We present theoretical calculations of quasiparticle energies in closed-shell molecules using the GW method. We compare three different approaches: a full-frequency (FF-) method with density functional theory (DFT-PBE) used as a starting mean field; a full-frequency (FF-) method where the interacting Green’s function is approximated by replacing the DFT energies with self-consistent quasiparticle energies or Hartree-Fock energies; and a method with a Hybertsen-Louie generalized plasmon-pole model (HL GPP-). While the latter two methods lead to good agreement with experimental ionization potentials and electron affinities for methane, ozone, and beryllium oxide molecules, FF- results can differ by more than one electron volt from experiment. We trace this failure of the FF- method to the occurrence of incorrect self-energy poles describing shake-up processes in the vicinity of the quasiparticle energies.

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