The time-independent perturbation theory in quantum mechanics is formulated
using projection operator techniques. The determination of the perturbed e
igenvalue can be decoupled from that of the perturbed eigenstate. Both the
Brillouin-Wigner theory and the Rayleigh-Schrodinger theory come out straig
htforwardly. Both degenerate and nondegenerate cases can be treated in a un
ified way for arbitrarily high order perturbations. (C) 2000 American Assoc
iation of Physics Teachers.