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Direct integrals of unitary representations
Definition
Assume the Axiom of Choice (The Axiom of Choice). Let be a locally compact Hausdorff group, let be a sigma-finite standard-Borel measure space (Standard Borel spaces, Finite, sigma-finite, and semifinite measures), and let be a measurable complex Hilbert field with a countable fundamental family (Measurable Hilbert field from a countable fundamental family). Write 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 over this field is a family such that each is strongly continuous (Strongly continuous unitary representations, invariant linear subspaces and intertwiners) and, for each fixed , the operator field is weakly measurable (Measurable and decomposable operator fields). The identities and are required for every and all . For each define By Measurable essentially bounded operator fields act decomposably, these operators define a group homomorphism . This operator family is called the direct integral of the field and written . The homomorphism and unitarity are proved below; strong continuity is not asserted by this definition. Changing the field on a -null set does not change any induced operator .
Facts & Assumptions
Given: AC; a locally compact Hausdorff group ; a sigma-finite standard-Borel measure space ; a measurable complex Hilbert field with countable fundamental family; and the representation field from the Definition.
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).
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).
Under AC, the direct integral of the given measurable Hilbert field is a Hilbert space (Direct integrals of measurable Hilbert fields are Hilbert spaces).
Each fibre map is a group homomorphism into its unitary group, so it preserves products and inverses and satisfies (Strongly continuous unitary representations, invariant linear subspaces and intertwiners).
Direct-integral vectors are measurable square-integrable sections modulo equality off measurable -null sets (Direct integral of a measurable Hilbert field).
Operator fields equal off a measurable -null set are identified (Measurable and decomposable operator fields).
Proof
Fix and set . Its fundamental matrix coefficients are measurable by the fixed- hypothesis, so is weakly measurable by [F1]. On a nonzero fibre , and on a zero fibre ; hence for every . Thus is essentially bounded, and [F2] gives a bounded decomposable operator on the Hilbert space of [F3].
For , [F2] and the pointwise identities [F4] give , , and . Therefore , so every is unitary and is a group homomorphism into . These identities use the stipulated pointwise group laws for every , so no group-element-dependent conull sets are intersected. Strong continuity is not established by this definition.
If the field is changed only on a measurable -null set, then for each fixed 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 is unchanged.
Remarks
The measurable field is required to be weakly measurable in each fixed group coordinate; no joint measurability in 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.
Depends on
- Measurable and decomposable operator fields
- Measurable Hilbert field from a countable fundamental family
- Direct integral of a measurable Hilbert field
- Direct integrals of measurable Hilbert fields are Hilbert spaces
- Measurable essentially bounded operator fields act decomposably
- Strongly continuous unitary representations, invariant linear subspaces and intertwiners
- Standard Borel spaces
- Finite, sigma-finite, and semifinite measures
- The Axiom of Choice
Used by
- Irreducible multiplicity data is not canonical outside type I Counterexample
- Canonical compact-group decompositions are atomic Hilbert sums Example
- The regular representation of the real line as a multiplicity-one integral of characters Example
- A measurable direct integral of unitary representations is strongly continuous Lemma
- Disintegration of a separable group representation over a commuting diagonal algebra Lemma
- Central decomposition into factor representations Theorem
- Non-type-I groups have non-smooth irreducible disintegration Theorem
- Plancherel support for SL2(R) Theorem
Dependency tree · two levels
73 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Bachir Bekka and Pierre de la Harpe, Unitary Representations of Groups, Duals, and Characters (arXiv:1912.07262v1, 16 December 2019) (standard reference, not scraped)