Math 2.0

Operator theory Definition

Friedrichs extension

Builds on Hilbert spaceDensely defined operatorSymmetric operatorSesquilinear formSelf-adjoint operator

Definition

Let HH be a complex Hilbert space with inner product ⟨⋅,⋅⟩\ip{\cdot}{\cdot}. Let TT be a densely defined symmetric operator on HH with domain D(T)D(T). Assume that TT is bounded below: there is a real number cc with ⟨Tx,x⟩≥c∥x∥2\ip{Tx}{x} \ge c \norm{x}^2 for all x∈D(T)x \in D(T). On D(T)D(T), put ⟨x,y⟩T=⟨Tx,y⟩+(1−c)⟨x,y⟩.\ip{x}{y}_T = \ip{Tx}{y} + (1 - c)\ip{x}{y}. This is an inner product on D(T)D(T), and its norm satisfies ∥x∥T≥∥x∥\norm{x}_T \ge \norm{x}. Let HTH_T be the completion of D(T)D(T) for ∥⋅∥T\norm{\cdot}_T. The inclusion of D(T)D(T) into HH extends to an injective map from HTH_T into HH, so HTH_T is a subspace of HH. The Friedrichs extension of TT is the operator TFT_F with domain D(TF)={x∈HT:there is z∈H with ⟨x,y⟩T=⟨z+(1−c)x,y⟩ for all y∈HT},D(T_F) = \set{x \in H_T : \text{there is } z \in H \text{ with } \ip{x}{y}_T = \ip{z + (1 - c)x}{y} \text{ for all } y \in H_T}, given by TFx=zT_F x = z.

Remarks

The operator TFT_F is a self-adjoint extension of TT, and ⟨TFx,x⟩≥c∥x∥2\ip{T_F x}{x} \ge c \norm{x}^2 for all x∈D(TF)x \in D(T_F). An equivalent description is that TFT_F is the restriction of the adjoint T∗T^* to D(T∗)∩HTD(T^*) \cap H_T. The space HTH_T is the form domain of TFT_F, and the sesquilinear form (x,y)↦⟨Tx,y⟩(x, y) \mapsto \ip{Tx}{y} extends to it.

Example: on H=L2(0,1)H = L^2(0, 1), let Tf=−f′′T f = -f'' on smooth functions with compact support in (0,1)(0, 1). Integration by parts gives ⟨Tf,f⟩=∫01∣f′∣2 dx≥0\ip{Tf}{f} = \int_0^1 \abs{f'}^2 \, dx \ge 0, so c=0c = 0 works. The space HTH_T is the Sobolev space H01(0,1)H^1_0(0, 1), and TFf=−f′′T_F f = -f'' on D(TF)=H2(0,1)∩H01(0,1)D(T_F) = H^2(0, 1) \cap H^1_0(0, 1), the Dirichlet Laplacian.

Non-example: on L2(0,∞)L^2(0, \infty), let Sf=−if′S f = -i f' on smooth functions with compact support in (0,∞)(0, \infty). It is symmetric, but ⟨Sf,f⟩\ip{Sf}{f} is not bounded below by any c∥f∥2c \norm{f}^2, so the construction does not apply. In fact the deficiency indices of SS are unequal, so SS has no self-adjoint extension at all.

Reading path

To understand this page from the ground up, read these 6 pages in order. The foundations come first.

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  1. Densely defined operator concept
  2. Hilbert space concept
  3. Self-adjoint operator concept
  4. Sesquilinear form concept
  5. Symmetric operator concept
  6. Friedrichs extension definition

Further reading

  1. Web https://en.wikipedia.org/wiki/Friedrichs_extension
About this page
TagNZ8WECT409
URIm2://NZ8WECT409
Kinddefinition
WritingW0 stub
MSC47B25, 47A20, 47A07
DefinesFriedrichs extension
UsesHilbert space, Densely defined operator, Symmetric operator, Sesquilinear form, Self-adjoint operator
Changed2 November 2026

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