Statement

Let U:RU(H)U:\mathbb R\to U(\mathcal H) be a of the additive group, equivalently a strongly continuous unitary . Stone's theorem states that there is a unique, possibly unbounded, AA on H\mathcal H such that

U(t)=eitA(tR).U(t)=e^{itA}\qquad(t\in\mathbb R).

Conversely, every self-adjoint AA defines such a group through the spectral functional calculus. Its domain is

Dom(A)={ξ:limt0U(t)ξξt exists in norm},\operatorname{Dom}(A)=\left\{\xi:\lim_{t\to0}\frac{U(t)\xi-\xi}{t}\text{ exists in norm}\right\},

and the displayed limit equals iAξiA\xi.

Generator and domain

The strong derivative at 00 is therefore not defined on every vector unless AA is bounded. On its dense domain it gives the closed skew-adjoint operator iAiA. 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 Dom(A)\operatorname{Dom}(A), even though no differentiability is assumed initially. The spectral theorem then yields

U(t)=ReitλdEA(λ).U(t)=\int_{\mathbb R}e^{it\lambda}\,dE_A(\lambda).

In a unitary , applying Stone's theorem to tπ(exp(tX))t\mapsto\pi(\exp(tX)) produces the self-adjoint generator associated with each Lie-algebra element XX Reed–Simon, Theorem VIII.8.

Sign conventions

Some authors write U(t)=eitHU(t)=e^{-itH}. Their self-adjoint generator HH is A-A, and the strong derivative is iH-iH. Other authors call the skew-adjoint operator iAiA, rather than AA, the infinitesimal generator. The exponential formula and derivative-domain identity must be stated together to remove this ambiguity.

References
  1. 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.
  2. M. Reed and B. Simon, Methods of Modern Mathematical Physics I: Functional Analysis, Academic Press, 1972. DOI record. Relevant: Theorem VIII.8.