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Kernel inclusion implies weak containment

Statement

Assume the Axiom of Choice. Let G be an LCH group and let π and ρ be strongly continuous unitary representations whose extended representations of C∗(G) (Nondegenerate representations of the full group C star algebra are unitary representations, The full (maximal) group C star algebra) satisfy ker⁡ρ⊆ker⁡π. Then π≺ρ (Weak containment of unitary representations).

Facts & Assumptions

Given: AC; an LCH group G; unitary representations π,ρ with ker⁡ρ⊆ker⁡π; unit vectors ξ∈Hπ.

[F1]

φ(a):=⟨π(a)ξ,ξ⟩ is a state of C∗(G) for every unit vector ξ (States and positive functionals on a C star algebra); it vanishes on ker⁡ρ⊆ker⁡π and therefore factors as φ=φ~∘ρ with φ~ a state of the C*-algebra B:=ρ(C∗(G))⊆B(Kρ), because C∗(G)/ker⁡ρ≅B isometrically (Quotients of C star algebras by closed two-sided ideals).

[F2]

Every state of B is a weak-* limit of a net of convex combinations of normalized vector states: for suitable nets θi=∑jλi,jωηi,j, with ∥ηi,j∥=1, λi,j≥0, ∑jλi,j=1, one has θi(b)→φ~(b) for every b∈B (States of a concretely represented C star algebra are weak star limits of finite sums of vector states).

[F3]

Translation estimates: for a normalized coefficient ψ(x)=⟨σ(x)η,η⟩, ∥η∥=1, one has ∣ψ(xh)−ψ(x)∣≤(2(1−Re⁡ψ(h)))1/2 (Translation estimates for continuous positive type functions, Continuous positive-type functions and normalization).

[F4]

For f∈Cc(G) the integrated forms give ⟨π(Lgf)ξ,ξ⟩=∫Gf(h)⟨π(gh)ξ,ξ⟩ dh and likewise for ρ and for vector functionals; the maps g↦Lgf are continuous in L1(G) with ∥Lgf∥C∗≤∥Lgf∥1=∥f∥1 (The integrated form of a unitary representation, Strong continuity of left and modular right translations on L1 and L2, Integrated forms are contractive nondegenerate star representations of L one, The full (maximal) group C star algebra).

Proof

technique · direct

Given: AC, an LCH group G, unitary representations π,ρ with ker⁡ρ⊆ker⁡π, a unit vector ξ∈Hπ, a compact set Q⊆G and ϵ>0.

1.1F3F4

Let k(g):=⟨π(g)ξ,ξ⟩ and, for a convex combination θ=∑jλjωηj of normalized vector states of B with associated coefficient kθ(g):=∑jλj⟨ρ(g)ηj,ηj⟩, and for f∈Cc(G) with ∫Gf=1 and f≥0, one has ∣k(g)−⟨π(f)ξ,ξ⟩g∣≤(2(1−Re⁡φ(f)))1/2 and ∣kθ(g)−θ(Lgf)∣≤(2(1−Re⁡θ(f)))1/2 for every g, where ⟨π(f)ξ,ξ⟩g:=∫Gf(h)k(gh) dh and θ(Lgf)=∫Gf(h)kθ(gh) dh by [F4]. Indeed, ∣k(g)−k(gh)∣≤(2(1−Re⁡k(h)))1/2 by [F3], and Cauchy–Schwarz for the probability measure f dh gives ∫Gf(h)(2(1−Re⁡k(h)))1/2dh≤(2(1−∫Gf(h)Re⁡k(h) dh))1/2=(2(1−Re⁡φ(f)))1/2; the same computation applies to kθ, whose summands satisfy the same estimate by [F3] and Cauchy–Schwarz for the weights λj.

1.2F1F2F4

Fix f∈Cc(G). The set {Lgf:g∈Q} is compact in L1(G) by [F4], hence its image under the continuous map into C∗(G) is compact; since θi(ρ(b))→φ~(ρ(b)) for every b∈C∗(G) by [F1] and [F2], a finite δ-net argument gives sup⁡g∈Q∣θi(Lgf)−φ(Lgf)∣→0, where φ(Lgf)=φ~(ρ(Lgf)).

2.1F1step 1.1step 1.2

Consequently k is a compact-uniform limit of the coefficients kθ: enlarging the given compact set Q to Q∪{e} if necessary, and given ϵ>0, choose f∈Cc(G) with f≥0, ∫f=1 and support so small that 1−Re⁡k(h)<ϵ on it, so that 1−Re⁡φ(f)<ϵ; eventually 1−Re⁡θi(f)<2ϵ by step 1.2 applied at e, and then sup⁡Q∣k−kθi∣≤(2ϵ)1/2+sup⁡Q∣θi(Lgf)−φ(Lgf)∣+(4ϵ)1/2, which is <4ϵ once i is large: the first and third terms sum to (2+2)ϵ<4ϵ, and the middle term tends to zero, by steps 1.1 and 1.2.

3.1step 2.1

Therefore every normalized diagonal coefficient of π is a compact-uniform limit of finite sums of diagonal coefficients of ρ; for an arbitrary vector ξ≠0 the coefficient cξ,ξ=∥ξ∥2cξ/∥ξ∥,ξ/∥ξ∥ is a nonnegative multiple of a normalized one and the approximating sums scale by the same factor, so by [F1]–[F2] and the definition of weak containment π≺ρ.

4.1givenF2∎

The Axiom of Choice is used for the geometric separation behind the vector-state approximation of step 2.1 and is inherited from the whole chain (The Axiom of Choice).

Depends on

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