Definition

Let (X,Σ)(X,\Sigma) be a and HH a . Write P(H)\mathcal P(H) for the set of on HH. A projection-valued measure on (X,Σ)(X,\Sigma) is a map

E:ΣP(H)E:\Sigma\longrightarrow\mathcal P(H)

such that E(X)=IE(X)=I, E(AB)=E(A)E(B)E(A\cap B)=E(A)E(B), and, for every pairwise disjoint sequence (An)(A_n) and every ξH\xi\in H,

E(n=1An)ξ=n=1E(An)ξE\left(\bigcup_{n=1}^{\infty}A_n\right)\xi =\sum_{n=1}^{\infty}E(A_n)\xi

with convergence in HH. Thus EE is countably additive in the . For ξ,ηH\xi,\eta\in H, the scalar function AE(A)ξ,ηA\mapsto\langle E(A)\xi,\eta\rangle is a countably additive complex .

Spectral integration

For a bounded ff, one first sets

Xjcj1AjdE=jcjE(Aj)\int_X\sum_j c_j1_{A_j}\,dE=\sum_j c_jE(A_j)

and then extends uniformly to define XfdE\int_X f\,dE. This construction preserves products, adjoints, and constants, so it is a unital *-homomorphism from bounded measurable functions into bounded operators. recover the projections: X1AdE=E(A)\int_X1_A\,dE=E(A).

Relation to spectral theorems

Every bounded TT has a unique projection-valued measure on its spectrum for which

T=σ(T)zdE(z).T=\int_{\sigma(T)}z\,dE(z).

Conversely, spectral integration of the coordinate function produces a normal operator. For an unbounded self-adjoint operator, define μξ(A)=E(A)ξ,ξ\mu_\xi(A)=\langle E(A)\xi,\xi\rangle; the is interpreted on the domain of vectors ξ\xi satisfying Rλ2dμξ(λ)<\int_{\mathbb R}\lambda^2\,d\mu_\xi(\lambda)<\infty. These forms of the spectral theorem are developed in Conway, Chapters IX and X.

Examples and conventions

If H=nHnH=\bigoplus_nH_n is an orthogonal decomposition and X=NX=\mathbb N, then E(A)E(A) projects onto nAHn\bigoplus_{n\in A}H_n. This is the discrete model for spectral decomposition.

References
  1. J. B. Conway, A Course in Functional Analysis, 2nd ed., Springer, 1990. Springer DOI record. Relevant: chapters on normal operators, spectral measures, and unbounded operators.