Self-consistent solution of the Dyson equation for atoms and molecules within a conserving approximation A novel method for the solution of the Schrödinger equation in the presence of exchange terms J. Chem. Phys. 118, 9149 (2003); 10.1063/1.1567254 Self-consistent solution of Dyson's equation up to second order for open-shell atomic systemsIn this paper, the single-particle Green's function approach is applied to the atomic many-body problem. We present the self-consistent solution of the Dyson equation up to second order in the self-energy for nonrelativistic spin-compensated atoms. This Dyson second-order scheme requires the solution of the Hartree-Fock integro-differential equations as a preliminary step, which is performed in coordinate space ͑i.e., without an expansion in a basis set͒. To cope with the huge amount of poles generated in the iterative approach to tackle Dyson's equation in second order, the BAGEL ͑BAsis GEnerated by Lanczos͒ algorithm is employed. The self-consistent scheme is tested on the atomic systems He, Be, Ne, Mg, and Ar with spin-saturated ground state 1 S 0 . Predictions of the total binding energy, ionization energy, and single-particle levels are compared with those of other computational schemes ͓density functional theory, Hartree-Fock ͑HF͒, post-HF, and configuration interaction͔ and with experiment. The correlations included in the Dyson second-order algorithm produce a shift of the Hartree-Fock single-particle energies that allow for a close agreement with experiment.