Original text: CC0 1.0. Prerequisite proofs and component terms.

Closing energy domains and comparing resolvents

CC0 1.0.

The operator applications use the complete closed-form representation and form-sum proofs, the self-adjoint spectral calculus and the bounded factorization lemma.

A quadratic expression on a convenient set of vectors does not yet determine a closed energy form. One must check whether limits in the energy norm still identify vectors uniquely in the original Hilbert space. This unit makes that test explicit, constructs the smallest closed extension, and explains which dense sets actually determine a form. It then recovers domain inclusion from the order of one pair of resolvents.

The mathematical antecedents include Takesaki, Theory of Operator Algebras II and III, Appendix A.8(ii), the core definition in A.8, A.10, and the remark following A.9. The course's proofs use an energy-space inclusion and a bounded factorization, organized around the domains required by later weight constructions.

OA-MOD-FC-01 — Objects and dependencies

Let HH be any complex Hilbert space, with inner product linear in its first variable. Let qq be a nonnegative sesquilinear form on a linear subspace D⊆HD\subseteq H. Density of DD is not assumed. Write

q[x]=q(x,x),∥x∥q2=∥x∥2+q[x]. q[x]=q(x,x),\qquad \|x\|_q^2=\|x\|^2+q[x].

A form rr extends qq if D⊆D(r)D\subseteq D(r) and r(x,y)=q(x,y)r(x,y)=q(x,y) for x,y∈Dx,y\in D. We call qq closable if it has a closed nonnegative extension on HH. Here closedness means completeness of the form domain in its form norm. Extension is a statement about domains and values; it does not mean the ordering of extended diagonals defined in OA-MOD-QF-02.

The first four results use only completion, bounded Hilbert-space adjoints, Riesz representation, and orthogonal complements. These facts are proved in Hilbert spaces and compact operators. They use neither a spectral theorem nor a von Neumann algebra.

The operator applications additionally use closed-form representation OA-MOD-QF-03, finite form sums OA-MOD-QF-10, and the exact self-adjoint Borel-calculus contract OA-MOD-DEP-SPECTRAL. The self-adjoint spectral-calculus proof is supplied in the linked programme provider. The order proof uses the bounded factorization proved in OA-MOD-DW-02. The last form-sum assertion uses the elementary reversal of graph inclusion under adjoints; its proof is recalled there.

OA-MOD-FC-02 — The completion test and canonical closure

Theorem. Complete the inner-product space (D,⟨⋅,⋅⟩q)(D,\langle\cdot,\cdot\rangle_q) to a Hilbert space VV, and denote its isometric dense inclusion by ι:D→V\iota:D\to V. There is a unique contraction j:V→Hj:V\to H satisfying jιx=xj\iota x=x. The following conditions are equivalent:

  1. qq has a closed nonnegative extension on HH.
  2. If xn∈Dx_n\in D, xn→0x_n\to0 in HH, and q[xn−xm]→0q[x_n-x_m]\to0 as n,m→∞n,m\to\infty, then q[xn]→0q[x_n]\to0.
  3. jj is injective.

When they hold, the closure q‾\overline q has the exact domain and values

D(q‾)=j(V),q‾(ju,jv)=⟨u,v⟩V−⟨ju,jv⟩H(u,v∈V). \begin{aligned} D(\overline q)&=j(V),\\ \overline q(ju,jv) &=\langle u,v\rangle_V-\langle ju,jv\rangle_H \qquad(u,v\in V). \end{aligned}

It is closed, extends qq, and its original domain DD is dense in D(q‾)D(\overline q) for the form norm. Every closed extension of qq extends q‾\overline q.

Proof. The inclusion D→HD\to H has norm at most one for the form norm, so it extends uniquely to the contraction jj.

Suppose rr is a closed extension. Under the hypotheses of condition 2, the sequence xnx_n is Cauchy for the rr-norm: its Hilbert-norm differences and its form differences both tend to zero. Completeness gives a limit in D(r)D(r). The continuous inclusion into HH identifies that limit as zero. Hence q[xn]=r[xn]→0q[x_n]=r[x_n]\to0. This proves 1⇒21\Rightarrow2.

