Statement

Let AA be a on a complex . Suppose the domain of AA contains a DD such that every vDv\in D is analytic for AA:

vn0D(An)andn=0tvnn!Anv<v\in\bigcap_{n\geq 0}\mathcal D(A^n) \quad\text{and}\quad \sum_{n=0}^{\infty}\frac{t_v^n}{n!}\lVert A^n v\rVert<\infty

for some tv>0t_v>0. Nelson's analytic vector theorem states that AA is . In particular, its closure is the unique self-adjoint operator extending AA from its stated domain.

Lie-algebra form

For a representation of a finite-dimensional real by skew-symmetric operators dπ(Xj)d\pi(X_j) on a common dense invariant domain, form the Δ=jdπ(Xj)2\Delta=-\sum_j d\pi(X_j)^2. Essential self-adjointness of Δ\Delta, obtainable from a dense set of for Δ\Delta, supplies analytic vectors for the Lie-algebra action and integrates it to a unitary representation of the . It also yields the of the infinitesimal generators Nelson, §§8–10.

Why analyticity matters

Symmetry alone does not imply essential self-adjointness: symmetric differential operators on incomplete domains may have several . Analyticity supplies convergent power-series control strong enough to prove uniqueness of the unitary evolution. The theorem is therefore a domain criterion, not merely a regularity statement about vectors already known to lie in a unitary representation.

Conventions and scope
References
  1. Edward Nelson, Analytic vectors, Annals of Mathematics 70 (1959), 572–615. DOI record. Relevant: the analytic-vector criterion and §§8–10 on Lie-algebra exponentiation.
  2. Michael Reed and Barry Simon, Methods of Modern Mathematical Physics II: Fourier Analysis, Self-Adjointness, Academic Press, 1975. Publisher record. Relevant: Theorem X.39 and §X.6.