Fundamental theorem of Hilbert spaces
In mathematics, specifically in functional analysis and Hilbert space theory, the fundamental theorem of Hilbert spaces gives a necessarily and sufficient condition for a Hausdorff pre-Hilbert space to be a Hilbert space in terms of the canonical isometry of a pre-Hilbert space into its anti-dual.
Preliminaries
Antilinear functionals and the anti-dual
Suppose that H is a topological vector space (TVS). A function f : H → [math]\displaystyle{ \mathbb{C} }[/math] is called semilinear or antilinear[1] if for all x, y ∈ H and all scalars c ,
- Additive: f (x + y) = f (x) + f (y);
- Conjugate homogeneous: f (c x) = c f (x).
The vector space of all continuous antilinear functions on H is called the anti-dual space or complex conjugate dual space of H and is denoted by [math]\displaystyle{ \overline{H}^{\prime} }[/math] (in contrast, the continuous dual space of H is denoted by [math]\displaystyle{ H^{\prime} }[/math]), which we make into a normed space by endowing it with the canonical norm (defined in the same way as the canonical norm on the continuous dual space of H).[1]
Pre-Hilbert spaces and sesquilinear forms
A sesquilinear form is a map B : H × H → [math]\displaystyle{ \mathbb{C} }[/math] such that for all y ∈ H, the map defined by x ↦ B(x, y) is linear, and for all x ∈ H, the map defined by y ↦ B(x, y) is antilinear.[1] Note that in Physics, the convention is that a sesquilinear form is linear in its second coordinate and antilinear in its first coordinate.
A sesquilinear form on H is called positive definite if B(x, x) > 0 for all non-0 x ∈ H; it is called non-negative if B(x, x) ≥ 0 for all x ∈ H.[1] A sesquilinear form B on H is called a Hermitian form if in addition it has the property that [math]\displaystyle{ B(x, y) = \overline{B(y, x)} }[/math] for all x, y ∈ H.[1]
Pre-Hilbert and Hilbert spaces
A pre-Hilbert space is a pair consisting of a vector space H and a non-negative sesquilinear form B on H; if in addition this sesquilinear form B is positive definite then (H, B) is called a Hausdorff pre-Hilbert space.[1] If B is non-negative then it induces a canonical seminorm on H, denoted by [math]\displaystyle{ \| \cdot \| }[/math], defined by x ↦ B(x, x)1/2, where if B is also positive definite then this map is a norm.[1] This canonical semi-norm makes every pre-Hilbert space into a seminormed space and every Hausdorff pre-Hilbert space into a normed space. The sesquilinear form B : H × H → [math]\displaystyle{ \mathbb{C} }[/math] is separately uniformly continuous in each of its two arguments and hence can be extended to a separately continuous sesquilinear form on the completion of H; if H is Hausdorff then this completion is a Hilbert space.[1] A Hausdorff pre-Hilbert space that is complete is called a Hilbert space.
Canonical map into the anti-dual
Suppose (H, B) is a pre-Hilbert space. If h ∈ H, we define the canonical maps:
- B(h, •) : H → [math]\displaystyle{ \mathbb{C} }[/math] where y ↦ B(h, y), and
- B(•, h) : H → [math]\displaystyle{ \mathbb{C} }[/math] where x ↦ B(x, h)
The canonical map[1] from H into its anti-dual [math]\displaystyle{ \overline{H}^{\prime} }[/math] is the map
- [math]\displaystyle{ H \to \overline{H}^{\prime} }[/math] defined by x ↦ B(x, •).
If (H, B) is a pre-Hilbert space then this canonical map is linear and continuous; this map is an isometry onto a vector subspace of the anti-dual if and only if (H, B) is a Hausdorff pre-Hilbert.[1]
There is of course a canonical antilinear surjective isometry [math]\displaystyle{ H^{\prime} \to \overline{H}^{\prime} }[/math] that sends a continuous linear functional f on H to the continuous antilinear functional denoted by f and defined by x ↦ f (x).
Fundamental theorem
- Fundamental theorem of Hilbert spaces:[1] Suppose that (H, B) is a Hausdorff pre-Hilbert space where B : H × H → [math]\displaystyle{ \mathbb{C} }[/math] is a sesquilinear form that is linear in its first coordinate and antilinear in its second coordinate. Then the canonical linear mapping from H into the anti-dual space of H is surjective if and only if (H, B) is a Hilbert space, in which case the canonical map is a surjective isometry of H onto its anti-dual.
See also
- Complex conjugate vector space
- Dual system
- Hilbert space
- Pre-Hilbert space
- Linear map
- Riesz representation theorem
- Sesquilinear form
References
- Narici, Lawrence; Beckenstein, Edward (2011). Topological Vector Spaces. Pure and applied mathematics (Second ed.). Boca Raton, FL: CRC Press. ISBN 978-1584888666. OCLC 144216834.
- Schaefer, Helmut H.; Wolff, Manfred P. (1999). Topological Vector Spaces. GTM. 8 (Second ed.). New York, NY: Springer New York Imprint Springer. ISBN 978-1-4612-7155-0. OCLC 840278135.
- Trèves, François (August 6, 2006). Topological Vector Spaces, Distributions and Kernels. Mineola, N.Y.: Dover Publications. ISBN 978-0-486-45352-1. OCLC 853623322.
Original source: https://en.wikipedia.org/wiki/Fundamental theorem of Hilbert spaces.
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