If u∈ker⁡ju\in\ker j, choose xn∈Dx_n\in D with ιxn→u\iota x_n\to u in VV. Then xn→0x_n\to0 in HH and q[xn−xm]→0q[x_n-x_m]\to0. Condition 2 gives

∥u∥V2=lim⁡n(∥xn∥2+q[xn])=0. \|u\|_V^2=\lim_n\bigl(\|x_n\|^2+q[x_n]\bigr)=0.

Thus jj is injective. Conversely, a sequence as in condition 2 is Cauchy in the form norm, so ιxn\iota x_n converges to some u∈Vu\in V. Its Hilbert limit gives ju=0ju=0. Injectivity forces u=0u=0, proving condition 2.

Now assume injectivity. The displayed formula is well-defined because a vector of j(V)j(V) has a unique preimage. It is sesquilinear and nonnegative since jj is a contraction. Moreover,

∥ju∥2+q‾[ju]=∥u∥V2. \|ju\|^2+\overline q[ju]=\|u\|_V^2.

Thus jj, viewed as a map from VV onto the new form domain with its form norm, is an isometry onto a complete space. This proves closedness. Substitution of u=ιxu=\iota x and v=ιyv=\iota y shows extension. Density of ι(D)\iota(D) proves the asserted density in form norm.

Finally, let rr be any closed extension. For u∈Vu\in V, choose ιxn→u\iota x_n\to u. The sequence is Cauchy for the rr-norm and hence converges there to a vector y∈D(r)y\in D(r). In HH it converges to juju, so y=juy=ju. Passing to the limit in the rr-inner product, for two such sequences, proves r(ju,jv)=q‾(ju,jv)r(ju,jv)=\overline q(ju,jv). Hence rr extends q‾\overline q. □\square

The range j(V)j(V) need not be closed in HH. It is complete for a stronger norm. No bounded inverse j−1:j(V)→Vj^{-1}:j(V)\to V for the Hilbert norm is asserted.

An equivalent concrete description is useful:

D(q‾)={x∈H:some xn∈D converges to x in H,q[xn−xm]⟶0},q‾[x]=lim⁡nq[xn]. D(\overline q)= \left\{x\in H: \begin{array}{l} \text{some }x_n\in D\text{ converges to }x\text{ in }H,\\ q[x_n-x_m]\longrightarrow0 \end{array} \right\}, \qquad \overline q[x]=\lim_n q[x_n].

The completion theorem proves both existence and independence of the limit; Hilbert-norm convergence by itself does not.

OA-MOD-FC-03 — Closedness and lower semicontinuity on all vectors

For any form qq, define q~:H→[0,∞]\widetilde q:H\to[0,\infty] by q[x]q[x] on D(q)D(q) and +∞+\infty elsewhere.

Theorem. A nonnegative form is closed if and only if q~\widetilde q is lower semicontinuous in the norm topology of HH. No density hypothesis is required.

Proof of necessity without spectral calculus. If qq is closed, put V=D(q)V=D(q) with its form norm and let j:V→Hj:V\to H be its inclusion. For x∈Hx\in H, set

G(x)=sup⁡f∈H(2Re⁡⟨x,f⟩H−∥j∗f∥V2). G(x)=\sup_{f\in H} \left(2\operatorname{Re}\langle x,f\rangle_H -\|j^*f\|_V^2\right).

We claim that

G(x)=∥x∥2+q~[x]. G(x)=\|x\|^2+\widetilde q[x].

First, ran⁡j∗\operatorname{ran}j^* is dense in VV: a vector orthogonal to that range lies in ker⁡j={0}\ker j=\{0\}. If x=jux=ju, the expression in the supremum equals

2Re⁡⟨u,j∗f⟩V−∥j∗f∥V2=∥u∥V2−∥u−j∗f∥V2. 2\operatorname{Re}\langle u,j^*f\rangle_V-\|j^*f\|_V^2 =\|u\|_V^2-\|u-j^*f\|_V^2.

