Dirac's perturbation solution of the time‐dependent Schrödinger equation ih\documentclass{article}\pagestyle{empty}\begin{document}$ ih\frac{d}{{dt}}\left| {\Phi \left. {\left( t \right)} \right\rangle = H} \right|\Phi \left. {\left( t \right)} \right\rangle $\end{document}, \documentclass{article}\pagestyle{empty}\begin{document}$ H = H_0 + \Psi $\end{document}is formulated by means of a well‐defined operator PD with the properties
where ϕn(t)〉 is the n‐th order correction of ϕ(t)〉. This operator PD can be used to solve the equation of motion of the evolution operator, of the statistical operator, and of quantum mechanical conserved quantities in a corresponding way. A simple proof of the quantum mechanical adiabatic theorem shows this formulation of perturbation corrections to be useful.