Hilbert–Schmidt integral operator

In mathematics, a Hilbert–Schmidt integral operator is a type of integral transform. Specifically, given a domain Ω in Rⁿ, any k : Ω × Ω → C such that

$\int _{\Omega }\int _{\Omega }|k(x,y)|^{2}\,dx\,dy<\infty ,$

is called a Hilbert–Schmidt kernel. The associated integral operator T : L²(Ω) → L²(Ω) given by

$(Tf)(x)=\int _{\Omega }k(x,y)f(y)\,dy$

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

$\Vert T\Vert _{\mathrm {HS} }=\Vert k\Vert _{L^{2}}.$

Hilbert–Schmidt integral operators are both continuous and compact.

The concept of a Hilbert–Schmidt integral operator may be extended to any locally compact Hausdorff space X equipped with a positive Borel measure. If L²(X) is separable, and k belongs to L²(X × X), then the operator T : L²(X) → L²(X) defined by

$(Tf)(x)=\int _{X}k(x,y)f(y)\,dy$

is compact. If

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

then T 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

• Hilbert–Schmidt operator

References

• Renardy, Michael; Rogers, Robert C. (2004-01-08). An Introduction to Partial Differential Equations. New York Berlin Heidelberg: Springer Science & Business Media. ISBN 0-387-00444-0.

• Bump, Daniel (1998). Automorphic Forms and Representations. Cambridge University Press. ISBN 0-521-65818-7.
• Simon, B. (1978). "An Overview of Rigorous Scattering Theory". S2CID 16913591.