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In [[mathematics]], the concept of a '''Hilbert space''', named after [[David Hilbert]], generalizes the notion of [[Euclidean space]].

== Description ==

Hilbert space extends the methods of [[vector algebra]] and [[calculus]] from the two-dimensional Euclidean plane and three-dimensional space to spaces with any finite or infinite number of dimensions. 

A Hilbert space is an [[abstract vector space]] possessing the structure of an inner product that allows length and angle to be measured. Furthermore, Hilbert spaces are complete: there are enough limits in the space to allow the techniques of calculus to be used.

Hilbert spaces arise naturally and frequently in [[mathematics]] and [[physics]], typically as infinite-dimensional function spaces. The earliest Hilbert spaces were studied from this point of view in the first decade of the 20th century by [[David Hilbert]], [[Erhard Schmidt]], and [[Frigyes Riesz]].

They are indispensable tools in the theories of [[Partial differential equation|partial differential equations]], quantum mechanics, [[Fourier analysis]] (which includes applications to [[signal processing]] and heat transfer)—and [[ergodic theory]], which forms the mathematical underpinning of thermodynamics.

The success of Hilbert space methods ushered in a very fruitful era for [[functional analysis]].

[[John von Neumann]] coined the term Hilbert space for the abstract concept that underlies many of these diverse applications.

Apart from the classical Euclidean spaces, examples of Hilbert spaces include spaces of square-integrable functions, spaces of sequences, Sobolev spaces consisting of generalized functions, and Hardy spaces of holomorphic functions.

Geometric intuition plays an important role in many aspects of Hilbert space theory. Exact analogs of the Pythagorean theorem and parallelogram law hold in a Hilbert space.

At a deeper level, perpendicular projection onto a subspace (the analog of "dropping the altitude" of a triangle) plays a significant role in optimization problems and other aspects of the theory. An element of a Hilbert space can be uniquely specified by its coordinates with respect to a set of coordinate axes (an orthonormal basis), in analogy with Cartesian coordinates in the plane. When that set of axes is countably infinite, this means that the Hilbert space can also usefully be thought of in terms of the space of infinite sequences that are square-summable. The latter space is often in the older literature referred to as the Hilbert space.

Linear operators on a Hilbert space are likewise fairly concrete objects: in good cases, they are simply transformations that stretch the space by different factors in mutually perpendicular directions in a sense that is made precise by the study of their spectrum.

== See also ==

* [[Hadamard space]]
* [[Hilbert algebra]]
* [[Hilbert C*-module]]
* [[Hilbert manifold]]
* [[Operator theory]]
* [[Operator topologies]]
* [[Rigged Hilbert space]]

== External links ==

* [https://en.wikipedia.org/wiki/Hilbert_space Hilbert space] @ Wikipedia


[[Category:Mathematics]]