Definition

Let MB(H)M\subseteq B(H) be a . A closed densely defined is measurable with respect to MM if its domain is strongly dense: there are projections pnMp_n\in M such that pn1p_n\uparrow1 strongly, pnHdom(T)p_nH\subseteq\operatorname{dom}(T), and each complementary projection 1pn1-p_n is in MM. This condition uses Murray–von Neumann finiteness, not a numerical trace. It permits unbounded operators while ensuring that TT is bounded on successively larger corners whose omitted parts are finite.

Spectral characterization

Write ETE^{|T|} for the spectral measure of the positive operator T|T|. Measurability is equivalent to the existence of s0s\geq0 for which the spectral tail ET((s,))E^{|T|}((s,\infty)) is a finite projection. Once one such tail is finite, every higher tail is finite and the projections ET([0,n])E^{|T|}([0,n]) supply a strongly dense domain. This formulation makes the definition independent of a chosen approximating sequence Nelson, pp. 103–106.

Algebra and examples

The measurable operators form a unital S(M)S(M) when sums, products, and adjoints are taken with their natural closed extensions. This is the noncommutative analogue of the algebra of almost-everywhere finite Segal, pp. 401–457.

If MM is finite, every closed densely defined affiliated operator is measurable. At the other extreme, for M=B(H)M=B(H) on an infinite-dimensional , finite projections have finite-dimensional range and S(M)=B(H)S(M)=B(H); the definition admits no genuinely unbounded operators there Nelson, pp. 103–106.

Conventions and scope
References
  1. Irving E. Segal, “A Non-Commutative Extension of Abstract Integration,” Annals of Mathematics 57 (1953), 401–457. DOI record. Relevant: the strongly dense domain and measurable-operator algebra.
  2. Edward Nelson, “Notes on Non-Commutative Integration,” Journal of Functional Analysis 15 (1974), 103–116. DOI record. Relevant: pp. 103–106 on affiliated measurable operators and the measure topology.