Effective Hamiltonians and effective operators act on a restricted model sp
ace to give the same energies and matrix elements as those of the full Hami
ltonian and operators between the corresponding true eigenstates. For the e
ffective Hamiltonian there are two "obvious" choices: the simplest non-Herm
itian effective Hamiltonian and the canonical Hermitian effective Hamiltoni
an. In this paper, we derive a perturbative effective operator which works
together with the non-Hermitian effective Hamiltonian, prove that it can be
expanded with only connected diagrams, and show how to construct the conne
cted diagrams easily from the diagrams of the effective Hamiltonian by subs
titution of vertices. This effective operator is much simpler than the Herm
itian effective operator and therefore is expected to be more suitable for
ab initio calculations. (C) 2001 American Institute of Physics.