“…Instead of asking about the time dependence of observables, of which there are many, one might ask the opposite question, whether in a complex time evolving system there are observables which remain constant in time, the 'constants of the motion'. These are all the observables C j for which the corresponding operators Ĉj commute with the Hamiltonian Ĥ Making use of the solution of the Heisenberg equations of motion given by eqn (23) the time independence of Ĉj can be proven in one line, because Û being a function of Ĥ, eqn (22), it commutes with the Ĉj as well and it is also unitary Û † Û ¼ 1, thus:…”