1. If I have PBE+SOC based WAVECAR and WAVEDER files for a semiconductor, I want to use ALGO=TDHF and LADDER=.True. to get the exciton effect. I also add LHARTREE = .TRUE. and AEXX = 0.25, but I don't set LMODELHF and HFSCREEN. It should work, right?
If these are the tags in your TDDFT
INCAR, then yes. If you would use the same PBE0 hybrid functional for the ground state, this approximation would be equivalent to proper TD-PBE0. However, what you are proposing here would be a combination of PBE for the ground state and TD-PBE0 for optical properties, which is also possible in VASP.
Then How to choose the value for AEXX? You said here AEXX is the screening of the electron-hole interaction. How to choose this value under LMODELHF=.False. ?
This is not an easy question. In TDDFT,
AEXX comes from the fraction of exact exchange in the exchange-correlation potential, but this choice is not a well-defined procedure. Essentially, your question is related to the general choice of the hybrid functional and it doesn't have an easy answer.
Usually, in TDDFT calculations, the same hybrid functional is used for the ground state calculation (
ALGO=Normal) and the optical absorption calculation (
ALGO=TDHF). But as I said earlier, in VASP, any ground state can be used with any approximation in TDHF.
2. Similar as in 1. If I turn on LMODELHF=.True. , then I need AEXX and HFSCREEN. Again, how to get the values of the AEXX and HFSCREEN? Can I use the same procedure as mentioned in your tutorial (get 1/epsilon_infinite, and fit the RPA dielectric function vs. G)? even here my ground state is from PBE+SOC, not from a hybrid functional?
Yes, you can start your TDHF calculation with the model dielectric function (
LMODELHF) from any ground state calculation. In the scheme you described, that would be PBE.
The approach with the model dielectric function (
LMODELHF) can be seen as an approximation for the RPA dielectric function, so one has to provide the parameters for the model, i.e.,
AEXX and
HFSCREEN. One way to approach it is to fit the RPA dielectric function as done in
Ref. [1,2]. In other works, the parameters for this model were determined without the costly RPA calculations [3,4].
In the tutorial, we use DDH calculations with the model dielectric function for the ground state and TD-DDH for the optical absorption calculations, which allows us to use the same hybrid functional consistently for the ground state as well as the optical excitations and yields accurate results [5].
[1] M. Bokdam, T. S, er, Aless, r. Stroppa, S. Picozzi, D.D. Sarma, C. Franchini, G. Kresse, Sci Rep 6, 28618 (2016)
[2] W. Chen, G. Miceli, G. Rignanese, A. Pasquarello, Phys. Rev. Materials 2, 073803 (2018)
[3] C. Zhi-Hao, W. Yue-Chao, Z. Min-Ye, X. Xi, J. Hong, J. Phys. Chem. Lett. 9, 2338-2345 (2018)
[4] H. Wang, A. Tal, T. Bischoff, P. Gono, A. Pasquarello, npj Comput Mater 8, 237 (2022)
[5] A. Tal, P. Liu, G. Kresse, A. Pasquarello, Phys. Rev. Research 2, 032019 (2020)