GGA: Difference between revisions
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|03 || range-separated ACFDT (LDA - sr RPA) <math>\mu=0.3 \AA^3</math> | |03 || range-separated ACFDT (LDA - sr RPA) <math>\mu=0.3 \AA^3</math> | ||
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|05 || range-separated ACFDT (LDA - sr RPA) <math>\mu=0.5 \AA^3 | |05 || range-separated ACFDT (LDA - sr RPA) <math>\mu=0.5 \AA^3</math> | ||
|- | |- | ||
|03 || range-separated ACFDT (LDA - sr RPA) <math>\mu=1.0 \AA^3</math> | |03 || range-separated ACFDT (LDA - sr RPA) <math>\mu=1.0 \AA^3</math> | ||
|- | |- | ||
|05 || range-separated ACFDT (LDA - sr RPA) <math>\mu=2.0 \AA^3 | |05 || range-separated ACFDT (LDA - sr RPA) <math>\mu=2.0 \AA^3</math> | ||
|- | |- | ||
|PL || new RPA+ Perdew Wang (by Judith Harl) | |PL || new RPA+ Perdew Wang (by Judith Harl) | ||
Revision as of 12:04, 2 February 2017
GGA = 91 | PE | RP | PS | AM
Default: GGA = type of exchange-correlation in accordance with the POTCAR file
Description: GGA specifies the type of generalized-gradient-approximation one wishes to use.
This tag was added to perform GGA calculation with pseudopotentials generated with conventional LDA reference configurations.
Possible options are:
GGA Description 91 Perdew -Wang 91 PE Perdew-Burke-Ernzerhof RP revised Perdew-Burke-Ernzerhof AM AM05[1][2][3] HL Hendin-Lundqvist[4] CA Ceperley-Alder[5] PZ Ceperley-Alder, parametrization of Perdew-Zunger[6] WI Wigner[7] RP RPBE with Pade Approximation[8] VW Vosko-Wilk-Nusair[9] (VWN) B3 B3LYP[10] (Joachim Paier), where LDA part is with VWN3-correlation B5 B3LYP (Joachim Paier), where LDA part is with VWN5-correlation BF BEEF[11], xc (with libbeef) CO no exchange-correlation PS Perdew-Burke-Ernzerhof revised for solids (PBEsol)[12] for range-separated ACFDT: RA new RPA Perdew Wang (by Judith Harl) 03 range-separated ACFDT (LDA - sr RPA) 05 range-separated ACFDT (LDA - sr RPA) 03 range-separated ACFDT (LDA - sr RPA) 05 range-separated ACFDT (LDA - sr RPA) PL new RPA+ Perdew Wang (by Judith Harl) for vdW (Jiri Klimes): RE revPBE[13] OR optPBE BO optB88 MK optB86b
The tags AM (AM05) and PS (PBEsol) are only supported by VASP.5.X. The AM05 functional and the PBEsol functional are constructed using different principles, but both aim at a decent description of yellium surface energies. In practice, they yield quite similar results for most materials. Both are available for spin polarized calculations.
References
- ↑ R. Armiento and A. E. Mattsson, Phys. Rev. B 72, 085108 (2005).
- ↑ A. E. Mattsson, R. Armiento, J. Paier, G. Kresse, J.M. Wills, and T.R. Mattsson, J. Chem. Phys. 128, 084714 (2008).
- ↑ A. E. Mattsson and R. Armiento, Phys. Rev. B 79, 155101 (2009).
- ↑ L. Hedin and B. I. Lundqvist, J. Phys. C 4, 2064 (1971).
- ↑ D. M. Ceperley and B. J. Alder, Phys. Rev. Lett. 45, 566 (1980).
- ↑ J. P. Perdew and Alex Zunger, Phys. Rev. B 23, 5048 (1981).
- ↑ E. Wigner, J. Chem. Phys. 5, 726 (1937).
- ↑ B. Hammer, L. B. Hansen and J. K. Nørskov, Phys. Rev. B 59, 7413 (1999).
- ↑ S. H. Vosko, L. Wilk and M. Nusair, Can. J. Phys. 58, 1200 (1980).
- ↑ A. D. Becke, J. Chem. Phys. 98, 5648 (1993).
- ↑ Jess Wellendorff, Keld T. Lundgaard, Andreas Møgelhøj, Vivien Petzold, David D. Landis, Jens K. Nørskov, Thomas Bligaard and Karsten W. Jacobsen, Phys. Rev. B 85, 235149 (2012).
- ↑ J. P. Perdew, A. Ruzsinszky, G. I. Csonka, O. A. Vydrov, G. E. Scuseria, L. A. Constantin, X. Zhou, and K. Burke, Phys. Rev. Lett. 100, 136406 (2008).
- ↑ Y. Zhang and W. Yang, Phys. Rev. Lett. 80, 890 (1998).