Math 2.0

Operator theory Definition

Symmetric operator

Builds on Hilbert spaceDensely defined operator

Definition

Let HH be a complex Hilbert space. Let T ⁣:D(T)→HT \colon D(T) \to H be a densely defined linear operator, where the domain D(T)D(T) is a dense linear subspace of HH. The operator TT is symmetric when ⟨Tx,y⟩=⟨x,Ty⟩for all x,y∈D(T).\ip{Tx}{y} = \ip{x}{Ty} \quad \text{for all } x, y \in D(T).

Remarks

Example: on H=L2(0,1)H = L^2(0, 1) let D(T)D(T) be the smooth functions with compact support in (0,1)(0, 1) and Tf=−if′Tf = -i f'. For f,g∈D(T)f, g \in D(T), integration by parts with vanishing boundary terms gives ∫01−if′gˉ=∫01f −ig′‾\int_0^1 -i f' \bar g = \int_0^1 f \, \overline{-i g'}, so TT is symmetric.

Non-example: on the same domain, Sf=f′Sf = f' satisfies ⟨Sf,g⟩=−⟨f,Sg⟩\ip{Sf}{g} = -\ip{f}{Sg}, so ⟨Sf,g⟩≠⟨f,Sg⟩\ip{Sf}{g} \ne \ip{f}{Sg} whenever ⟨f,Sg⟩≠0\ip{f}{Sg} \ne 0; it is skew-symmetric, not symmetric.

An equivalent form: TT is symmetric if and only if its adjoint T∗T^* extends TT, written T⊆T∗T \subseteq T^*. TT is self-adjoint when moreover T∗=TT^* = T, including equality of domains. By the Hellinger–Toeplitz theorem, a symmetric operator with D(T)=HD(T) = H is bounded, and then it is self-adjoint. Some authors, and Mathlib, call a linear map T ⁣:E→ET \colon E \to E on an inner product space symmetric when the identity holds on all of EE, without a domain.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Self-adjoint_operator
About this page
TagKR4KX354JN
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Kinddefinition
WritingW0 stub
MSC47B25, 47B02
DefinesSymmetric operator
UsesHilbert space, Densely defined operator
Changed2 November 2026

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