Hilbert–Schmidt integral operator explained

In mathematics, a Hilbert–Schmidt integral operator is a type of integral transform. Specifically, given a domain in -dimensional Euclidean space, then the square-integrable function belonging to such that

\int\Omega\int\Omega|k(x,y)|2dxdy<infty,

is called a Hilbert–Schmidt kernel and the associated integral operator given by

(Tf)(x)=\int\Omegak(x,y)f(y)dy,f\inL2(\Omega),

is called a Hilbert–Schmidt integral operator.Then is a Hilbert–Schmidt operator with Hilbert–Schmidt norm

\VertT\VertHS=\Vertk

\Vert
L2

.

Hilbert–Schmidt integral operators are both continuous and compact.

The concept of a Hilbert–Schmidt operator may be extended to any locally compact Hausdorff spaces. Specifically, let be a separable Hilbert space and a locally compact Hausdorff space equipped with a positive Borel measure. The initial condition on the kernel on can be reinterpreted as demanding belong to . Then the operator

(Tf)(x)=\intXk(x,y)f(y)dy,

is compact. If

k(x,y)=\overline{k(y,x)},

then is also self-adjoint and so the spectral theorem applies. This is one of the fundamental constructions of such operators, which often reduces problems about infinite-dimensional vector spaces to questions about well-understood finite-dimensional eigenspaces.

See also

References