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DefinitionDefinition: AI-adaptedProof: AI-adaptedPipeline-generatedprecheck passjudge pass (gpt-6.1-sol)audited 2026-10-08
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Direct integrals of unitary representations

Definition

Assume the Axiom of Choice (The Axiom of Choice). Let G be a locally compact Hausdorff group, let (X,B,μ) be a sigma-finite standard-Borel measure space (Standard Borel spaces, Finite, sigma-finite, and semifinite measures), and let (Hx,en(x))x∈X be a measurable complex Hilbert field with a countable fundamental family (Measurable Hilbert field from a countable fundamental family). Write H=∫X⊕Hx dμ(x) for its direct-integral Hilbert space (Direct integral of a measurable Hilbert field, Direct integrals of measurable Hilbert fields are Hilbert spaces). A measurable field of unitary representations of G over this field is a family (πx)x∈X such that each πx:G→U(Hx) is strongly continuous (Strongly continuous unitary representations, invariant linear subspaces and intertwiners) and, for each fixed g∈G, the operator field x↦πx(g) is weakly measurable (Measurable and decomposable operator fields). The identities πx(gh)=πx(g)πx(h) and πx(e)=IHx are required for every x∈X and all g,h∈G. For each g∈G define π(g)=∫X⊕πx(g) dμ(x)∈B(H). By Measurable essentially bounded operator fields act decomposably, these operators define a group homomorphism G→U(H). This operator family is called the direct integral of the field and written π=∫X⊕πx dμ(x). The homomorphism and unitarity are proved below; strong continuity is not asserted by this definition. Changing the field on a μ-null set does not change any induced operator π(g).

Facts & Assumptions

Given: AC; a locally compact Hausdorff group G; a sigma-finite standard-Borel measure space (X,B,μ); a measurable complex Hilbert field with countable fundamental family; and the representation field from the Definition.

[F1]

For a weakly measurable operator field, the norm function is measurable, and coefficient measurability is equivalent to measurability against all pairs of measurable sections (Measurable and decomposable operator fields).

[F2]

A weakly measurable essentially bounded operator field induces a bounded decomposable operator, and induced products and adjoints agree with their pointwise field products and adjoints (Measurable essentially bounded operator fields act decomposably).

[F3]

Under AC, the direct integral of the given measurable Hilbert field is a Hilbert space (Direct integrals of measurable Hilbert fields are Hilbert spaces).

[F4]

Each fibre map is a group homomorphism into its unitary group, so it preserves products and inverses and satisfies πx(g)∗=πx(g−1) (Strongly continuous unitary representations, invariant linear subspaces and intertwiners).

[F5]

Direct-integral vectors are measurable square-integrable sections modulo equality off measurable μ-null sets (Direct integral of a measurable Hilbert field).

[F6]

Operator fields equal off a measurable μ-null set are identified (Measurable and decomposable operator fields).

Proof

technique · direct
1.1F1F2F3given

Fix g∈G and set Tx=πx(g). Its fundamental matrix coefficients are measurable by the fixed-g hypothesis, so T is weakly measurable by [F1]. On a nonzero fibre ∥Tx∥=1, and on a zero fibre ∥Tx∥=0; hence ∥Tx∥≤1 for every x. Thus T is essentially bounded, and [F2] gives a bounded decomposable operator Pg=∫X⊕πx(g) dμ(x) on the Hilbert space H of [F3].

2.1F2F3F4step 1.1

For g,h∈G, [F2] and the pointwise identities [F4] give PgPh=∫X⊕πx(g)πx(h) dμ(x)=Pgh, Pe=IH, and Pg∗=∫X⊕πx(g)∗ dμ(x)=Pg−1. Therefore PgPg∗=Pg∗Pg=IH, so every Pg is unitary and g↦Pg is a group homomorphism into U(H). These identities use the stipulated pointwise group laws for every x, so no group-element-dependent conull sets are intersected. Strong continuity is not established by this definition.

3.1F5F6step 1.1∎

If the field is changed only on a measurable μ-null set, then for each fixed g the corresponding operator fields agree off that set by [F6]. Their pointwise actions on every measurable section therefore define the same class in the quotient [F5], so every induced operator Pg is unchanged.

Remarks

The measurable field is required to be weakly measurable in each fixed group coordinate; no joint measurability in (x,g) is asserted. The locally compact Hausdorff scope supports the algebraic homomorphism and unitary operators proved above. Strong continuity is a separate assertion, not a consequence claimed here.

Bekka and de la Harpe state the representation construction for second-countable locally compact groups and refer to a separate strong-continuity result. The proof above uses only their fixed-coordinate operator-field construction and the local decomposable-operator theorem, so its algebraic conclusion holds on the stated locally compact Hausdorff scope.

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Sources