Definition

Let AA be a densely defined on a complex with Ax,xmx2\langle Ax,x\rangle\geq m\lVert x\rVert^2 for some real mm. The form

a[x,y]=Ax,y,x,yD(A),\mathfrak a[x,y]=\langle Ax,y\rangle,\qquad x,y\in\mathcal D(A),

is closable. The Friedrichs extension AFA_F is the unique self-adjoint operator associated by the representation theorem to the resulting . It is a of AA and satisfies AFmIA_F\geq mI. Thus it preserves the original lower bound while replacing the initial operator domain by the domain determined by the closed form.

Construction from the form norm

Choose c>1mc>1-m and complete D(A)\mathcal D(A) in the norm

xa,c2=Ax,x+cx2.\lVert x\rVert_{\mathfrak a,c}^2 =\langle Ax,x\rangle+c\lVert x\rVert^2.

The closure of a\mathfrak a has this completion as its form domain. The first representation theorem then produces AFA_F, characterized by

a[x,y]=AFx,y\overline{\mathfrak a}[x,y]=\langle A_Fx,y\rangle

for xD(AF)x\in\mathcal D(A_F) and every yy in the form domain. Different admissible values of cc give equivalent form norms and the same extension Kato, Chapter VI, §2.

Canonical but not generally unique

The Friedrichs construction depends only on the semibounded symmetric operator and selects an extension with the same . It does not say that AA has only one self-adjoint extension. Other boundary conditions may produce other semibounded extensions. Among nonnegative self-adjoint extensions, the Friedrichs and Kreĭn–von Neumann extensions occupy opposite extremal positions in the standard form or resolvent order; they coincide when the original operator is essentially self-adjoint.

Example

Let A=d2/dx2A=-d^2/dx^2 on L2(0,1)L^2(0,1) with initial domain Cc(0,1)C_c^\infty(0,1). Its quadratic form is

a[f,g]=01f(x)g(x)dx.\mathfrak a[f,g]=\int_0^1 f'(x)\overline{g'(x)}\,dx.

The form closure has domain H01(0,1)H_0^1(0,1), and its associated operator is the Dirichlet Laplacian with domain H2(0,1)H01(0,1)H^2(0,1)\cap H_0^1(0,1). This is the Friedrichs extension; Neumann and periodic Laplacians are other self-adjoint realizations but are not selected by closing this initial form.

References
  1. Tosio Kato, Perturbation Theory for Linear Operators, 2nd ed., Springer, 1995. DOI record. Relevant: Chapter VI, §§1–2 on closed forms and representation theorems.
  2. Konrad Schmüdgen, Unbounded Self-adjoint Operators on Hilbert Space, Graduate Texts in Mathematics 265, Springer, 2012. DOI record. Relevant: Chapter 10 on the Friedrichs extension.