Math 2.0

Operator theory Definition

Hilbert–Schmidt operator

Builds on Hilbert spaceOrthonormal basisContinuous linear map

Definition

Let HH and KK be Hilbert spaces and let A ⁣:H→KA \colon H \to K be a bounded linear operator. The operator AA is a Hilbert–Schmidt operator if there is an orthonormal basis (ei)i∈I(e_i)_{i \in I} of HH such that ∑i∈I∥Aei∥2<∞.\sum_{i \in I} \norm{A e_i}^2 < \infty. The Hilbert–Schmidt norm of AA is ∥A∥HS=(∑i∈I∥Aei∥2)1/2\norm{A}_{\mathrm{HS}} = \big( \sum_{i \in I} \norm{A e_i}^2 \big)^{1/2}.

Remarks

The condition and the value of the sum do not depend on the orthonormal basis. Indeed, for an orthonormal basis (fj)j∈J(f_j)_{j \in J} of KK, Parseval's identity gives ∑i∥Aei∥2=∑i∑j∣⟨Aei,fj⟩∣2=∑j∥A∗fj∥2\sum_i \norm{A e_i}^2 = \sum_i \sum_j \abs{\ip{A e_i}{f_j}}^2 = \sum_j \norm{A^* f_j}^2, and the right side does not involve (ei)(e_i).

Every Hilbert–Schmidt operator is compact and satisfies ∥A∥≤∥A∥HS\norm{A} \le \norm{A}_{\mathrm{HS}}. A compact operator is Hilbert–Schmidt if and only if its singular values σn\sigma_n satisfy ∑nσn2<∞\sum_n \sigma_n^2 < \infty, and then ∥A∥HS2=∑nσn2\norm{A}_{\mathrm{HS}}^2 = \sum_n \sigma_n^2. The Hilbert–Schmidt operators form the Schatten class S2S_2; every trace class operator is Hilbert–Schmidt. On L2L^2 spaces of σ\sigma-finite measure spaces, they are the integral operators with square-integrable kernels, and ∥A∥HS\norm{A}_{\mathrm{HS}} is the L2L^2 norm of the kernel.

Example: on ℓ2\ell^2, the operator A(x1,x2,… )=(x1,x2/2,x3/3,… )A(x_1, x_2, \dots) = (x_1, x_2/2, x_3/3, \dots) is Hilbert–Schmidt. For the standard basis, ∥Aen∥=1/n\norm{A e_n} = 1/n and ∑n1/n2=π2/6\sum_n 1/n^2 = \pi^2/6.

Non-example: on ℓ2\ell^2, the operator B(x1,x2,… )=(x1,x2/2,x3/3,… )B(x_1, x_2, \dots) = (x_1, x_2/\sqrt{2}, x_3/\sqrt{3}, \dots) is compact but not Hilbert–Schmidt, since ∑n∥Ben∥2=∑n1/n\sum_n \norm{B e_n}^2 = \sum_n 1/n diverges. The identity of an infinite-dimensional Hilbert space is not Hilbert–Schmidt either.

Reading path

To understand this page from the ground up, read these 4 pages in order. The foundations come first.

Show the path as a graph
Each page uses the pages above it. The colour of the bar on a box shows how strong the evidence is, and the box also gives it as text. The list has the same pages.
  • no evidence level
  1. Continuous linear map concept
  2. Hilbert space concept
  3. Orthonormal basis concept
  4. Hilbert–Schmidt operator definition

Further reading

  1. Web https://en.wikipedia.org/wiki/Hilbert%E2%80%93Schmidt_operator
About this page
TagNPBWWBGV37
URIm2://NPBWWBGV37
Kinddefinition
WritingW0 stub
MSC47B10, 45P05, 47G10
DefinesHilbert–Schmidt operator
UsesHilbert space, Orthonormal basis, Continuous linear map

Markdown · JSON · Edit on GitHub

What this page needs for W1

  • a source with a locator (0 of 1)

The writing levels say how complete the text of a page is. They do not measure its truth.

What links here

No page links to this page yet.