Reproducibility in Calculations for Solids
arXiv:1903.06865 · doi:10.1016/j.cpc.2020.107242
Abstract
Ab initio many-body perturbation theory within the approximation is a Green's function formalism widely used in the calculation of quasiparticle excitation energies of solids. In what has become an increasingly standard approach, Kohn-Sham eigenenergies, generated from a DFT calculation with a strategically-chosen exchange correlation functional ``starting point'', are used to construct and , and then perturbatively corrected by the resultant self-energy. In practice, there are several ways to construct the self-energy, and these can lead to variations in predicted quasiparticle energies. For example, for ZnO and TiO, reported fundamental gaps can vary by more than 1 eV. In this work, we address the convergence and key approximations in contemporary calculations, including frequency-integration schemes and the treatment of the Coulomb divergence in the exact-exchange term. We study several systems,and compare three different codes: BerkeleyGW, Abinit and Yambo. We demonstrate, for the first time, that the same quasiparticle energies for systems in the condensed phase can be obtained with different codes, and we provide a comprehensive assessment of implementations of the approximation.
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