The closure of the derivation
λD : Cc1(ℝ) → C0(ℝ) defined by (λD)(f) = λf′, where λ : ℝ → ℝ is continuous,
generates a C0-group on C0(ℝ) (corresponding to a flow on ℝ) if and only if 1∕λ is
not locally integrable on either side of any zero of λ or at ±∞.
If S is a flow on a locally compact, Hausdorff, space X with fixed point set XS0,
δS is the generator of the induced action on C0(X), λ : X ∖XS0 → ℝ is continuous,
and bounded on sets of low frequency under S, and t → λ(Stω)−1 is not locally
integrable on either side of any zero or at ±∞, then the flows along the orbits of S
form a flow on X whose generator acts as λδS.
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