Riesz representation theorem
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 φx, defined by
where 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 Φ: H → H* defined by Φ(x) = φx is an isometric (anti-) isomorphism, meaning that:
- Φ is bijective.
- The norms of x and Φ(x) agree: .
- Φ is additive: .
- If the base field is R, then for all real numbers λ.
- If the base field is C, then for all complex numbers λ, where denotes the complex conjugation of λ.
The inverse map of Φ can be described as follows. Given a non-zero element φ of H*, the orthogonal complement of the kernel of φ is a one-dimensional subspace of H. Take a non-zero element z in that subspace, and set . Then Φ(x) = φ.
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 has a corresponding bra , and the correspondence is unambiguous.
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