Let π\pi be a of a finite-dimensional GG on HH, and let k≥0k\geq0 be an integer. A vector v∈Hv\in H is a CkC^k vector if its

g⟼π(g)vg\longmapsto\pi(g)v

is CkC^k: in local coordinates its through order kk exist and are continuous. Write HkH^k for this subspace. A C1C^1 vector is also called a differentiable vector.

All orders versus one order

Strong continuity gives H0=HH^0=H, and

H⊇H1⊇H2⊇⋯ ,H∞=⋂k≥0Hk.H\supseteq H^1\supseteq H^2\supseteq\cdots, \qquad H^\infty=\bigcap_{k\geq0}H^k.

The last space consists of . Differentiability once must not be used as a synonym for smoothness at all orders.

Generator interpretation

For a finite-dimensional Lie group, membership in HkH^k is equivalent to existence of every ordered composition of at most kk infinitesimal generators on the vector. The makes these domain requirements precise. For the , Hk={f∈L2(R):xkf∈L2(R)}H^k=\{f\in L^2(\mathbb R):x^k f\in L^2(\mathbb R)\}.

References
  1. Karl-Hermann Neeb, On Differentiable Vectors for Representations of Infinite Dimensional Lie Groups. Definition 3.1(b) and Theorem 9.4.