List of hybrid functionals: Difference between revisions
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:with the default values {{TAG|AEXX}}=0.25, {{TAG|AGGAX}}=1-{{TAG|AEXX}}=0.75, {{TAG|AGGAC}}=1.0, and {{TAG|ALDAC}}=1.0. | :with the default values {{TAG|AEXX}}=0.25, {{TAG|AGGAX}}=1-{{TAG|AEXX}}=0.75, {{TAG|AGGAC}}=1.0, and {{TAG|ALDAC}}=1.0. | ||
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*HSEsol{{cite|berger:cpl:2005}} | |||
{{TAG|LHFCALC}} = .TRUE. | |||
{{TAG|GGA}} = CA (or PZ) | |||
{{TAG|HFSCREEN}} = 0.5 | |||
:with the default values {{TAG|AEXX}}=1.0, {{TAG|AGGAX}}=1-{{TAG|AEXX}}=0.75, {{TAG|AGGAC}}=1.0, and {{TAG|ALDAC}}=1.0. | |||
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=== Unscreened hybrid functionals === | === Unscreened hybrid functionals === |
Revision as of 07:08, 18 October 2023
A certain number of hybrid functionals are available in VASP, and furthermore if VASP is compiled with the library of exchange-correlation functionals Libxc, then most of the existing hybrid functionals can be used[1]. Examples of INCAR files are shown below. Since VASP.6.4.0 it is possible to use hybrid functionals that mix meta-GGA and Hartree-Fock exchange. Note that it is in general recommended to use the PBE POTCAR files for hybrid functionals.
Range-separated hybrid functionals
- HSE06[2]
LHFCALC = .TRUE. GGA = PE HFSCREEN = 0.2
LHFCALC = .TRUE. GGA = PE HFSCREEN = 0.3
- HSEsol[6]
LHFCALC = .TRUE. GGA = PS HFSCREEN = 0.2
- HSEsol
LHFCALC = .TRUE. GGA = CA (or PZ) HFSCREEN = 0.5
Unscreened hybrid functionals
LHFCALC = .TRUE. GGA = PE
- B3LYP[10] with VWN3 (or VWN5) for LDA correlation
LHFCALC = .TRUE. GGA = B3 (or B5) AEXX = 0.2 AGGAX = 0.72 AGGAC = 0.81 ALDAC = 0.19
LHFCALC = .TRUE. GGA = LIBXC LIBXC1 = HYB_GGA_XC_B3PW91 # or 401 AEXX = 0.2
LHFCALC = .TRUE. GGA = LIBXC LIBXC1 = HYB_GGA_XC_B1WC # or 412 AEXX = 0.16
- SCAN0
LHFCALC = .TRUE. METAGGA = SCAN
- Hartree-Fock (no correlation)
LHFCALC = .TRUE. AEXX = 1.0
Related tags and articles
GGA, METAGGA, LIBXC1, LIBXC2, AEXX, ALDAX, ALDAC, AGGAX, AGGAC, AMGGAX, AMGGAC, LHFCALC, HFSCREEN, LRHFCALC
References
- ↑ https://libxc.gitlab.io/functionals/
- ↑ A. V. Krukau , O. A. Vydrov, A. F. Izmaylov, and G. E. Scuseria, J. Chem. Phys. 125, 224106 (2006).
- ↑ J. Heyd, G. E. Scuseria, and M. Ernzerhof, J. Chem. Phys. 118, 8207 (2003).
- ↑ J. Heyd and G. E. Scuseria, J. Chem. Phys. 121, 1187 (2004).
- ↑ J. Heyd, G. E. Scuseria, and M. Ernzerhof, J. Chem. Phys. 124, 219906 (2006).
- ↑ L. Schimka, J. Harl, and G. Kresse, J. Chem. Phys. 134, 024116 (2011).
- ↑ J. P. Perdew, M. Ernzerhof, and K. Burke, J. Chem. Phys. 105, 9982 (1996).
- ↑ M. Ernzerhof and G. E. Scuseria, J. Chem. Phys. 110, 5029 (1999).
- ↑ C. Adamo and V. Barone, Phys. Rev. Lett., 110, 6158 (1999).
- ↑ P. J. Stephens, F. J. Devlin, C. F. Chabalowski, and M. J. Frisch, J. Phys. Chem. 98, 11623 (1994).
- ↑ A. D. Becke, J. Chem. Phys. 98, 5648 (1993).
- ↑ D. I. Bilc, R. Orlando, R. Shaltaf, G.-M. Rignanese, J. Iniguez, and P. Ghosez, Phys. Rev. B 77, 165107 (2008).