Definition
Spectral projection of a self-adjoint or normal operator
The projection assigned to a Borel subset of the spectrum by an operator's projection-valued spectral measure.
Definition
Let be a self-adjoint or normal operator with spectral measure , and let be a Borel subset of in the self-adjoint case or in the normal case. The spectral projection of for is
where is defined by the Borel functional calculus. It is an orthogonal projection. Its range is the spectral subspace on which has spectrum concentrated in the closure of , and it reduces , including the domain when is unbounded.
Projection-valued measure laws
The assignment is a projection-valued measure:
For pairwise disjoint , the projections are orthogonal and , where the sum converges strongly. These laws encode countable additivity at the operator level.
Eigenvalues, intervals, and reconstruction
For , the atomic projection has range ; it is nonzero exactly when is an eigenvalue. If is self-adjoint, the family
is an increasing right-continuous resolution of the identity. The operator is reconstructed as
with its domain determined by square integrability of the coordinate function.
Operator-algebraic role
Every spectral projection belongs to the von Neumann algebra generated by 's bounded resolvents, while it need not lie in the norm-closed -algebra generated by a bounded . This distinction explains why von Neumann algebras support measurable Borel operations. In quantum mechanics, spectral projections of a self-adjoint observable represent sharp yes-or-no events.
References
- 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.
- Masamichi Takesaki, Theory of Operator Algebras I, Springer, 1979. DOI record. Relevant: Chapter III on spectral projections in von Neumann algebras.