Density gives G(ju)=∥u∥V2=∥ju∥2+q[ju]G(ju)=\|u\|_V^2=\|ju\|^2+q[ju].

If G(x)=C<∞G(x)=C<\infty, the term f=0f=0 gives C≥0C\geq0. Varying a complex scalar multiplying ff, and minimizing the corresponding quadratic, gives

∣⟨x,f⟩∣2≤C∥j∗f∥V2(f∈H). |\langle x,f\rangle|^2\leq C\|j^*f\|_V^2 \qquad(f\in H).

When j∗f=0j^*f=0, the same conclusion follows by scaling the linear term: it must vanish. Therefore j∗f↦⟨x,f⟩j^*f\mapsto\langle x,f\rangle is a well-defined bounded conjugate-linear functional on the dense subspace ran⁡j∗\operatorname{ran}j^*. By Riesz representation it has the form ⟨u,j∗f⟩V\langle u,j^*f\rangle_V for some u∈Vu\in V. The adjoint identity then gives ⟨x,f⟩=⟨ju,f⟩\langle x,f\rangle=\langle ju,f\rangle for every ff, so x=jux=ju. Consequently G(x)=+∞G(x)=+\infty outside j(V)j(V), proving the claim.

Each function in the supremum defining GG is norm continuous and real-valued. Hence GG is lower semicontinuous. Subtraction of the continuous function x↦∥x∥2x\mapsto\|x\|^2 proves that q~\widetilde q is lower semicontinuous.

Proof of sufficiency. Let xnx_n be Cauchy in the form norm. It has a Hilbert-norm limit xx. The numbers q[xn]q[x_n] are bounded, so lower semicontinuity implies q~[x]<∞\widetilde q[x]<\infty, or x∈D(q)x\in D(q). For any ε>0\varepsilon>0, choose NN with q[xn−xm]≤ε2q[x_n-x_m]\leq\varepsilon^2 for n,m≥Nn,m\geq N. For each fixed n≥Nn\geq N, lower semicontinuity applied as m→∞m\to\infty gives

q[xn−x]≤lim inf⁡mq[xn−xm]≤ε2. q[x_n-x]\leq\liminf_m q[x_n-x_m]\leq\varepsilon^2.

Thus xn→xx_n\to x in the form norm. The domain is complete. □\square

The proof uses sequences only for completeness in a metric norm; it places no countability condition on a basis or on later families of forms. The supremum formula proves topological lower semicontinuity directly.

OA-MOD-FC-04 — Closability and lower semicontinuity on the given domain

Theorem. A nonnegative form qq on D⊆HD\subseteq H is closable if and only if the function x↦q[x]x\mapsto q[x] is lower semicontinuous on DD for the topology inherited from the Hilbert norm.

Equivalently, for every sequence xn∈Dx_n\in D with Hilbert-norm limit x∈Dx\in D,

q[x]≤lim inf⁡nq[xn]. q[x]\leq\liminf_n q[x_n].

Proof. If qq is closable, its closure is closed by OA-MOD-FC-02. The extended diagonal of that closure is lower semicontinuous by OA-MOD-FC-03. Restriction to DD gives the assertion.

Conversely, suppose the stated relative lower semicontinuity holds. Let xnx_n satisfy condition 2 of OA-MOD-FC-02. For fixed nn, the sequence xn−xmx_n-x_m lies in DD and converges in HH to xn∈Dx_n\in D. Hence

q[xn]≤lim inf⁡mq[xn−xm]. q[x_n]\leq\liminf_m q[x_n-x_m].

The right side is arbitrarily small for all sufficiently large nn, by the form-Cauchy hypothesis. Thus q[xn]→0q[x_n]\to0, and OA-MOD-FC-02 supplies a closed extension. □\square

The distinction between the two topologies of the assertion is substantive. A zero form on a proper dense subspace is closable. Its extension by infinity is not lower semicontinuous on HH, so the original form is not closed. Both claims are checked explicitly in OA-MOD-FC-08.

