Alphabeta Math
TheoremStatement: AI-adaptedProof: AI-adaptedPipeline-generatedaudited 2026-09-22
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Support and uniqueness of the spectral measure

Statement

Assume AC. Let T be a bounded normal operator on a nonzero complex Hilbert space H with spectral projection valued measure E on the Borel σ-algebra of σ(T). Then:

  1. support: E(U)≠0 for every nonempty relatively open subset U⊆σ(T); equivalently the support of E is σ(T);
  2. uniqueness: if Λ⊆C is nonempty and compact and E′ is a regular projection valued measure on the Borel σ-algebra of Λ with ∫z dE′(z)=T, then E′(Λ∖σ(T))=0 and E′(B)=E(B) for every Borel set B⊆σ(T); in particular every scalar pairing ⟨E(⋅)x,y⟩ is determined by T.

Facts & Assumptions

[A1]

For every continuous f on σ(T) one has ∥f(T)∥=∥f∥∞ and f(T)=ΦE(f)=∫f dE; for every bounded Borel h one has ⟨h(T)x,y⟩=∫h dEx,y with Ex,y(B)=⟨E(B)x,y⟩. For every PVM F, its bounded integral ΦF is a unital star-homomorphism (Continuous functional calculus for bounded normal operators, Spectral theorem for bounded normal operators pvm form, Borel functional calculus for bounded normal operators, Pvm integral is a star homomorphism).

[A2]

The Borel calculus is multiplicative: (fg)(T)=f(T)g(T) for bounded Borel f,g, and E(B)=1B(T); in particular ΦE(g)=0 whenever g vanishes on a Borel set carrying the full projection (Borel functional calculus for bounded normal operators, Projection valued measure).

[A3]

Ex(B)=⟨E(B)x,x⟩=∥E(B)x∥2 is a positive measure; for a nonnegative measurable g one has ∫g dEx=0 if and only if g=0 Ex-almost everywhere (Scalar and complex measures from a pvm, A nonnegative measurable function has integral 0 exactly when it vanishes almost everywhere).

[A4]

E is the unique regular PVM on the Borel σ-algebra of σ(T) whose coordinate integral is T, and Λ∖σ(T) is a countable union of compact subsets of Λ (Spectral theorem for bounded normal operators pvm form, Continuous functional calculus produces a regular PVM, Regular Borel measure on an LCH space).

[A5]

The ∗-polynomials are uniformly dense in C(Λ;C) for compact Λ⊆C, and for compact Λ⊆C the distance function z↦d(z,σ(T)) is continuous, nonnegative, and vanishes exactly on σ(T) (Complex Stone–Weierstrass dichotomy for separating self-adjoint algebras; the unital case is dense).

[A6]

AC is the declared choice hypothesis of this page from the construction item onward (The Axiom of Choice).

Proof

technique · direct

Given: A nonzero complex Hilbert space H, a bounded normal operator T with spectral PVM E on σ(T), a nonempty relatively open U⊆σ(T), and a regular PVM E′ on a nonempty compact Λ⊆C with ∫z dE′(z)=T.

1.1A1A2

Suppose U⊆σ(T) is nonempty and relatively open with E(U)=0; choose λ∈U and r>0 with σ(T)∩{∣z−λ∣<r}⊆U and put q(z):=max⁡{0,r−∣z−λ∣} on σ(T). Then q is continuous, q≥0, q(λ)=r=∥q∥∞ because λ∈σ(T), and q vanishes outside U, so q1U=q and ΦE(q)=ΦE(q1U)=ΦE(q)ΦE(1U)=q(T)E(U)=0, whence ∥q(T)∥=0; by the isometry of the continuous calculus ∥q∥∞=∥q(T)∥=0, contradicting q(λ)=r>0.

1.2A1A5

For a *-polynomial p in z,z‾ on Λ one has ΦE′(p)=p(T,T∗), while the continuous calculus on σ(T) gives p(T,T∗)=(p∣σ(T))(T)=ΦE(p∣σ(T)); hence the bounded linear maps f↦ΦE′(f) and f↦ΦE(f∣σ(T)) on C(Λ;C) agree on the uniformly dense family of *-polynomials and therefore on all continuous f.

2.1step 1.2A2A3A5

Consequently ΦE′(q)=0 for q(z):=d(z,σ(T)), since q is continuous on Λ with q∣σ(T)=0; then ∫q dEx′=⟨ΦE′(q)x,x⟩=0 with q≥0, so q=0 Ex′-almost everywhere and Ex′(Λ∖σ(T))=0; as ∥E′(Λ∖σ(T))x∥2=Ex′(Λ∖σ(T))=0 for every x, one gets E′(Λ∖σ(T))=0.

3.1step 2.1A2A4

The restriction E′′(B):=E′(B) for Borel B⊆σ(T) is a regular PVM on σ(T) with E′′(σ(T))=E′(Λ)−E′(Λ∖σ(T))=I and ΦE′′(z)=ΦE′(z)−ΦE′(z1Λ∖σ(T))=T−0=T, because functions supported in the E′-null set Λ∖σ(T) integrate to 0; by the uniqueness clause of the spectral theorem E′′=E, so E′(B)=E(B) for every Borel B⊆σ(T).

4.1step 1.1step 3.1A6∎

The support of E is all of σ(T), and any regular PVM on a compact set whose coordinate integral is T agrees with E on σ(T) and vanishes off it; in particular all pairings of E are determined by T.

Depends on

Dependency tree · 2 levels

Sources