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TheoremStatement: AI-adaptedProof: AI-adaptedPipeline-generatedaudited 2026-09-22
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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 Uσ(T); equivalently the support of E is σ(T);
  2. uniqueness: if ΛC is nonempty and compact and E is a regular projection valued measure on the Borel σ-algebra of Λ with zdE(z)=T, then E(Λσ(T))=0 and E(B)=E(B) for every Borel set Bσ(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)=fdE; for every bounded Borel h one has h(T)x,y=hdEx,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)x2 is a positive measure; for a nonnegative measurable g one has gdEx=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 Λσ(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 ΛC, and for compact ΛC the distance function zd(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 Uσ(T), and a regular PVM E on a nonempty compact ΛC with zdE(z)=T.

1.1

Suppose Uσ(T) is nonempty and relatively open with E(U)=0; choose λU and r>0 with σ(T){zλ<r}U and put q(z):=max{0,rzλ} on σ(T). Then q is continuous, q0, q(λ)=r=q because λσ(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.

A1A2
1.2

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)=(pσ(T))(T)=ΦE(pσ(T)); hence the bounded linear maps fΦE(f) and fΦE(fσ(T)) on C(Λ;C) agree on the uniformly dense family of *-polynomials and therefore on all continuous f.

A1A5
2.1

Consequently ΦE(q)=0 for q(z):=d(z,σ(T)), since q is continuous on Λ with qσ(T)=0; then qdEx=ΦE(q)x,x=0 with q0, so q=0 Ex-almost everywhere and Ex(Λσ(T))=0; as E(Λσ(T))x2=Ex(Λσ(T))=0 for every x, one gets E(Λσ(T))=0.

step 1.2A2A3A5
3.1

The restriction E(B):=E(B) for Borel Bσ(T) is a regular PVM on σ(T) with E(σ(T))=E(Λ)E(Λσ(T))=I and ΦE(z)=ΦE(z)ΦE(z1Λσ(T))=T0=T, because functions supported in the E-null set Λσ(T) integrate to 0; by the uniqueness clause of the spectral theorem E=E, so E(B)=E(B) for every Borel Bσ(T).

step 2.1A2A4
4.1

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.

step 1.1step 3.1A6

Depends on

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Sources