Hilbert-schmidt Operator

In mathematics, a Hilbert-Schmidt operator is a bounded operator A on a Hilbert space H1->H2 such that there exists an orthonormal basis \{e_i : i \in I\} of H1 such that
\sum_{i\in I} \|Ae_i\|^2 < \infty
is finite. Let A and B are two Hilbert-Schmidt operators, the Hilbert-Schmidt inner product can be defined as \langle A,B \rangle_{HS} = \sum_{i \in I} \langle Ae_i, Be_i \rangle. This definition is independent of the choice of orthonormal basis The Hilbert-Schmidt operators form an ideal in the algebra of bounded operators on H, which is usually not closed in the norm topology. They also form a Hilbert space, and can be shown to be isometrically isomorphic to the tensor product of Hilbert spaces \overline{H} \otimes H.

 

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