OA-MOD-FC-05 — Cores determine the domain, not just a dense set of vectors

For a closed form qq, a linear subspace E⊆D(q)E\subseteq D(q) is a form core if it is dense in D(q)D(q) for ∥⋅∥q\|\cdot\|_q.

Proposition. The restriction q∣Eq|_E is closable, and its closure is exactly qq if and only if EE is a form core. More generally, its closed domain is the closure of EE inside the form Hilbert space D(q)D(q), with the restricted form.

Proof. The original qq is a closed extension. Complete EE in the restricted form norm. Its completion is the closed subspace E‾∥⋅∥q\overline E^{\|\cdot\|_q} of the Hilbert space D(q)D(q). The inclusion of this subspace into HH is injective. OA-MOD-FC-02 therefore identifies the closure with exactly this subspace and this form. It equals qq precisely when the subspace is all of D(q)D(q). □\square

Spectral core proposition. Let A≥0A\geq0 be self-adjoint and qA[x]=∥A1/2x∥2q_A[x]=\|A^{1/2}x\|^2. Then D(A)D(A) is a form core. The subspace

Ecut=⋃n≥1EA([0,n])H E_{\mathrm{cut}} =\bigcup_{n\geq1} E_A([0,n])H

is both a form core for qAq_A and an operator core for AA. An operator core means density in D(A)D(A) for (∥x∥2+∥Ax∥2)1/2(\|x\|^2+\|Ax\|^2)^{1/2}.

Proof. For x∈D(A1/2)x\in D(A^{1/2}), write xn=EA([0,n])xx_n=E_A([0,n])x. It lies in D(A)D(A), and

∥x−xn∥qA2=∫(n,∞)(1+t) d⟨EA(t)x,x⟩⟶0. \|x-x_n\|_{q_A}^2 =\int_{(n,\infty)}(1+t)\,d\langle E_A(t)x,x\rangle \longrightarrow0.

The integral is finite because x∈D(A1/2)x\in D(A^{1/2}). The same truncations applied to x∈D(A)x\in D(A) give convergence in the operator graph norm by replacing 1+t1+t with 1+t21+t^2. This proves both assertions. □\square

Any operator core for AA is a form core: graph-norm convergence implies form-norm convergence because t≤1+t2t\leq1+t^2, and D(A)D(A) is already a form core. Mere density in HH is insufficient; a dense subspace can be closed and proper in the form norm, as OA-MOD-FC-08 demonstrates.

OA-MOD-FC-06 — One resolvent inequality recovers the whole form order

Theorem. For nonnegative self-adjoint operators A1,A2A_1,A_2 on HH, the following are equivalent:

  1. D(A21/2)⊆D(A11/2)D(A_2^{1/2})\subseteq D(A_1^{1/2}), and ∥A11/2x∥2≤∥A21/2x∥2\|A_1^{1/2}x\|^2\leq\|A_2^{1/2}x\|^2 on D(A21/2)D(A_2^{1/2}).
  2. For some λ>0\lambda>0, (A2+λI)−1≤(A1+λI)−1. (A_2+\lambda I)^{-1}\leq(A_1+\lambda I)^{-1}.
  3. The inequality in condition 2 holds for every λ>0\lambda>0.

The operators need not commute. The inequality in condition 1 is between forms, not an assertion that the unbounded operators have the same domain.

Proof. OA-MOD-QF-05 gives 1⇒31\Rightarrow3, and 3⇒23\Rightarrow2 is immediate. Fix a λ\lambda as in condition 2 and put

Bj=(Aj+λI)−1,j=1,2. B_j=(A_j+\lambda I)^{-1},\qquad j=1,2.

