A propagator method referred to as third-order algebraic-diagrammatic const
ruction [ADC(3)] for the direct computation of electronic excitation energi
es and transition moments is presented. This approach is based on a specifi
c reformulation of the diagrammatic perturbation expansion for the polariza
tion propagator, and extends the existing second-order [ADC(2)] scheme to t
he next level of perturbation theory. The computational scheme combines dia
gonalization of a Hermitian secular matrix and perturbation theory for the
matrix elements. The characteristic properties of the method are compact co
nfiguration spaces, regular perturbation expansions, and size-consistent re
sults. The configuration space is spanned by singly and doubly excited stat
es, while the perturbation expansions in the secular matrix extend through
third order in the p-h block, second order in the p-h/2p-2h coupling block,
and first order in the 2p-2h block. While the simpler ADC(2) method, repre
senting a counterpart to the MP2 (second-order Moller-Plesset) ground-state
method, recommends itself for application to larger molecules, the ADC(3)
scheme is aimed at a more accurate description of molecular excitation spec
tra. The relationship of the ADC(3) scheme with coupled cluster methods is
discussed, focusing here in particular on the treatment of transition momen
ts. (C) 1999 American Institute of Physics. [S0021-9606(99)30345-7].