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State-preserving symmetries implemented unitarily

Statement

Assume Countable Choice ACω, the hypothesis of GNS Hilbert reconstruction with invariant operator domain. Let G be a topological group with identity e. Let A be a unital complex star algebra with positive normalized state ω, and let α:G→Aut⁡∗(A) be a group action: each αg is a bijective complex-linear map preserving product, unit and involution, with αe=id and αgαh=αgh. Suppose ω(αg(a))=ω(a) for all g∈G and a∈A. Also suppose that, for every a,b∈A, the coefficient function g↦ω(b∗αg(a)) is continuous at e.

Use the GNS representation from GNS Hilbert reconstruction with invariant operator domain, with common dense domain Dω and cyclic vector Ωω. Then Ug[a]:=[αg(a)] extends to a strongly continuous unitary representation U:G→U(Hω), fixes Ωω, and satisfies

Ugπω(a)Ug−1∣Dω=πω(αg(a))(a∈A,g∈G).

Here strongly continuous means that g↦Ugξ is norm-continuous for every ξ∈Hω. No differentiability, generator domain or spectral theorem follows from these hypotheses alone.

Facts & Assumptions

Given: Countable Choice ACω, a topological group G, a unital complex star algebra A, a positive normalized state ω, a state-preserving action α by unital star automorphisms, and continuity at e of every g↦ω(b∗αg(a)).

[F1]

GNS Hilbert reconstruction with invariant operator domain: the state has a Hilbert-space GNS representation on a common invariant dense domain Dω=A/Nω, with πω(a)[b]=[ab], Ωω=[1A], and inner product ([a],[b])ω=ω(b∗a).

[A1]

By the action assumptions, each αg is a unital star automorphism, αgh=αg∘αh, and ω∘αg=ω; multiplication and inversion in the topological group are continuous.

[A2]

For every a,b∈A, the scalar function g↦ω(b∗αg(a)) is continuous at e.

Proof

technique · direct
1.1F1A1given

If n∈Nω, then ω((αgn)∗αgn)=ω(αg(n∗n))=ω(n∗n)=0, so αg(Nω)⊆Nω. Applying the same argument to g−1 gives equality. For a,b∈A, ([αg(a)],[αg(b)])ω=ω(αg(b∗a))=ω(b∗a), so [a]↦[αg(a)] is an isometry on Dω with inverse induced by αg−1; it extends uniquely to a unitary Ug on Hω. The action law gives UgUh=Ugh, and UgΩω=Ωω.

2.1F1A1step 1.1

For [b]∈Dω, Ugπω(a)Ug−1[b]=Ug[aαg−1(b)]=[αg(a)b]=πω(αg(a))[b], using the representation rule and multiplicativity of αg. This is the claimed covariance identity on the common domain.

2.2F1A1A2step 1.1algebra

For a∈A, state invariance and the quotient inner product give ∥Ug[a]−[a]∥2=2ω(a∗a)−ω(a∗αg(a))−ω((αg(a))∗a). The first cross term tends to ω(a∗a) as g→e by [A2]. For the second, invariance gives ω((αg(a))∗a)=ω(αg−1((αg(a))∗a))=ω(a∗αg−1(a)), which also tends to ω(a∗a) by [A2] and continuity of inversion. Thus Ug[a]→[a] for every [a]∈Dω.

3.1step 1.1step 2.2givenalgebra∎

Let ξ∈Hω and ε>0. Choose y∈Dω with ∥ξ−y∥<ε/3. Since each Ug is unitary, ∥Ugξ−ξ∥≤2∥ξ−y∥+∥Ugy−y∥; step 2.2 makes the last term less than ε/3 for g sufficiently near e. Hence every orbit is continuous at e. For any g0∈G, ∥Ugξ−Ug0ξ∥=∥Ug0−1gξ−ξ∥, so continuity of multiplication transfers continuity to g0. The unitary representation is strongly continuous on all of G.

Depends on

Dependency tree · 2 levels

Sources