So, can I say that, in the Schrodinger picture, every operator is time independent, except (maybe) the hamiltonian? In this case, if I try to compute the expection value of the hamiltonian ##\hat{H}(t)## in the state ##| \psi (t) \rangle##, I get $$\langle \psi (t) | \hat{H}(t) | \psi(t) \rangle...