How can I prove:
Tr(AeLtB)=Tr(Be−LtA)
where A and B are observables in the Schrödinger picture and L is the quantum Liouville super-operator defined by:
LA=iℏ[H,A]
so defining the Liouville propagator as: A(t)=eLtA(0)
This post imported from StackExchange Physics at 2015-08-27 17:28 (UTC), posted by SE-user pindakaas