Both operators are bounded, positive, and injective. Apply the bounded factorization of OA-MOD-DW-02 to B2≤B1B_2\leq B_1. In that lemma's left-factor notation, B21/2=VB11/2B_2^{1/2}=V B_1^{1/2} for a contraction VV. Taking adjoints, using that the square roots are self-adjoint, gives

B21/2=B11/2C,C=V∗,∥C∥≤1. B_2^{1/2}=B_1^{1/2}C,\qquad C=V^*,\quad\|C\|\leq1.

The spectral calculus gives actual range equalities and norms

ran⁡Bj1/2=D(Aj1/2),∥Bj−1/2x∥2=λ∥x∥2+∥Aj1/2x∥2. \operatorname{ran}B_j^{1/2}=D(A_j^{1/2}),\qquad \|B_j^{-1/2}x\|^2 =\lambda\|x\|^2+\|A_j^{1/2}x\|^2.

For x∈D(A21/2)x\in D(A_2^{1/2}), let ξ=B2−1/2x\xi=B_2^{-1/2}x. Then

x=B21/2ξ=B11/2Cξ. x=B_2^{1/2}\xi=B_1^{1/2}C\xi.

Thus x∈D(A11/2)x\in D(A_1^{1/2}). Injectivity of B11/2B_1^{1/2} gives B1−1/2x=CξB_1^{-1/2}x=C\xi, and therefore

λ∥x∥2+∥A11/2x∥2=∥Cξ∥2≤∥ξ∥2=λ∥x∥2+∥A21/2x∥2. \lambda\|x\|^2+\|A_1^{1/2}x\|^2 =\|C\xi\|^2 \leq\|\xi\|^2 =\lambda\|x\|^2+\|A_2^{1/2}x\|^2.

Canceling the Hilbert-norm term proves condition 1. □\square

This argument reads the form domain directly from the range of a bounded square root. It does not infer domain inclusion from a pointwise inequality on a previously chosen common subspace.

OA-MOD-FC-07 — When a form sum equals an operator sum

Let A1,…,Am≥0A_1,\ldots,A_m\geq0 be self-adjoint, and assume

D=⋂k=1mD(Ak1/2) D=\bigcap_{k=1}^m D(A_k^{1/2})

is dense in HH. The sum q[x]=∑k∥Ak1/2x∥2q[x]=\sum_k\|A_k^{1/2}x\|^2 is closed on DD, by the finite-sum proof in OA-MOD-QF-10. Its representing nonnegative self-adjoint operator is the form sum, denoted AformA_{\mathrm{form}}.

Proposition. On Dalg=⋂kD(Ak)D_{\mathrm{alg}}=\bigcap_k D(A_k), the algebraic sum Sx=∑kAkxSx=\sum_k A_kx is a restriction of AformA_{\mathrm{form}}. If SS is densely defined and essentially self-adjoint on that domain, then

Aform=S‾. A_{\mathrm{form}}=\overline S.

Proof. If x∈Dalgx\in D_{\mathrm{alg}} and v∈Dv\in D, the spectral pairing identity gives

q(x,v)=∑k⟨Akx,v⟩=⟨Sx,v⟩. q(x,v)=\sum_k\langle A_kx,v\rangle =\langle Sx,v\rangle.

The graph characterization in OA-MOD-QF-03 yields x∈D(Aform)x\in D(A_{\mathrm{form}}) and Aformx=SxA_{\mathrm{form}}x=Sx. Since AformA_{\mathrm{form}} is closed, S‾⊆Aform\overline S\subseteq A_{\mathrm{form}}.

For densely defined operators, T⊆UT\subseteq U implies U∗⊆T∗U^*\subseteq T^*: the adjoint identity holding for every vector in the larger domain also holds in the smaller domain, with the same representing vector. If SS is essentially self-adjoint, both S‾\overline S and AformA_{\mathrm{form}} are self-adjoint. Taking adjoints of their inclusion gives the reverse inclusion. Hence equality holds. □\square

Density of DD alone does not assert essential self-adjointness of SS, or even density of DalgD_{\mathrm{alg}}. Those are separate hypotheses in the stated implication.

Editable source · Proof dependencies and component terms