Strongly continuous
semi-groups {Qt} of quasinormal operators on Hilbert space are characterized as
follows: there exist Hilbert spaces ℒ and 𝒦, a strongly continuous normal semi-group
{Nt} on ℒ and a strongly continuous self-adjoint semi-group {h(t)} on 𝒦 such that
{Qt} is unitarily equivalent to {Nt}⊕{h(t)Lt} on ℒ⊕ℒ2(𝒦), where {Lt} is the
forward translation semi-group on ℒ2(𝒦) and (h(t)f)(x) = h(t)f(x) a.e. for each f in
ℒ2(𝒦).