Hi all,
I am calculating GW band structures of AA′-stacked TMDC bilayers using QE + BerkeleyGW with Wannier interpolation (sig2wan).
For MoSe₂–WSe₂ (AA′): PBE-DFT gives an indirect gap. GW shifts the CBM to K, giving a direct quasiparticle gap
For MoSe₂–MoSe₂ (AA′): The gap character remains the same in DFT and GW.
Is it reasonable that GW gives this result (indirect → direct) in the heterobilayer, or should this be treated as an issue?
I am uploading input/output files for reference and the Band Structure plots (Comparison of DFT/Wannier and GW band structures)
P.S: Key parameters:
GW: num_bands = 200
Thank you.
Dear Zhenglu,
Thank you very much for your clarification and for emphasising the importance of careful GW convergence in 2D systems.
I understand your concern that a limited number of bands can lead to misleading GW results. In my tests so far, I increased the number of bands from 200 up to 400 while keeping the same dielectric and self-energy parameters, and the nature of the gap (direct vs. indirect) remained unchanged. However, I fully agree that this alone does not establish convergence.
I also wanted to ask for your perspective regarding the comparison with existing literature. For example, in a recent GW-BSE study (https://doi.org/10.48550/arXiv.2509.14200) on bilayer MoS2 using BerkeleyGW (G0W0 with PBE), the authors report converged quasiparticle and optical properties using 200 bands, an 8 Ry dielectric cutoff. They note that these settings are sufficient to reproduce consistent band gaps and spectra.
And, I would appreciate your advice on how to interpret such results when benchmarking my calculations.
Thank you again for your time and guidance.
Best regards,
Agathyan