Math 2.0

Operator theory Definition

Toeplitz operator

Builds on Hardy spaceOrthogonal projectionToeplitz matrix

Definition

Let 𝕋\mathbb{T} be the unit circle with normalised Lebesgue measure, and let L2=L2(𝕋)L^2 = L^2(\mathbb{T}) (Lp space). Let H2βŠ†L2H^2 \subseteq L^2 be the Hardy space, the closed subspace of functions whose Fourier coefficients of negative index vanish. Let P ⁣:L2β†’H2P \colon L^2 \to H^2 be the orthogonal projection. For Ο†βˆˆL∞(𝕋)\varphi \in L^\infty(\mathbb{T}), the Toeplitz operator with symbol Ο†\varphi is the operator Tφ ⁣:H2β†’H2T_\varphi \colon H^2 \to H^2 given by TΟ†f=P(Ο†f).T_\varphi f = P(\varphi f).

Remarks

TΟ†T_\varphi is a bounded linear operator, and in fact βˆ₯TΟ†βˆ₯=βˆ₯Ο†βˆ₯∞\norm{T_\varphi} = \norm{\varphi}_\infty. With respect to the orthonormal basis en(t)=einte_n(t) = e^{int}, nβ‰₯0n \ge 0, its matrix entries are ⟨TΟ†ek,ej⟩=Ο†^(jβˆ’k)\ip{T_\varphi e_k}{e_j} = \hat\varphi(j - k), so the matrix is a Toeplitz matrix. If Ο†\varphi is continuous and has no zeros on 𝕋\mathbb{T}, then TΟ†T_\varphi is a Fredholm operator whose index is minus the winding number of Ο†\varphi around 00.

Example: Ο†(eit)=eit\varphi(e^{it}) = e^{it}. For f∈H2f \in H^2 the product Ο†f\varphi f has no negative Fourier coefficients, so P(Ο†f)=Ο†fP(\varphi f) = \varphi f and TΟ†T_\varphi is the shift operator f↦zff \mapsto z f.

Non-example: for Ο†(eit)=eβˆ’it\varphi(e^{it}) = e^{-it}, plain multiplication by Ο†\varphi does not map H2H^2 into itself, since it sends 11 to eβˆ’itβˆ‰H2e^{-it} \notin H^2. So the projection PP in the definition cannot be omitted; the Toeplitz operator TΟ†T_\varphi is the backward shift.

Reading path

To understand this page from the ground up, read these 15 pages in order. The foundations come first.

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  1. Hardy space concept
  2. Toeplitz matrix concept
  3. Vector space definition
  4. Inner product definition
  5. Linear map definition
  6. Linear subspace definition
  7. Orthogonal vectors definition
  8. Endomorphism definition
  9. Sum of subspaces definition
  10. Orthogonal complement definition
  11. Direct sum of subspaces definition
  12. A space is the direct sum of a subspace and its orthogonal complement statement
  13. Projection definition
  14. Orthogonal projection definition
  15. Toeplitz operator definition

Further reading

  1. Web https://en.wikipedia.org/wiki/Toeplitz_operator
About this page
Tag3VCD0T7QNG
URIm2://3VCD0T7QNG
Kinddefinition
WritingW0 stub
MSC47B35, 30H10
DefinesToeplitz operator
UsesHardy space, Orthogonal projection, Toeplitz matrix
Changed2 November 2026

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