=$ $\frac{\pi}{4}\log(2^{-3}S_{2}(\frac{1}{4})^{-8})$ , $L(2, (_{*}^{\underline{-3}}))$ $=$ $\frac{-2\sqrt{3}\pi}{9}\log(S_{2}(\frac{1}{3})^{3}S_{1}(\frac{1}{3})S_{2}(\frac{2}{3})^{-3}S_{1}(\frac{2}{3})^{-2})$ $=$ $\frac{4\sqrt{3}\pi}{9}\log(\frac{3}{4}S_{2}(\frac{1}{3})^{-3})$

.

Theorem 17 ([KK3]) Let$\chi$ be

a

primitive

even

Dirichlet character $(\mathrm{m}\mathrm{o}\mathrm{d} N)$.

$L(3, \chi)=\frac{2\pi^{2}\tau(\chi)}{N^{3}}\log\prod_{k=1}^{N-1}(S_{3}(\frac{k}{N})^{2N^{2}}S_{2}(\frac{k}{N})^{2Nk-3N^{2}}S_{1}(\frac{k}{N})^{k^{2}})^{\overline{\chi}(k)}$

(10)

Examples.

$L$(3, $(^{\underline{12}}*)$ ) $=$ $\frac{\sqrt{3}\pi^{2}}{432}\log(S_{3}(\frac{1}{12})288S_{2}(\frac{1}{12})-408S_{1}(\frac{1}{12})$

$S_{3}( \frac{5}{12})-288S_{2}(\frac{5}{12})312S_{1}(\frac{5}{12})-25$

$S_{3}( \frac{7}{12})-288S_{2}(\frac{7}{12})264S_{1}(\frac{7}{12})-49$

$S_{3}( \frac{11}{12})288S_{2}(\frac{11}{12})-164S_{1}(\frac{11}{12})121)$ .

3Application

to

$\Gamma$

-factors of Selberg Zeta

Func-tions

Let $M=\Gamma\backslash G/K$ be acompact locally symmetric space of rank

one.

In

this section

we

present the explicit form of the $\Gamma$-factors of the Selberg zeta

function of $M$

.

When $\dim M$ is odd, it has only trivial $\Gamma$-factors which

are

exponential of

some

polynomials. So in what follows

we assume

$\dim M$ is

even.

Let $M’=G’/K$ be the compact dual symmetric space of $M$ which is

given by the following table:

$G$ A $(\acute{\mathrm{z}}’$ $M’$

50

$(1, n)$ SO(n) SO(l+n) $S^{n}$

$SU(1,n)$ $SU(n)$ $SU(1+n)$ $\mathrm{P}_{\mathrm{C}}^{n}$

$Sp(1,n)F_{4}$ $Sp(n))$ $Sp(1,+n)F_{4}$ $\mathrm{P}_{\mathrm{O}}^{2}\mathrm{P}_{\mathrm{H}}^{n}$

Spin(9)

Let$\sigma$be unitary representation of$\Gamma$. TheSelberg zetafunction $Z_{M}(s, \sigma)$

is defined by Gangolli [G]. It has

an

analytic continuation to all $s\in \mathbb{C}$

as a

meromorphic function of order $\dim M$

.

It also has afunctional equation:

$Z_{M}(2 \rho_{0}-s, \sigma)=Z_{M}(s, \sigma)\exp(\mathrm{v}\mathrm{o}\mathrm{l}(M)\dim(\sigma)\int_{0}^{s-n}\mu_{M}(it)dt)$

where $\rho_{0}>0$ and $\mu_{M}(l)$ is the Plancherel

measure

(11)

Lemma 18 Let $S(\Delta_{M’})$ be the set

of

eigenvalues

of

$\Delta_{M’}$

.

The spectral zeta

function

$\zeta$

(

$s$,$z$, $\sqrt{\Delta_{M’}+\rho_{0}^{2}}$

)

$:= \sum_{\lambda\in S(\Delta_{M’})}(\sqrt{\lambda+\rho_{0}^{2}}+z)^{-s}$

is holomorphic at $s=0$

.

Thus

we

define $\coprod_{\lambda\in S(\Delta_{M’})}(\sqrt{\lambda+\rho_{0}^{2}}+z)=\det(\sqrt{\Delta_{M’}+\rho_{0}^{2}}+z)$

.

