• 検索結果がありません。

ON THE KOTTWITZ-SHELSTAD NORMALIZATION OF TRANSFER FACTORS FOR AUTOMORPHIC INDUCTION FOR $rm{GL_n}$(JOINT WORK WITH K. HIRAGA) (Automorphic forms, automorphic representations and related topics)

N/A
N/A
Protected

Academic year: 2021

シェア "ON THE KOTTWITZ-SHELSTAD NORMALIZATION OF TRANSFER FACTORS FOR AUTOMORPHIC INDUCTION FOR $rm{GL_n}$(JOINT WORK WITH K. HIRAGA) (Automorphic forms, automorphic representations and related topics)"

Copied!
3
0
0

読み込み中.... (全文を見る)

全文

(1)

ON THE

KOTTWITZ-SHELSTAD

NORMALIZATION

OF

TRANSFER FACTORS FOR AUTOMORPHIC

INDUCTION FOR

$GL_{n}$

(JOINT WORK WITH K. HIRAGA)

ATSUSHI ICHINO

This note is

a

report

on

ajoint work with Kaoru Hiraga. Details will appear elsewhere.

Automorphic induction for $GL_{n}$

over a

p-adic field is

an

example

of endoscopic transfer and its character identity

was

established by Henniart and Herb [2], up to

a

constant. We discuss

a

relation of this constant to the Kottwitz-Shelstad transfer factor [5], in particular, to the normalization using $\epsilon$-factors.

Let $F$ be

a

non-archimedean local field of characteristic

zero.

Let

$G=GL_{n}(F)$ and $a\in H^{1}(W_{F}, Z(\hat{G}))$, where $W_{F}$ is the Weil group of

$F$ and $Z($

$)$ is the center of the dual group of $G$. Let $(H, \mathcal{H}, s, \xi)$ be

an

endoscopic data for ($G$, id, a) (see [5]). Then

we

have

a

map

$Ran_{H}^{G}$ :

{(stable)

invariant distributions

on

$H$

}

$arrow$

{

$twisted$ invariant distributions

on

$G$

}

defined

as

follows.

Let $\omega$ be the character of $F^{\cross}$ associated to $a$. We write $\omega(g)=$

$\omega(\det g)$ for $g\in G$

.

For a (strongly) regular semisimple element $\gamma\in G$

such that $G_{\gamma}\subset ker\omega$ and $f^{G}\in C_{c}^{\infty}(G)$, put

$O_{\gamma}^{\omega}(f^{G})= \int_{G_{\gamma}\backslash G}\omega(g)f^{G}(g^{-1}\gamma g)dg$,

where $G_{\gamma}$ is the centralizer of

$\gamma$ in $G$. Similarly, for

a

(strongly)

G-regular semisimple element $\gamma_{H}\in H$ and $f^{H}\in C_{c}^{\infty}(H)$, put $O_{\gamma H}(f^{H})= \int_{H_{\gamma_{H}}\backslash H}f^{H}(h^{-1}\gamma_{H}h)dh$,

where $H_{\gamma_{H}}$ is the centralizer of$\gamma_{H}$ in $H$. Here

we

choose suitable Haar

measures

on

$G,$ $G_{\gamma},$ $H$, and $H_{\gamma_{H}}$. By

a

result of Waldspurger [7], for

数理解析研究所講究録

(2)

ATSUSHI ICHINO

each $f^{G}\in C_{c}^{\infty}(G)$, there exists $f^{H}\in C_{c}^{\infty}(H)$ such that

$O_{\gamma_{H}}(f^{H})= \sum_{\gamma}\triangle(\gamma_{H}, \gamma)O_{\gamma}^{\omega}(f^{G})$

for all G-regular semisimple elements $\gamma_{H}\in H$. Here the

sum

is taken

over a

set of representatives for the conjugacy classes of $\gamma\in G$ whose

norm

is $\gamma_{H}$ and

$\triangle$ is

a

transfer factor (see [5]). Since $G$ is quasi-split

over

$F$,

we

can

normalize $\triangle$ using Whittaker data and

$\epsilon$-factors

as

in

[5,

\S 5.3].

