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Hilbert Basis


A Hilbert basis of a Hilbert space V is an orthonormal basis (e_i)_(i in I) for which every element v in V has an expansion converging in the norm of V,

 v=sum_(i in I)a_ie_i,

with sum_(i in I)|a_i|^2<infty. For each v, at most countably many coefficients a_i are nonzero. If V is a separable space, the orthonormal basis can be indexed by a finite set or countable set. A nonseparable Hilbert space requires an uncountable set of indices I.

For example, a Hilbert basis for the vector space of square summable sequences (a_n)=a_1, a_2, ... is given by the standard basis e_i, where the nth entry of e_i is delta_(in), the Kronecker delta. Then

 (a_n)=suma_ie_i,

with sum|a_i|^2<infty. The e_i are not a vector basis, because some elements are not a finite linear combination of them, but are a Hilbert basis.


See also

Fourier Series, Hilbert Space, L2-Space, Orthonormal Set, Vector Basis

Portions of this entry contributed by Todd Rowland

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Cite this as:

Weisstein, Eric W., with contributions by Todd Rowland. "Hilbert Basis." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/HilbertBasis.html

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