Handling f electrons
Posted: Sat Dec 17, 2005 9:21 pm
I'm doing some calculations on a Ce-containing perovskite.
Formally this should be Ce III. Yet if I do the calulation with the standard Ce potential, in which the f electon is "valence" (allowing Ce IV), I get an energy that is 0.2 eV/atom lower than if I use the Ce_3, frozen f potential. Now I realise that the VASP total energy is only an approximation to the true cohesive energy, but this is quite a large energy difference. In addition, the calculated charge density suggests that if allowed, the Ce f electron delocalises. However, that's of course subject to the RWIGS, which I haven't explored very much.
My question is, what is the most appropriate way to treat this system? My normal reaction would be that adding more electrons to the valence space should not change the solution if they are supposed to stay localised, whereas artificially freezing them (using the Ce_3 potential) can cause spurious results.
A related issue is what is the reference state for these heavy elements for the potential-generation code? Are they forced to be spherically-symmetric? Can this symmetrisation of the reference f electron account for the observed 0.2 eV/atom stabalisation?
And on that note, is there a Ce_3 LDA potential available?
Formally this should be Ce III. Yet if I do the calulation with the standard Ce potential, in which the f electon is "valence" (allowing Ce IV), I get an energy that is 0.2 eV/atom lower than if I use the Ce_3, frozen f potential. Now I realise that the VASP total energy is only an approximation to the true cohesive energy, but this is quite a large energy difference. In addition, the calculated charge density suggests that if allowed, the Ce f electron delocalises. However, that's of course subject to the RWIGS, which I haven't explored very much.
My question is, what is the most appropriate way to treat this system? My normal reaction would be that adding more electrons to the valence space should not change the solution if they are supposed to stay localised, whereas artificially freezing them (using the Ce_3 potential) can cause spurious results.
A related issue is what is the reference state for these heavy elements for the potential-generation code? Are they forced to be spherically-symmetric? Can this symmetrisation of the reference f electron account for the observed 0.2 eV/atom stabalisation?
And on that note, is there a Ce_3 LDA potential available?