Construction
Direct integral of Hilbert spaces
The Hilbert space of square-integrable measurable sections of a measurable field of Hilbert spaces.
Core idea
Let be a measure space and a measurable field of Hilbert spaces. Its direct integral is
the space of measurable sections , modulo equality almost everywhere, for which the Lebesgue integral is finite. Addition and scalar multiplication are fiberwise, and
After quotienting by null sections, this is a Hilbert space. The construction is the measure-theoretic analogue of a Hilbert direct sum.
Constant fields and direct sums
For a constant field , the direct integral is the vector-valued space . If has counting measure, it reduces to the Hilbert direct sum . Atomic and continuous parts of the measure therefore interpolate between discrete sums and continuously indexed decompositions.
Decomposable operators
Suppose is a measurable field of bounded operators with essentially bounded norms. Then
defines a bounded operator between the corresponding direct integrals. Such decomposable operators preserve the fiberwise structure and are basic tools in spectral and representation-theoretic decompositions.
Conventions and use
The phrase “measurable field” includes the chosen measurable structure on sections; a bare family of Hilbert spaces is not enough. Changing fibers or sections on a null set does not change the direct integral. Standard decomposition theorems usually impose -finiteness and separability hypotheses, which must be stated separately from the construction Takesaki, Chapter IV, §8.
References
- Masamichi Takesaki, Theory of Operator Algebras I, Springer, 1979. DOI record. Relevant: Chapter IV, §8 on direct integrals.
- Jacques Dixmier, Von Neumann Algebras, North-Holland, 1981. Publisher record. Relevant: Chapter II, §1 on measurable fields and direct integrals.