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Full and reduced group C star algebras of a finite group

Example

Assume the Axiom of Choice. Let G be a finite group, regarded as a compact Hausdorff group, with normalized Haar probability (The unitary dual of a compact group). Then the full and reduced group C*-algebras coincide, C∗(G)=Cr∗(G)≅⨁π∈G^End⁡(Hπ)≅⨁π∈G^Mdπ(C),dπ=dim⁡CHπ, a finite-dimensional semisimple C*-algebra (The full (maximal) group C star algebra, The reduced group C star algebra, End⁡F(V) is a ring and matrix representation is a ring isomorphism End⁡F(V)≅Mn(F)).

Facts & Assumptions

Given: AC; a finite group G; its unitary dual G^; the left regular representation λ on L2(G); the dense embedding L1(G)→C∗(G).

[F1]

A finite group is compact Hausdorff, and every strongly continuous unitary representation ρ of G is a discrete Hilbert direct sum ρ≅⨁^iσi of finite-dimensional irreducibles σi∈G^; the dual G^ is finite (Unitary representations of compact groups are discrete Hilbert sums of irreducibles, The unitary dual of a compact group).

[F2]

The normalized irreducible matrix coefficient family B=(uijπ)π∈G^, 1≤i,j≤dπ is an orthonormal basis of L2(G), and the left regular representation satisfies λ≅⨁^π∈G^dπ π (The normalized matrix coefficients form an orthonormal basis of L2(K), Peter-Weyl decomposition of the regular representation, The normalized irreducible matrix coefficient family, Left and right regular unitary representations of an LCH group).

[F3]

For a unitary representation π the integrated form f↦π(f)=∫Gf(g)π(g) dg is a ∗-homomorphism of L1(G), and unitary representations correspond to nondegenerate star-representations through this construction (Unitary representations correspond to nondegenerate star representations of L one, Nondegenerate representations of the full group C star algebra are unitary representations).

[F4]

C∗(G) is the completion of L1(G) in the norm ∥f∥C∗=sup⁡ρ∥ρ(f)∥, and Cr∗(G) is the norm closure of {λ(f):f∈L1(G)} in B(L2(G)); the integrated form of λ extends to a surjective star-homomorphism C∗(G)↠Cr∗(G) which is the identity on L1(G) (The full (maximal) group C star algebra, The reduced group C star algebra, The canonical map from the full to the reduced group C star algebra).

[F5]

End⁡(H)≅Md(C) as rings after a basis is chosen (End⁡F(V) is a ring and matrix representation is a ring isomorphism End⁡F(V)≅Mn(F)). Choosing an orthonormal basis for the finite-dimensional Hilbert space makes the matrix of the Hilbert adjoint the conjugate transpose: its entries satisfy ⟨T∗ej,ei⟩=⟨Tei,ej⟩‾. Thus this identification is a ∗-isomorphism locally, rather than an extra assertion of the ring supplier.

[F6]

A unital ring is semisimple when its left regular module is a direct sum of simple submodules (A semisimple ring as a ring whose left regular module is semisimple, Semisimple modules as direct sums of simple modules).

Verification

technique · direct

Given: AC, a finite group G, its unitary dual G^, the regular representation λ and L1(G)⊆C∗(G).

1.1F2F3

The evaluation map Φ:L1(G)→⨁π∈G^End⁡(Hπ), f↦(π(f))π∈G^, is injective and ∗-multiplicative. It is ∗-multiplicative by [F3]; for injectivity suppose π(f)=0 for every π∈G^. Then every matrix element ⟨π(f)ej,ei⟩ vanishes, and these are (1/dπ)∫Gf(g)ujiπ(g) dμ(g), the inner products of f with ujiπ‾ up to nonzero constants. Conjugation sends the complete orthonormal family of [F2] to another complete orthonormal family: it preserves norms and turns each inner product into its conjugate. Hence vanishing of all these inner products forces f=0.

2.1F2step 1.1

Φ is bijective. It is injective by step 1.1, dim⁡L1(G)=∣G∣ for the finite group, and the orthonormal basis of [F2] is indexed by the triples (π,i,j), so ∑π∈G^dπ2=∣G∣=dim⁡L2(G) [F2]; hence the two finite-dimensional spaces have equal dimension and Φ is a linear isomorphism. Consequently Φ is a ∗-isomorphism of L1(G) onto the finite-dimensional C*-algebra ⨁π∈G^End⁡(Hπ), and it is isometric for the transported norm ∥f∥Φ:=∥Φ(f)∥=max⁡π∈G^∥π(f)∥.

3.1F1F2F4step 2.1

The full and reduced norms coincide on L1(G). By [F4] ∥f∥C∗=sup⁡ρ∥ρ(f)∥ over all unitary representations ρ; by [F1] each ρ is a discrete direct sum ⨁^iσi of irreducibles, so ∥ρ(f)∥=sup⁡i∥σi(f)∥ and therefore sup⁡ρ∥ρ(f)∥=max⁡π∈G^∥π(f)∥=∥f∥Φ. By [F2] λ≅⨁^πdππ, so also ∥λ(f)∥=max⁡π∥π(f)∥=∥f∥Φ; as Cr∗(G) is the completion of λ(L1(G)), its norm on L1(G) is ∥f∥Φ as well.

4.1F4F5F6step 3.1

The canonical surjection C∗(G)↠Cr∗(G) of [F4] is isometric on the dense image of L1(G) by step 3.1, hence is injective on a dense subspace and therefore an isometric isomorphism of C*-algebras; both algebras are the completion of L1(G) in the common norm ∥⋅∥Φ. That completion is L1(G) itself, because step 2.1 exhibits it as isometric to the finite-dimensional, hence complete, algebra ⨁πEnd⁡(Hπ). Therefore C∗(G)=Cr∗(G)≅⨁π∈G^End⁡(Hπ)≅⨁π∈G^Mdπ(C) by [F5], a finite-dimensional algebra with one matrix block per irreducible class. It is semisimple by [F6]: the regular module of Md(C) is the direct sum of its column left ideals, each simple because matrix units send any nonzero column vector to every coordinate vector. The central block projections give the corresponding direct sum for the finite product of matrix algebras.

5.1given∎

The Axiom of Choice is inherited from the Peter-Weyl decomposition, the representation correspondence and the group C*-algebra constructions; the dimension count and the norm comparison add no further choice (The Axiom of Choice).

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