Theorem
Stone's theorem for one-parameter unitary groups
Strongly continuous one-parameter unitary groups are exactly exponentials of self-adjoint operators.
Statement
Let be a strongly continuous unitary representation of the additive group, equivalently a strongly continuous unitary one-parameter group. Stone's theorem states that there is a unique, possibly unbounded, self-adjoint operator on such that
Conversely, every self-adjoint defines such a group through the spectral functional calculus. Its domain is
and the displayed limit equals .
Generator and domain
The strong derivative at is therefore not defined on every vector unless is bounded. On its dense domain it gives the closed skew-adjoint operator . The group determines both the operator and its domain: specifying only a formal derivative or an eigenvalue formula does not specify an unbounded generator.
Consequences
Strong continuity, the group law, and unitarity force differentiability precisely on , even though no differentiability is assumed initially. The spectral theorem then yields
In a unitary representation of a Lie group, applying Stone's theorem to produces the self-adjoint generator associated with each Lie-algebra element Reed–Simon, Theorem VIII.8.
Sign conventions
Some authors write . Their self-adjoint generator is , and the strong derivative is . Other authors call the skew-adjoint operator , rather than , the infinitesimal generator. The exponential formula and derivative-domain identity must be stated together to remove this ambiguity.
References
- M. H. Stone, “On One-Parameter Unitary Groups in Hilbert Space,” Annals of Mathematics 33 (1932), 643–648. DOI record. Relevant: the original correspondence theorem.
- M. Reed and B. Simon, Methods of Modern Mathematical Physics I: Functional Analysis, Academic Press, 1972. DOI record. Relevant: Theorem VIII.8.