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
- {\displaystyle \int _{\Omega }\int _{\Omega }|k(x,y)|^{2},円dx,円dy<\infty ,}
is called a Hilbert–Schmidt kernel. The associated integral operator T : L2(Ω) → L2(Ω) given by
- {\displaystyle (Tf)(x)=\int _{\Omega }k(x,y)f(y),円dy}
is called a Hilbert–Schmidt integral operator.[1] [2] T is a Hilbert–Schmidt operator with Hilbert–Schmidt norm
- {\displaystyle \Vert T\Vert _{\mathrm {HS} }=\Vert k\Vert _{L^{2}}.}
Hilbert–Schmidt integral operators are both continuous and compact.[3]
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 ×ばつ X), then the operator T : L2(X) → L2(X) defined by
- {\displaystyle (Tf)(x)=\int _{X}k(x,y)f(y),円dy}
is compact. If
- {\displaystyle 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.[4]
See also
[edit ]Notes
[edit ]- ^ Simon 1978, p. 14.
- ^ Bump 1998, pp. 168.
- ^ Renardy & Rogers 2004, pp. 260, 262.
- ^ Bump 1998, pp. 168–185.
References
[edit ]- Renardy, Michael; Rogers, Robert C. (2004年01月08日). 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.