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Peter-Weyl for an infinite product of finite groups

Example

Assume the Axiom of Choice (The Axiom of Choice). Let (Gi)i∈I be finite discrete groups with I arbitrary and let K:=∏i∈IGi with the product topology; K is compact, Hausdorff and totally disconnected, hence profinite with normalized Haar probability μ. By Continuous finite-dimensional representations of a product of finite groups factor through a finite subproduct, every continuous finite-dimensional unitary representation of K factors through the projection pF:K→KF=∏i∈FGi for some finite F⊆I; conversely every finite-dimensional representation of the finite group KF pulls back to K, and it is irreducible exactly when the representation of KF is irreducible (pullback along the surjection pF). The finite-coordinate irreducibles of K are therefore exactly the pullbacks of the irreducibles of the finite groups KF; their coefficient spaces are the pullbacks of the coefficient spaces of KF, and the coefficient algebra R(K) is the union of these pullbacks over finite F, i.e. the algebra of continuous functions depending on finitely many coordinates. This algebra is dense in C(K) by Uniform density of representative functions (topological Peter-Weyl theorem) (equivalently by Stone-Weierstrass: it is a unital self-adjoint algebra separating points because coordinates separate points and the finite-group coefficient algebra separates points), the normalized coefficient family is an orthonormal basis of L2(K) (The normalized matrix coefficients form an orthonormal basis of L2(K)), and the regular representation decomposes as in Peter-Weyl decomposition of the regular representation. No countability of I or of the dual is assumed, and point separation in the product uses only finitely many coordinates.

Facts & Assumptions

[A1]

The Axiom of Choice is inherited through the profinite compactness and Haar suppliers and through the representative and basis choices in the general Peter–Weyl coefficient family (The Axiom of Choice). No further choice is needed for the finite-coordinate factorization and pullback arguments.

[F1]

The product K=∏i∈IGi of finite discrete groups is the inverse limit of the finite groups KF over the directed set of finite subsets F⊆I, hence a profinite group: compact, Hausdorff, totally disconnected; it carries a normalized Haar probability μ, and the kernels ker⁡pF form an open normal neighbourhood basis. (A profinite group is a topological group isomorphic to an inverse limit of finite discrete groups, Normalized Haar probability on a compact group, The product set ∏i∈IXi of functions choosing a point in each factor, the projections, the box topology, and the product topology as the initial topology of the projections; the empty product is a one-point space, Continuous finite-dimensional representations of a product of finite groups factor through a finite subproduct)

[F2]

Every continuous finite-dimensional unitary representation ρ of K factors as ρ=ρF∘pF through a finite subproduct, and every matrix coefficient of ρ depends only on the coordinates in F. Conversely a representation ρF of KF pulls back along the surjection pF to a continuous finite-dimensional unitary representation of K with coefficients ρF-coefficients composed with pF. (Continuous finite-dimensional representations of a product of finite groups factor through a finite subproduct, Matrix coefficient of a unitary representation)

[F3]

Pullback along a surjective homomorphism preserves and reflects irreducibility: a closed invariant subspace of the pullback corresponds bijectively to a closed invariant subspace of the representation on the quotient, because the acting groups coincide, ρ(K)=ρF(KF). (Strongly continuous unitary representations, invariant linear subspaces and intertwiners, Continuous finite-dimensional representations of a product of finite groups factor through a finite subproduct)

[F4]

For the finite group KF the coefficient algebra R(KF) equals C(KF): R(KF) is a dense linear subspace of the finite-dimensional space C(KF) by the general density theorem, and a finite-dimensional subspace of a normed space is closed. (Uniform density of representative functions (topological Peter-Weyl theorem), A finite-dimensional normed subspace is closed)

[F5]

The general compact-group theory applies to K: irreducible representations are finite dimensional, R(K) is uniformly dense in C(K), the normalized coefficient family is an orthonormal basis of L2(K), and the regular representation decomposes into the isotypic blocks. (Irreducible unitary representations of compact groups are finite dimensional, Uniform density of representative functions (topological Peter-Weyl theorem), The normalized matrix coefficients form an orthonormal basis of L2(K), Peter-Weyl decomposition of the regular representation, The unitary dual of a compact group, The normalized irreducible matrix coefficient family)

[F6]

The functions K→C depending on finitely many coordinates form a unital self-adjoint complex algebra containing the constants, and they separate points: distinct points differ in some coordinate i, and the function of that coordinate alone taking value 1 at one coordinate and 0 at the other is continuous because Gi is discrete. (Complex Stone–Weierstrass dichotomy for separating self-adjoint algebras; the unital case is dense, The product set ∏i∈IXi of functions choosing a point in each factor, the projections, the box topology, and the product topology as the initial topology of the projections; the empty product is a one-point space, Representative functions on a compact group)

Verification

Given: AC, finite groups Gi indexed by an arbitrary set I, the product K=∏iGi with product topology, and its finite subproducts KF.

1.1F1F2F3F4

By [F1] the product K is a profinite group, hence compact Hausdorff, with normalized Haar probability, and the kernels of the coordinate projections form an open normal neighbourhood basis. By [F2] every continuous finite-dimensional unitary representation of K factors through some pF, and every matrix coefficient then depends on the coordinates in F only; by [F3] such a pullback is irreducible exactly when the representation of the finite group KF is, so the finite-coordinate irreducibles of K are exactly the pullbacks of the irreducibles of the groups KF. Consequently R(K) is the union over finite F of the pullbacks pF∗R(KF): one inclusion is [F2], and conversely a pullback of an element of R(KF) is a finite linear combination of pullbacks of matrix coefficients, hence a representative function of K. Since R(KF)=C(KF) for the finite group KF by [F4], R(K) is exactly the algebra of continuous functions depending on finitely many coordinates.

2.1A1F5F6step 1.1∎

The general theory applies to the compact Hausdorff group K by [F5]: R(K) is uniformly dense in C(K) and the normalized coefficient family is an orthonormal basis of L2(K), while the regular representation decomposes into its isotypic blocks. The density also follows directly from the description of R(K) in step 1.1: it is a unital self-adjoint algebra of continuous functions separating points by [F6], so the unital Stone-Weierstrass theorem gives uniform density; point separation uses only the finitely many coordinates in which two points differ, and no countability of I is needed or claimed. This completes the verification. The Axiom of Choice enters exactly through the suppliers and coefficient-family choices of [A1].

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