Riesz representation theorem

There are several well-known theorems in functional analysis known as the Riesz representation theorem. They are named in honor 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 theoremEdit

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; a natural isomorphism.

Let H be a Hilbert space, and let H* denote its dual space, consisting of all continuous linear functionals from H into the field   or  .

If   is an element of H, then the function   for all   in H 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.

Riesz–Fréchet representation theorem. Let   be a Hilbert space and  . Then there exists   such that for any  ,  . Moreover  

Proof. Let  . Clearly   is closed subspace of  . If  , then we can trivially choose  . Now assume  . Then   is one-dimensional. Indeed, let   be nonzero vectors in  . Then there is nonzero real number  , such that  . Observe that   and  , so  . This means that  . Now let   be unit vector in  . For arbitrary  , let   be the orthogonal projection of   onto  . Then   and   (from the properties of orthogonal projections), so that   and  . Thus  . Hence  . We also see  . From the Cauchy-Bunyakovsky-Schwartz inequality  , thus for   with unit norm  . This implies that  .

Given any continuous linear functional g in H*, the corresponding element   can be constructed uniquely by  , where   is an orthonormal basis of H, and the value of   does not vary by choice of basis. Thus, if  , then  

Theorem. The mapping  : HH* defined by   =   is an isometric (anti-) isomorphism, meaning that:

  •   is bijective.
  • The norms of   and   agree:  .
  •   is additive:  .
  • If the base field is  , then   for all real numbers λ.
  • If the base field is  , then   for all complex numbers λ, where   denotes the complex conjugation of  .

The inverse map of   can be described as follows. Given a non-zero element   of H*, the orthogonal complement of the kernel of   is a one-dimensional subspace of H. Take a non-zero element z in that subspace, and set  . Then   =  .

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. The theorem says that, every bra   has a corresponding ket  , and the latter is unique.


  • Fréchet, M. (1907). "Sur les ensembles de fonctions et les opérations linéaires". Les Comptes rendus de l'Académie des sciences (in French). 144: 1414–1416.
  • Riesz, F. (1907). "Sur une espèce de géométrie analytique des systèmes de fonctions sommables". Comptes rendus de l'Académie des Sciences (in French). 144: 1409–1411.
  • Riesz, F. (1909). "Sur les opérations fonctionnelles linéaires". Comptes rendus de l'Académie des Sciences (in French). 149: 974–977.
  • P. Halmos Measure Theory, D. van Nostrand and Co., 1950.
  • P. Halmos, A Hilbert Space Problem Book, Springer, New York 1982 (problem 3 contains version for vector spaces with coordinate systems).
  • Walter Rudin, Real and Complex Analysis, McGraw-Hill, 1966, ISBN 0-07-100276-6.
  • "Proof of Riesz representation theorem for separable Hilbert spaces". PlanetMath.