Definition

Let {Hx}xX\{H_x\}_{x\in X} be a over (X,μ)(X,\mu), and let AxA_x be a measurable family of closed on the fibers. The direct integral

A=XAxdμ(x)A=\int_X^\oplus A_x\,d\mu(x)

has domain consisting of measurable sections ξ\xi such that ξ(x)Dom(Ax)\xi(x)\in\operatorname{Dom}(A_x) and xAxξ(x)x\mapsto A_x\xi(x) is square-integrable; it acts by (Aξ)(x)=Axξ(x)(A\xi)(x)=A_x\xi(x). Here measurability of the family can be expressed by measurability of the graph projections. Operators and families that agree almost everywhere define the same direct integral.

Bounded and unbounded cases

If the AxA_x are bounded and ess supxAx<\operatorname*{ess\,sup}_x\lVert A_x\rVert<\infty, then AA is the bounded determined by the field. Without a uniform essential bound, the same formula usually defines an unbounded operator with the stated maximal natural domain. The graph of AA is the direct integral of the fiber graphs, so closedness passes from the fibers to AA.

Fiberwise spectral properties

Adjoints and standard operator properties are computed fiberwise under the measurability hypotheses:

A=XAxdμ(x).A^*=\int_X^\oplus A_x^*\,d\mu(x).

In particular, AA is self-adjoint when AxA_x is self-adjoint almost everywhere. Fiberwise functional calculus then gives

f(A)=Xf(Ax)dμ(x)f(A)=\int_X^\oplus f(A_x)\,d\mu(x)

for bounded Borel ff. These results are part of the direct-integral operator theory in Takesaki, Chapter IV, §8.

Examples and scope

For one-dimensional fibers Hx=CH_x=\mathbb C, the direct integral of scalar operators Axz=a(x)zA_x z=a(x)z is the multiplication operator by the measurable function aa on L2(X,μ)L^2(X,\mu), possibly unbounded. A bare family of closed operators need not be measurable and therefore need not define a direct integral.

References
  1. Masamichi Takesaki, Theory of Operator Algebras I, Springer, 1979. DOI record. Relevant: Chapter IV, §8, direct integrals and decomposable operators.
  2. Jacques Dixmier, Von Neumann Algebras, North-Holland, 1981. Publisher record. Relevant: Chapter II, measurable fields and direct integrals of operators.