The GW and BSE workflows implemented in atomate2 are built for automating these multistep and interdependent calculations. For example, the calculation of quasiparticle energies using Abinit involves a four-step calculation. First, one performs a standard DFT (SCF) calculation to obtain self-consistent charge density which is then used to perform an exact diagonalization calculation (NSCF) to generate a large number of unoccupied bands required for the actual GW calculation. Once these bands are generated the inverse dielec- The implementation of the GW workflow for FHI-aims is simpler, as FHI-aims allows the user to run a SCF calculation and all the post-SCF steps in one run. However, if one wants to study the convergence of the quasiparticle energies on the parameters defining the GW calculation, such as the number of frequency points used to expand the elements of self-energy on the imaginary frequency axis, or the type of its analytical continuation on the real frequency axis, they can effectively re-use the results of the SCF part of the calculation by restarting the calculations from the converged charge density. This functionality is implemented in GWMaker for FHI-aims. GWConvergenceMaker, allowing the study of the convergence of GW results with respect to calculation parameters, is also implemented similarly to the ABINIT workflows.