Abstract

The dependence of ab initio many-body perturbation theory within the GWGW approximation on the eigensystem used in calculating quasiparticle corrections limits this method's predictive power. Here, we investigate the accuracy of the recently developed Wannier-localized optimally tuned screened range-separated hybrid (WOT-SRSH) functional as a generalized Kohn-Sham starting point for single-shot GWGW (G0W0G_0W_0) calculations for a range of semiconductors and insulators. Comparison to calculations based on well-established functionals, namely PBE, PBE0, and HSE, as well as to self-consistent GWGW schemes and to experiment, shows that band gaps computed via G0W0G_0W_0@WOT-SRSH have a level of precision and accuracy that is comparable to that of more advanced methods such as quasiparticle self-consistent GWGW (QSGWGW) and eigenvalue self-consistent GWGW (evGWGW). We also find that G0W0G_0W_0@WOT-SRSH improves the description of states deeper in the valence band manifold. Finally, we show that G0W0G_0W_0@WOT-SRSH significantly reduces the sensitivity of computed band gaps to ambiguities in the underlying WOT-SRSH tuning procedure.

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