翻訳と辞書
Words near each other
・ Rifa'i
・ Rifaat al-Assad
・ Rifaat Eid
・ Rifaat El-Fanagily
・ Rifaat el-Mahgoub
・ Rifaat Garrana
・ Rifaat Hussain
・ Rifaat Turk
・ Rifabutin
・ Rifaina
・ Rifalazil
・ Rifampicin
・ Riesz mean
・ Riesz potential
・ Riesz rearrangement inequality
Riesz representation theorem
・ Riesz sequence
・ Riesz space
・ Riesz theorem
・ Riesz transform
・ Riesz's lemma
・ Riesz–Fischer theorem
・ Riesz–Markov–Kakutani representation theorem
・ Riesz–Thorin theorem
・ Riet
・ Riet River
・ Riet River (Doring)
・ Riet, Germany
・ Rietavas
・ Rietavas Manor


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

Riesz representation theorem : ウィキペディア英語版
Riesz representation theorem
There are several well-known theorems in functional analysis known as the Riesz representation theorem. They are named in honour of Frigyes Riesz.
This article will describe his theorem concerning the dual of a Hilbert space, which is sometimes called the Fréchet-Riesz theorem. For the theorems relating linear functionals to measures, see Riesz–Markov–Kakutani representation theorem.
== The Hilbert space representation theorem ==
This theorem establishes an important connection between a Hilbert space and its (continuous) dual space. If the underlying field is the real numbers, the two are isometrically isomorphic; if the underlying field is the complex numbers, the two are isometrically anti-isomorphic. The (anti-) isomorphism is a particular, natural one as will be described next.
Let ''H'' be a Hilbert space, and let ''H
*'' denote its dual space, consisting of all continuous linear functionals from ''H'' into the field R or C. If ''x'' is an element of ''H'', then the function φ''x'', for all ''y'' in ''H'' defined by
:\varphi_x(y) = \left\langle y , x \right\rangle,
where \langle\cdot,\cdot\rangle denotes the inner product of the Hilbert space, is an element of ''H
*''. The Riesz representation theorem states that ''every'' element of ''H
*'' can be written uniquely in this form.
Theorem. The mapping \Phi: ''H'' → ''H
*'' defined by \Phi(x) = \varphi_x is an isometric (anti-) isomorphism, meaning that:
* \Phi is bijective.
* The norms of x and \varphi_x agree: \Vert x \Vert = \Vert\Phi(x)\Vert.
* \Phi is additive: \Phi( x_1 + x_2 ) = \Phi( x_1 ) + \Phi( x_2 ).
* If the base field is R, then \Phi(\lambda x) = \lambda \Phi(x) for all real numbers λ.
* If the base field is C, then \Phi(\lambda x) = \bar \Phi(x) for all complex numbers λ, where \bar denotes the complex conjugation of λ.
The inverse map of \Phi can be described as follows. Given a non-zero element \varphi of ''H
*'', the orthogonal complement of the kernel of \varphi is a one-dimensional subspace of ''H''. Take a non-zero element ''z'' in that subspace, and set x = \overline \cdot z /^2. Then \Phi(x) = \varphi.
Historically, the theorem is often attributed simultaneously to Riesz and Fréchet in 1907 (see references).
In the mathematical treatment of quantum mechanics, the theorem can be seen as a justification for the popular bra–ket notation. When the theorem holds, every ket |\psi\rangle has a corresponding bra \langle\psi|, and the correspondence is unambiguous. cf. also Rigged Hilbert space

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「Riesz representation theorem」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.