Definition

Let TT be a self-adjoint or with spectral measure ETE_T, and let BB be a Borel subset of R\mathbb R in the self-adjoint case or C\mathbb C in the normal case. The spectral projection of TT for BB is

ET(B)=1B(T),E_T(B)=1_B(T),

where 1B(T)1_B(T) is defined by the . It is an . Its range is the spectral subspace on which TT has spectrum concentrated in the closure of BB, and it reduces TT, including the domain when TT is unbounded.

Projection-valued measure laws

The assignment BET(B)B\mapsto E_T(B) is a :

ET()=0,ET(σ(T))=I,ET(BC)=ET(B)ET(C).E_T(\varnothing)=0,\qquad E_T(\sigma(T))=I,\qquad E_T(B\cap C)=E_T(B)E_T(C).

For pairwise disjoint BnB_n, the projections ET(Bn)E_T(B_n) are orthogonal and ET(nBn)=nET(Bn)E_T(\bigcup_nB_n)=\sum_nE_T(B_n), where the sum converges strongly. These laws encode countable additivity at the operator level.

Eigenvalues, intervals, and reconstruction

For λC\lambda\in\mathbb C, the atomic projection ET({λ})E_T(\{\lambda\}) has range ker(TλI)\ker(T-\lambda I); it is nonzero exactly when λ\lambda is an eigenvalue. If TT is self-adjoint, the family

Eλ=ET((,λ])E_\lambda=E_T((-\infty,\lambda])

is an increasing right-continuous resolution of the identity. The operator is reconstructed as

T=RλdET(λ),T=\int_{\mathbb R}\lambda\,dE_T(\lambda),

with its domain determined by square integrability of the coordinate function.

Operator-algebraic role

Every spectral projection belongs to the generated by TT's bounded resolvents, while it need not lie in the norm-closed CC^*-algebra generated by a bounded TT. This distinction explains why von Neumann algebras support measurable Borel operations. In quantum mechanics, spectral projections of a represent sharp yes-or-no events.

References
  1. Michael Reed and Barry Simon, Methods of Modern Mathematical Physics I: Functional Analysis, revised ed., Academic Press, 1980. DOI record. Relevant: Chapter VII on spectral resolutions and functional calculus.
  2. Masamichi Takesaki, Theory of Operator Algebras I, Springer, 1979. DOI record. Relevant: Chapter III on spectral projections in von Neumann algebras.