Hilbert–Schmidt operator explained

A\colonH\toH

that acts on a Hilbert space

H

and has finite Hilbert–Schmidt norm

\|A\|^2_ \ \stackrel\ \sum_ \|Ae_i\|^2_H,

where

\{ei:i\inI\}

is an orthonormal basis.[1] The index set

I

need not be countable. However, the sum on the right must contain at most countably many non-zero terms, to have meaning. This definition is independent of the choice of the orthonormal basis. In finite-dimensional Euclidean space, the Hilbert–Schmidt norm

\|\|HS

is identical to the Frobenius norm.

||·|| is well defined

The Hilbert–Schmidt norm does not depend on the choice of orthonormal basis. Indeed, if

\{ei\}i\in

and

\{fj\}j\in

are such bases, then\sum_i \|Ae_i\|^2 = \sum_ \left| \langle Ae_i, f_j\rangle \right|^2 = \sum_ \left| \langle e_i, A^*f_j\rangle \right|^2 = \sum_j\|A^* f_j\|^2.If

ei=fi,

then \sum_i \|Ae_i\|^2 = \sum_i\|A^* e_i\|^2. As for any bounded operator,

A=A**.

Replacing

A

with

A*

in the first formula, obtain \sum_i \|A^* e_i\|^2 = \sum_j\|A f_j\|^2. The independence follows.

Examples

An important class of examples is provided by Hilbert–Schmidt integral operators. Every bounded operator with a finite-dimensional range (these are called operators of finite rank) is a Hilbert–Schmidt operator. The identity operator on a Hilbert space is a Hilbert–Schmidt operator if and only if the Hilbert space is finite-dimensional. Given any

x

and

y

in

H

, define

xy:H\toH

by

(xy)(z)=\langlez,y\ranglex

, which is a continuous linear operator of rank 1 and thus a Hilbert–Schmidt operator; moreover, for any bounded linear operator

A

on

H

(and into

H

),

\operatorname{Tr}\left(A\left(xy\right)\right)=\left\langleAx,y\right\rangle

.

If

T:H\toH

is a bounded compact operator with eigenvalues

\ell1,\ell2,...

of

|T|=\sqrt{T*T}

, where each eigenvalue is repeated as often as its multiplicity, then

T

is Hilbert–Schmidt if and only if \sum_^ \ell_i^2 < \infty, in which case the Hilbert–Schmidt norm of

T

is \left\| T \right\|_ = \sqrt.

If

k\inL2\left(\mu x \mu\right)

, where

\left(X,\Omega,\mu\right)

is a measure space, then the integral operator

K:L2\left(\mu\right)\toL2\left(\mu\right)

with kernel

k

is a Hilbert–Schmidt operator and

\left\|K\right\|\operatorname{HS

} = \left\| k \right\|_2.

Space of Hilbert–Schmidt operators

The product of two Hilbert–Schmidt operators has finite trace-class norm; therefore, if A and B are two Hilbert–Schmidt operators, the Hilbert–Schmidt inner product can be defined as

\langle A, B \rangle_\text = \operatorname(A^* B) = \sum_i \langle Ae_i, Be_i \rangle.

The Hilbert–Schmidt operators form a two-sided

in the Banach algebra of bounded operators on . They also form a Hilbert space, denoted by or, which can be shown to be naturally isometrically isomorphic to the tensor product of Hilbert spaces

H^* \otimes H,

where is the dual space of . The norm induced by this inner product is the Hilbert–Schmidt norm under which the space of Hilbert–Schmidt operators is complete (thus making it into a Hilbert space). The space of all bounded linear operators of finite rank (i.e. that have a finite-dimensional range) is a dense subset of the space of Hilbert–Schmidt operators (with the Hilbert–Schmidt norm).

The set of Hilbert–Schmidt operators is closed in the norm topology if, and only if, is finite-dimensional.

Properties

S:H1\toH2

and

T:H2\toH3

are Hilbert–Schmidt operators between Hilbert spaces then the composition

T\circS:H1\toH3

is a nuclear operator.

\left\|T\right\|\leq\left\|T\right\|\operatorname{HS

}.

\operatorname{Tr}

of the nonnegative self-adjoint operator

T*T

is finite, in which case
2
\|T\|
HS

=\operatorname{Tr}(T*T)

.[1]

\left\|S*\right\|\operatorname{HS

} = \left\| S \right\|_,

\left\|TS\right\|\operatorname{HS

} \leq \left\| T \right\| \left\| S \right\|_, and

\left\|ST\right\|\operatorname{HS

} \leq \left\| S \right\|_ \left\| T \right\|. In particular, the composition of two Hilbert–Schmidt operators is again Hilbert–Schmidt (and even a trace class operator).

B\left(H\right)

that contains the operators of finite-rank.

\{ei:i\inI\}

is an orthonormal basis of H, and

\|A\|2

is the Schatten norm of

A

for . In Euclidean space,

\|\|HS

is also called the Frobenius norm.

References

. John B. Conway. A course in functional analysis . Springer-Verlag . New York . 1990 . 978-0-387-97245-9 . 21195908.

. Helmut H. Schaefer. Topological Vector Spaces . Springer New York Imprint Springer . . 3 . New York, NY . 1999 . 978-1-4612-7155-0 . 840278135 .

Notes and References

  1. Web site: Moslehian . M. S. . Hilbert–Schmidt Operator (From MathWorld) .