“…We show that this strategy does not depend on what Hamiltonian is used to read the qubit. However, we make the assumption that the state of the system (qubit + cavity) is at all times in a state ρ = a |g, α g (t) g, α g (t)| + b |e, α e (t) e, α e (t)| + c |e, α e (t) g, α g (t)| + d |g, α g (t) e, α e (t)| (20) From this we usually perform a polaron transform [5,12]. Here, we first displace the cavity to the barycenter of the two coherent states (α g + α e )/2.…”