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Hilbert–Schmidt operator

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In mathematics, a Hilbert–Schmidt operator, named for David Hilbert and Erhard Schmidt, is a bounded operator A on a Hilbert space H with finite Hilbert–Schmidt norm

∥ A ∥ H S 2 = T r ( A ∗ A ) := ∑ i ∈ I ∥ A e i ∥ 2

where ∥   ∥ is the norm of H, { e i : i ∈ I } an orthonormal basis of H, and Tr is the trace of a nonnegative self-adjoint operator. Note that the index set need not be countable. This definition is independent of the choice of the basis, and therefore

∥ A ∥ H S 2 = ∑ i , j | A i , j | 2 = ∥ A ∥ 2 2

for A i , j = ⟨ e i , A e j ⟩ and ∥ A ∥ 2 the Schatten norm of A for p = 2. In Euclidean space ∥   ∥ H S is also called Frobenius norm, named for Ferdinand Georg Frobenius.

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

⟨ A , B ⟩ H S = Tr ⁡ ( A ∗ B ) = ∑ i ⟨ A e i , B e i ⟩ .

The Hilbert–Schmidt operators form a two-sided *-ideal in the Banach algebra of bounded operators on H. They also form a Hilbert space, which can be shown to be naturally isometrically isomorphic to the tensor product of Hilbert spaces

H ∗ ⊗ H ,

where H∗ is the dual space of H.

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

An important class of examples is provided by Hilbert–Schmidt integral operators.

Hilbert–Schmidt operators are nuclear operators of order 2, and are therefore compact.

References

Hilbert–Schmidt operator Wikipedia


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