Definition

Let (X,Σ)(X,\Sigma) be a . A measurable field of Hilbert spaces consists of HxH_x and a MxXHx\mathcal M\subseteq\prod_{x\in X}H_x of sections such that:

  1. xξ(x)x\mapsto\lVert\xi(x)\rVert is measurable for every ξM\xi\in\mathcal M;
  2. a section η\eta lies in M\mathcal M whenever xη(x),ξ(x)x\mapsto\langle\eta(x),\xi(x)\rangle is measurable for every ξM\xi\in\mathcal M; and
  3. some sequence (ξn)(\xi_n) in M\mathcal M has {ξn(x):n1}\{\xi_n(x):n\geq1\} dense in every HxH_x.

The elements of M\mathcal M are the measurable sections.

Fundamental sequences and coordinates

A sequence as in the third axiom is called a fundamental sequence. Measurable fiberwise Gram–Schmidt operations turn one into sections that form an after zero vectors are omitted. Relative to such sections, measurability can be checked through scalar coordinate functions. The countability requirement forces every fiber to be separable and is what makes direct-integral constructions manageable Takesaki, Chapter IV, §8.

Direct integrals

Given a (X,Σ,μ)(X,\Sigma,\mu), one takes measurable sections satisfying

Xξ(x)2dμ(x)<\int_X\lVert\xi(x)\rVert^2\,d\mu(x)<\infty

and identifies sections equal . The resulting Hilbert space, denoted XHxdμ(x)\int_X^\oplus H_x\,d\mu(x), has obtained by integrating the fiber inner products. Measurable fields therefore supply the varying-fiber data behind continuous decompositions of operators and representations.

Examples and conventions

A fixed separable Hilbert space HH gives the constant field Hx=HH_x=H, with measurability tested against a countable orthonormal basis. More generally, measurable subsets can carry fibers of different finite or countably infinite dimensions. Unlike a topological , a measurable field need not have a topology on the disjoint union of its fibers.

References
  1. M. Takesaki, Theory of Operator Algebras I, Springer, 1979. Springer DOI record. Relevant: Chapter IV, §8, and the chapter “Tensor Products of Operator Algebras and Direct Integrals.”