Jf. Stanton et J. Gauss, PERTURBATIVE TREATMENT OF THE SIMILARITY TRANSFORMED HAMILTONIAN IN EQUATION-OF-MOTION COUPLED-CLUSTER APPROXIMATIONS, The Journal of chemical physics, 103(3), 1995, pp. 1064-1076
A series of size-consistent approximations to the equation-of-motion c
oupled cluster method in the singles and doubles approximation (EOM-CC
SD) are developed by subjecting the similarity transformed Hamiltonian
($) over bar H=exp(-T)H exp(T) to a perturbation expansion. Attention
is directed to N and N-1 electron final state realizations of the met
hod defined by truncation of H at second order. Explicit spin-orbital
equations for the energy and its first derivative are documented for b
oth approaches [EOMEE-CCSD(2) and EOMIP-CCSD(2), respectively], and ha
ve been implemented in a large-scale quantum chemistry pro,sram. Verti
cal ionization potentials calculated by EOMIP-CCSD(2) are shown to be
equivalent to those of an approach presented recently by Nooijen and S
nijders [J. Chem. Phys. 102, 1681 (1995)]. Applications of both EOMIP-
CCSD(2) and EOMEE-CCSD(2) provide results for final state properties t
hat compare favorably with these obtained in full EOM-CCSD calculation
s. Analysis of the computational aspects of the approximate and full E
OM-CCSD methods shows that the cost of EOMIP-CCSD(2) energy and gradie
nt calculations scales in proportion to the fifth power of the basis s
et size, a significant savings over the sixth power dependence of EOMI
P-CCSD. This feature is of great practical importance, as it shows tha
t this N-1 electron final state approach has a large domain of applica
bility and is therefore likely to become a valuable tool for applicati
on calculations. On the other hand, the same cannot be said for EOMEE-
CCSD(2) since its asymptotic computational dependence and storage requ
irements are the same as the full EOMEE-CCSD method. (C) 1995 American
Institute of Physics.