Thanks Henrique! I'm aware of both papers and yes agreed they generally indicate good agreement with AE calculations.
From the procedures/recommendations in the Bosoni et al. paper and internal benchmarks, I've primarily been using the hard pseudos for f-block elements. Still, there are only a few hard pseudos for the main group in the 64 release
I'm asking in the context of developing datasets for ML interatomic potentials where a fixed set of pseudopotentials is require to avoid ambiguities in the vacuum levels of different pseudopotentials (e.g., using a harder pseudo only for higher-pressure phases can change the vacuum level even with the same XC functional). The properties I'm looking at would be total energies, Hellmann-Feynman forces, and stress, and especially for distorted / higher-pressure phases
I have two major concerns then, based mostly on older literature:
* The Kresse and Joubert PAW paper makes it clear that terms in the total energy involving overlap of pseudo-cores are neglected. So in cases with "strong" overlap, there could be significant errors in the PAW formalism
* Another paper from Kresse and coworkers suggests errors in energy differences on the order of 10 meV/atom due to overlap of pseudocores
The question would be: How significant are these errors given modern PAWs and have there been any recent tests of errors due to pseudocore overlap?