For an invariant distribution $D$

on

$H$,

we

define

a

twisted

invariant distribution $Tran_{H}^{G}(D)$ by

$Tran_{H}^{G}(D)(f^{G})=D(f^{H})$

for $f^{G}\in C_{c}^{\infty}(G)$.

On the other hand, by

a

result of Henniart and Herb [2], for each irreducible tempered admissible representation $\pi_{H}$ of $H$, there exist

an

irreducible tempered admissible representation $\pi$ of $G$ and

a

constant $c\in \mathbb{C}^{\cross}$ such that $\pi\otimes\omega\cong\pi$ and

$Tran_{H}^{G}(\Theta_{\pi_{H}})=c\cdot\Theta_{\pi}^{\omega}$.

Here $\Theta_{\pi}H(f^{H})=$ trace$(\pi_{H}(f^{H}))$ for $f^{H}\in C_{c}^{\infty}(H)$ and $\Theta_{\pi}^{\omega}(f^{G})=$

trace$(\pi(f^{G})\circ \mathcal{A}_{\omega})$ for $f^{G}\in C_{c}^{\infty}(G)$, where $\mathcal{A}_{4}$ : $\pi\otimes\omegaarrow\pi$ is

an

isomorphism

as

vector spaces.

Since

$\pi$ is generic,

we

can

normalize $\mathscr{N}$

using Whittaker

functionals.

By a result of Henniart and Lemair [3], the constant $c$ does not depend

on

the representations.

Our main result is as follows. Theorem 1. We have

$c=1$.

Remark 2. An analogous result for $F=\mathbb{R}$

was

proved by Henniart [1].

REFERENCES

[1] G. Henniart, Induction automorphe pour$GL(n, \mathbb{C})$, preprint.

[2] G. Henniart and R. Herb, Automorphic induction

for

GL(n) (over local

non-Archimedeanfields), Duke Math. J. 78 (1995), 131-192.

[3] G. Henniart and B. Lemaire, Fomules de camct\‘erespour l’induction

automor-phe, preprint.

[4] K. Hiraga and H. Saito, On L-packets

for

inner

forms

of

$SL_{n}$, preprint.

[5] R. E. Kottwitz and D. Shelstad, Foundations oftwisted endoscopy, Ast\’erisque

255 (1999).

[6] R. P. Langlands and D. Shelstad, On the definition of transferfactors, Math.

Ann. 278 (1987), 219-271.

(3)

[7] J.-L. Waldspurger, Sur les integrales orbitales tordues pour les groupes

lineaires: un lemme fondamental, Canad. J. Math. 43 (1991), 852-896.

DEPARTMENT OF MATHEMATICS, GRADUATE SCHOOL OF SCIENCE, OSAKA

CITY UNIVERSITY, $3arrow 3-138$SUGIMOTO, SUMIYOSHI-KU, OSAKA 558-8585, JAPAN

E-mail address: ichinoQsci.osaka-cu.ac.jp

参照

関連したドキュメント

Keywords: continuous time random walk, Brownian motion, collision time, skew Young tableaux, tandem queue.. AMS 2000 Subject Classification: Primary:

Thus, we use the results both to prove existence and uniqueness of exponentially asymptotically stable periodic orbits and to determine a part of their basin of attraction.. Let

, 6, then L(7) 6= 0; the origin is a fine focus of maximum order seven, at most seven small amplitude limit cycles can be bifurcated from the origin.. Sufficient

The stage was now set, and in 1973 Connes’ thesis [5] appeared. This work contained a classification scheme for factors of type III which was to have a profound influence on

Nevertheless, a dis- tributional Poincar´ e series may be constructed via an averaging map, and global automorphic Sobolev theory ensures the existence and uniqueness of an

The aim of this paper is to establish a new extension of Hilbert’s inequality and Hardy- Hilbert’s inequality for multifunctions with best constant factors.. Also, we present

We provide an efficient formula for the colored Jones function of the simplest hyperbolic non-2-bridge knot, and using this formula, we provide numerical evidence for the

Zhang; Blow-up of solutions to the periodic modified Camassa-Holm equation with varying linear dispersion, Discrete Contin. Wang; Blow-up of solutions to the periodic