In multiconfiguration perturbation theory, the generalized Brillouin t
heorem is normally fulfilled, which imposes constraints on the matrix
elements involved in the description of single excitations. This can b
e considered as guaranteeing coherence of the configurations and orbit
als describing the zeroth order wavefunction. In quasi-degenerate pert
urbation theory (QDPT) single excitations are treated independently, w
hich causes a loss of coherence. It is argued that a loss of orbital c
oherence leads to unreasonable QDPT correlation energies.