翻訳と辞書
Words near each other
・ Yamaguchi Korean High School
・ Yamaguchi Line
・ Yamaguchi opening rule
・ Yamaguchi Prefectural Museum
・ Yama-bito
・ Yama-Con
・ Yama-dera
・ Yama-no Attchan
・ Yama-no-Kami
・ Yama-uba
・ YamaArashi
・ Yamabal
・ Yamabe
・ Yamabe District, Nara
・ Yamabe flow
Yamabe invariant
・ Yamabe no Akahito
・ Yamabe problem
・ Yamabe Station
・ Yamabiko
・ Yamabiko (folklore)
・ Yamabiko Corporation
・ Yamabuggy
・ Yamabuki Station
・ Yamabushi
・ Yamaceratops
・ Yamachiche
・ Yamacraw
・ Yamacraw (disambiguation)
・ Yamacraw Bluff


Dictionary Lists
翻訳と辞書 辞書検索 [ 開発暫定版 ]
スポンサード リンク

Yamabe invariant : ウィキペディア英語版
Yamabe invariant
In mathematics, in the field of differential geometry, the Yamabe invariant (also referred to as the sigma constant) is a real number invariant associated to a smooth manifold that is preserved under diffeomorphisms. It was first written down independently by O. Kobayashi and R. Schoen and takes its name from H. Yamabe.
== Definition ==
Let M be a compact smooth manifold (without boundary) of dimension n\geq 2. The normalized Einstein–Hilbert functional \mathcal assigns to each Riemannian metric g on M a real number as follows:
: \mathcal(g) = \frac}},
where R_g is the scalar curvature of g and dV_g is the volume density associated to the metric g. The exponent in the denominator is chosen so that the functional is scale-invariant: for every positive real constant c, it satisfies \mathcal(cg) = \mathcal(g). We may think of \mathcal(g) as measuring the average scalar curvature of g over M. It was conjectured by Yamabe that every conformal class of metrics contains a metric of constant scalar curvature (the so-called Yamabe problem); it was proven by Yamabe, Trudinger, Aubin, and Schoen that a minimum value of \mathcal(g) is attained in each conformal class of metrics, and in particular this minimum is achieved by a metric of constant scalar curvature.
We define
: Y(g) = \inf_ \mathcal(e^ g),
where the infimum is taken over the smooth real-valued functions f on M. This infimum is finite (not -\infty): Hölder's inequality implies Y(g) \geq -\left(\textstyle\int_M |R_g|^ \,dV_g\right)^. The number Y(g) is sometimes called the conformal Yamabe energy of g (and is constant on conformal classes).
A comparison argument due to Aubin shows that for any metric g, Y(g) is bounded above by \mathcal(g_0), where
g_0 is the standard metric on the n-sphere S^n. It follows that if we define
: \sigma(M) = \sup_ Y(g),
where the supremum is taken over all metrics on M, then \sigma(M) \leq \mathcal(g_0) (and is in particular finite). The
real number \sigma(M) is called the Yamabe invariant of M.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「Yamabe invariant」の詳細全文を読む



スポンサード リンク
翻訳と辞書 : 翻訳のためのインターネットリソース

Copyright(C) kotoba.ne.jp 1997-2016. All Rights Reserved.