Abstract Hilbert-Schmidt Operators
Hilbert-Schmidt operators are a special class of compact operators that play an important role in functional analysis and quantum mechanics. They can be thought of as infinite-dimensional analogues of matrices with finite Frobenius norm.
Hilbert-Schmidt Operator
An operator on a Hilbert space \newcommand{\H}{\mathcal{H}} is called Hilbert-Schmidt if its Hilbert-Schmidt norm
e.g.
- In , the Hilbert–Schmidt norm is identical to the Frobenius norm.
Proposition
The product of two Hilbert-Schmidt operators is a trace class operator. Thus we can define the Hilbert–Schmidt inner product of two Hilbert-Schmidt operators as
Proposition
Suppose \H is a complex Hilbert space. Then the space of all Hilbert-Schmidt operators, denoted or , is an two-sided -ideal in the Banach algebra . Moreover, is isometrically isomorphic to the Hilbert space tensor product \overline{\H} \otimes \H, where \overline{\H} is the conjugate Hilbert space of \H.
This means for each Hilbert-Schmidt operator , we can define a bilinear form \beta_{T}\colon \H \times \H \to \C,\quad (x,y) \mapsto \langle x, Ty \rangle_{\H}.
Proof
Integral Operators
Integral Operator
On \newcommand{\R}{\mathbb{R}}L^{2}(\R^d), we can define an operator by the formula we call it an integral operator with associated kernel , where is a measurable function such that for almost every .
Proposition
An integral operator is Hilbert-Schmidt if the associated kernel is an element of .
Proposition
Let be a Hilbert-Schmidt operator on with kernel . Then
- for every , and almost every , the function is integrable.
- is bounded, and .
- the adjoint of is also a Hilbert-Schmidt operator with kernel .