Actually $\det(\sqrt{\Delta_{M’}+\rho_{0}^{2}}+s$ $-\rho 0)^{-1}$ $=\{\begin{array}{l}\Gamma_{2n}(s)\Gamma_{2n}(s+\mathrm{l})\prod_{k=0}^{n}\Gamma_{2n}(s+k)^{(})^{2}\prod_{k=0}^{2\mathrm{n}-1}\Gamma_{4n}(s+k)^{\frac{1}{2n}(})()\Gamma_{16}(s)\Gamma_{16}(s+\mathrm{l})^{10}\Gamma_{16}(s+2)^{28}\mathrm{x}\Gamma_{16}(s+3)^{28}\Gamma_{16}(s+4)^{10}\Gamma_{16}(s+5)\end{array}$ $(G=SU(1,n))(G=Sp(1,n))(G=SO(1,2n))(G=F_{4})$ Theorem 19 ([KK1]) Put $\Gamma_{M}(s,\sigma)=\det(\sqrt{\Delta_{M’}+\rho_{0}^{2}}+s-\rho 0)^{\mathrm{v}\mathrm{o}\mathrm{l}(M)\dim(\sigma)(-1)^{\dim M/2}}$

Then $\hat{Z}_{M}(s,\sigma)=\Gamma_{M}(s, \sigma)Z_{M}(s, \sigma)$

satisfies

the symmetric

functional

equa-tion:

$\hat{Z}_{M}(s, \sigma)=\hat{Z}_{M}(2\rho_{0}-s,\sigma)$

.

(12)

Proof.

We prove for the

case

of

SO

$(1, 2n)$

.

All other

cases

are

proved by

similar methods. It suffices to show

$\exp$

(

$\int_{0}^{s-\beta 0}\mu_{M}$(it)$dt$

)

$\underline{\mathrm{d}}\mathrm{i}\mathrm{m}\underline{M}\mathrm{T}=S_{2n}(s)S_{2n}(s+1)$

. (3)

Both sides

are

equal to 1, when $s=\rho_{0}=n$$- \frac{1}{2}$

.

We compare the logarithmic

derivative of (3). We appeal to the differential equation of $S_{r}(z)$ which is

obtained in [KK1]:

$\frac{S_{r}’}{S_{r}}(z)=(-1)^{r-1}$ $(\begin{array}{ll}z -\mathrm{l}r -\mathrm{l}\end{array})$ $\pi\cot(\pi z)$

.

Theorem follows by the facts

$\mu_{M}$(it)$)=(-1)^{n}P_{M}(t)\pi\tan(\pi t)$

and

$P_{M}(t)= \frac{2}{(2n-\mathrm{I})!}t\prod_{k=1}^{n-1}(t^{2}-(k-\frac{1}{2})^{2}).\mathrm{I}$

References

[A] H. Akatsuka: Euler product expression of triple zeta functions.

(preprint)

[B] E.W. Barnes: On the theory of the multiple

gamma

function. TVans.

Cambridge Philos. Soc, 19 (1904)

374-425.

[G] R. Gangolli: Zeta functions ofSelberg’s type for compact space forms

ofsymmetric spaces of rank

one.

Ilinois J. Math. 21 (1977) 1-41.

[KK1] N. Kurokawa and S. Koyama: Multiple sine functions. Forum Math,

(in press)

[KK2] S. Koyama and N. Kurokawa: Multiple zeta functions I. Composit.

Math, (in press)

[KK3]

S.

Koyama and N. Kurokawa: Zeta functions and normalzed multiple

sine functions. (preprint)

(13)

[KK4] N. Kurokawa andS. Koyama: Normalized double sinefunctions. Proc.

Japan Acad. 79 (2003) 14-18.

[KK5] S. Koyama and N. Kurokawa: Certain series related to the triple sine

function (preprint).

[KK6] S. Koyama and N. Kurokawa: Rummer’s formula for multiple gamma

functions (preprint).

[M] Yu. I. Manin: Lectures

on

zeta functions and motives (according to

Deninger and Kurokawa). Asterisque 228 (1995) 121-163

参照

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