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A bounded form is represented by a unique bounded operator

Statement

Assume Countable Choice (The Axiom of Countable Choice (ACω)), used through Riesz representation for Hilbert spaces. Let H be a real or complex Hilbert space and let a be a bounded sesquilinear form on H with bound M in the sense of Bounded, coercive and symmetric sesquilinear forms. Then there is a unique bounded linear operator A∈B(H) with a(u,v)=(Au,v)for all u,v∈H, and ∥A∥≤M; if M is the least bound of a then ∥A∥=M. The map a↦A is linear, and a is coercive with constant α if and only if Re⁡(Au,u)≥α∥u∥2 for all u. For the adjoint form one has a∗(u,v)=(A∗u,v), where A∗ is the Hilbert adjoint of The Hilbert-space adjoint of a bounded operator.

Facts & Assumptions

Given: Countable Choice; a real or complex Hilbert space H with inner product (⋅,⋅) linear in the first argument and conjugate-linear in the second; a sesquilinear form a on H, linear in the first argument and conjugate-linear in the second, with bound M≥0.

[F1]

Bounded and sesquilinear: a(u,λv)=λ‾ a(u,v), a(λu,v)=λ a(u,v), a(u+u′,v)=a(u,v)+a(u′,v), and ∣a(u,v)∣≤M∥u∥ ∥v∥ for all u,v∈H (Bounded, coercive and symmetric sesquilinear forms).

[F2]

Inner-product facts: (v,w)=(w,v)‾, positive definiteness (so a vector orthogonal to all of H is 0), and Cauchy--Schwarz ∣(u,v)∣≤∥u∥ ∥v∥; the inner product is linear in the first slot and conjugate-linear in the second (Real and complex inner-product spaces and their induced length, Cauchy–Schwarz: ∣⟨x,y⟩∣≤∥x∥ ∥y∥, with equality exactly for dependent pairs, Hilbert space).

[F3]

Riesz representation under Countable Choice: every bounded linear functional f on H has a unique y∈H with f(x)=(x,y) for all x, and ∥f∥=∥y∥ (Riesz representation for Hilbert spaces, The Axiom of Countable Choice (ACω), The operator norm as the least bound and as the unit-sphere or unit-ball supremum).

[F4]

Bounded operators and the operator norm: T is bounded when some C≥0 has ∥Tx∥≤C∥x∥, and ∥T∥=sup⁡∥x∥≤1∥Tx∥ is its least bound (A bounded linear operator between normed spaces, The operator norm as the least bound and as the unit-sphere or unit-ball supremum).

[F5]

Hilbert adjoint: there is a unique A∗∈B(H) with (Au,v)=(u,A∗v) for all u,v∈H (The Hilbert-space adjoint of a bounded operator, Hilbert-adjoint identities).

Proof

1.1F1F2

For fixed u∈H the map fu(v):=a(u,v)‾ is linear in v and bounded: fu(λv)=a(u,λv)‾=λ‾a(u,v)‾=λfu(v) and, more generally, conjugate-linearity of a in the second slot makes fu additive, while ∣fu(v)∣=∣a(u,v)∣≤M∥u∥ ∥v∥ shows that ∥fu∥≤M∥u∥.

2.1F2F3step 1.1

Riesz representation defines A: by [F3] there is a unique Au∈H with fu(v)=(v,Au) for every v, that is a(u,v)‾=(v,Au), and ∥Au∥=∥fu∥≤M∥u∥. Conjugating the representing identity with the conjugate symmetry of the inner product gives a(u,v)=(v,Au)‾=(Au,v) for all v; so every u is assigned a unique vector Au with a(u,v)=(Au,v) for all u,v, and in particular ∥Au∥≤M∥u∥.

3.1F1F2F4step 2.1

A is linear: for scalars s,t and u,w∈H, first-slot linearity of a gives a(su+tw,v)=s a(u,v)+t a(w,v) for every v, hence (A(su+tw),v)=s(Au,v)+t(Aw,v)=(sAu+tAw,v) by linearity of the inner product in its first slot, and positive definiteness forces A(su+tw)=sAu+tAw. Therefore A is linear and, by step 2.1, bounded with ∥A∥≤M.

3.2F2step 2.1

A is unique: if B∈B(H) also satisfies a(u,v)=(Bu,v) for all u,v, then (Au−Bu,v)=0 for every v, and positive definiteness gives Au=Bu for every u, that is A=B. The assignment a↦A is linear: for forms a,b with operators A,B and a scalar c, (Aa+cbu,v)=(a+cb)(u,v)=(Au,v)+c(Bu,v)=((A+cB)u,v) for all v, so Aa+cb=A+cB by the same uniqueness argument.

4.1F1F2F4step 3.1algebra

Least bound and coercivity: if M is the least bound of a, then for all u,v∈H one has ∣a(u,v)∣=∣(Au,v)∣≤∥Au∥ ∥v∥≤∥A∥ ∥u∥ ∥v∥, so ∥A∥ is itself a bound of a and M≤∥A∥; with step 3.1 this gives ∥A∥=M. Also, substituting v=u in a(u,v)=(Au,v) gives a coercive with constant α>0 if and only if Re⁡(Au,u)≥α∥u∥2 for every u.

5.1F2F5∎

Adjoint form: for all u,v∈H, a∗(u,v)=a(v,u)‾=(Av,u)‾=(u,Av)=(A∗u,v) by conjugate symmetry of the inner product and the defining identity (Av,u)=(v,A∗u) of the Hilbert adjoint; hence the adjoint form is represented by A∗.

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