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    • CommentRowNumber1.
    • CommentAuthorDmitri Pavlov
    • CommentTimeOct 19th 2024

    Created:

    Idea

    Maharam’s theorem states a complete classification of isomorphism classes of the appropriate category of measurable spaces.

    In the σ-finite case, the theorem classifies measure spaces up to an isomorphism. Here an isomorphism is an equivalence class of measurable bijections ff with measurable inverse such that ff and f 1f^{-1} preserve measure 0 sets.

    As explained in the article categories of measure theory, for a truly general, unrestricted statement for non-σ-finite spaces there are additional subtleties to consider: equality almost everywhere must be refined to weak equality almost everywhere, and σ-finiteness should be relaxed to a combination of Marczewski-compactness and strict localizibility.

    In this unrestricted form, by the Gelfand-type duality for commutative von Neumann algebras, Maharam’s theorem also classifies isomorphism classes of localizable Boolean algebras, abelian von Neumann algebras, and hyperstonean spaces (or hyperstonean locales).

    Statement

    Every object in one of the above equivalent categories canonically decomposes as a coproduct (disjoint union) of ergodic objects. Here an object XX is ergodic if the only subobjects of XX invariant under all automorphisms of XX are \emptyset and XX itself.

    Furthermore, an ergodic object XX is (noncanically, using the axiom of choice) isomorphic to 𝔠×2 κ\mathfrak{c}\times 2^\kappa, where κ\kappa is 0 or infinite, and 𝔠\mathfrak{c} is infinite if κ\kappa is infinite. Here the cardinal 𝔠\mathfrak{c} is known as the cellularity of XX and κ\kappa is its Maharam type.

    In particular, if κ=0\kappa=0, we get a classification of isomorphism classes of atomic measure spaces: they are classified by the cardinality 𝔠\mathfrak{c} of their set of atoms.

    Otherwise, κ\kappa is infinite, and we get a classification of isomorphism classes of ergodic atomless (or diffuse) measure spaces: such spaces are isomorphic to 𝔠×2 κ\mathfrak{c}\times 2^\kappa, where 𝔠\mathfrak{c} and κ\kappa are infinite cardinals.

    Thus, a completely general object XX has the form

    κ𝔠 κ×2 κ,\coprod_\kappa \mathfrak{c}_\kappa\times 2^\kappa,

    where κ\kappa runs over 0 and all infinite cardinals, 𝔠 κ\mathfrak{c}_\kappa is a cardinal that is infinite or 0 if κ0\kappa\ne0, and 𝔠 κ0\mathfrak{c}_\kappa\ne0 only for a set of κ\kappa.

    References

    The original reference is

    • Dorothy Maharam, On homogeneous measure a lgebras, Proc. Nat. Acad. Sci. U.S.A. 28 (1942) 108-111. doi.

    A modern exposition can be found in Chapter 33 (Volume 3, Part I) of

    v1, current

    • CommentRowNumber2.
    • CommentAuthorDmitri Pavlov
    • CommentTimeOct 19th 2024

    Added a relative version:

    Relative version

    There is also a relative version of Maharam’s theorem, which classifies morphisms in any of the equivalent categories considered above.

    Observe that morphisms 2 κ2 λ2^\kappa\to2^\lambda exist if and only if κλ\kappa\ge\lambda. For example, there are no morphisms from the terminal space 2 02^0 (i.e., a singleton) to the real line R2 0\mathbf{R}\cong 2^{\aleph_0}, since the image of such a point is a measure 0 subset, whose preimage therefore cannot have measure 0. In the language of commutative von Neumann algebras, this translates to saying that there are no normal *-homomorphisms L (R)CL^\infty(\mathbf{R})\to\mathbf{C}.

    Observe also that we have a natural notion of locality for a measure space: a covering family is given by a family of measurable subsets whose essential supremum equals the entire space. (This is more than just an analogy to open covers in topological spaces: when translated to the language of locales, the two notions become identical.)

    With these two observations in mind, we can succinctly formulate the relative Maharam theorem as follows: every morphism f:XYf\colon X\to Y locally in XX and YY is isomorphic to a morphism of the form 2 κ2 λ2^\kappa\to2^\lambda, where κλ\kappa\ge\lambda and the map is given by projecting to the first λ\lambda coordinates.

    diff, v2, current