Workshop | Announcement | Programme | FHI98md

Exchange-correlation energy: From LDA to GGA and beyond

Martin Fuchs
Unité PCPM, Université Catholique de Louvain, 1348 Louvain-la-Neuve, Belgium

Abstract

Density-functional theory reduces the quantum mechanical many-electron groundstate problem to self-consistent one electron form through the Kohn-Sham equations [1,2]. In this formally exact theory, the many-electron exchange and correlation effects are described by the exchange-correlation functional. Except in limiting cases such as the homogeneous electron gas the explicit form of this functional is not known however. In DFT calculations of real systems one must therefore use approximations for the exchange-correlation functional, and it is important to be aware where these work and where they break down.

The local (spin) density approximation (LDA) [3], having long been the standard choice, provides a realistic description of the atomic structure, elastic and vibrational properties for a wide range of systems. Yet the LDA is not reliable enough to describe the energetics of chemical reactions, say, reaction enthalpies and activation energy barriers. In particular, it leads to binding energies of molecules and solids which are overestimated on the order of $\approx 1$~eV/atom. Also several cases are documented where the LDA puts molecular conformations or crystal bulk phases in an even qualitatively wrong energetic order.

The more recent generalized gradient approximations (GGA's) [4] have overcome such deficiencies to a large extent, giving, for instance, a more realistic account of energy barriers and adsorption energies for molecules on metal or semiconductor surfaces. At the same time GGA's are computationally as simple to use as the LDA. On the other hand, the results of many applications as well as formal analysis suggest [5] that GGA functionals are still too limited to yield a fully consistent improvement over the LDA and to describe binding energies within the desired "chemical accuracy" (better than 1 kcal/mol or 50 meV/atom) in general.

In this lecture we review present formulations of the GGA and compare them with the LDA, examine general trends and specific examples to illustrate what should or should not be expected from them. To complement this "phenomenological" view, we consider the exact exchange-correlation functional, in terms of the exchange-correlation hole and the adiabatic connection, and discuss how important aspects, for instance sum rules, are retained in approximate functionals like the LDA and GGA. In addition we look at orbital-dependent exchange-correlation functionals (such as exact Kohn-Sham exchange [6], hybrid functionals [7], Meta GGA's [8], and functionals based on the fluctuation-dissipation theorem [9]) that are being explored in the quest for ever more accurate and more widely applicable exchange-correlation functionals.

Literature

  1. R. G. Parr and W. Yang, Density Functional Theory of Atoms and Molecules (Oxford University Press, New York, 1989).
  2. W. Kohn, A. D. Becke and R. G. Parr, Density functional theory of electronic structure, J. Chem. Phys. 100, 12 974 (1996).
  3. R. O. Jones and O. Gunnarsson, The density functional formalism, its applications and prospects, Rev. Mod. Phys. 61, 689 (1989).
  4. M. Ernzerhof, J. P. Perdew and K. Burke, Density functionals: Where do they come from, why do they work?, in Topics in Current Chemistry, Vol. 180, edited by R. F. Nalewajski (Springer, Berlin, 1996).
  5. A. Zupan, K. Burke, M. Ernzerhof and J.P. Perdew, Distributions and averages of electron density parameters: Explaining the effects of gradient corrections, J. Chem. Phys. 106, 10 184 (1997); N. Moll, M. Bockstedte, M. Fuchs, E. Pehlke and M. Scheffler, Application of generalized gradient approximations: The diamond-beta-tin phase transition in Si and Ge, Phys. Rev. B 52, 2550 (1995); B. Hammer, L. B. Hansen and J. K. Nørskov, Improved adsorption energetics within density-functional theory using revised Perdew-Burke-Ernzerhof functionals, Phys. Rev. B 59, 7413 (1999).
  6. M. Städele, M. Moukara, J.A. Majewski, P. Vogl and A. Görling, Exact exchange Kohn-Sham formalism applied to semiconductors, Phys. Rev. B 59, 10 031 (1999).
  7. A. D. Becke, Density-functional thermochemistry III. The role of exact exchange, J. Chem. Phys. 98, 5648 (1993); K. Burke, M. Ernzerhof and J. P. Perdew, The adiabatic connection method: A non­empirical hybrid, Chem. Phys. Lett. 265, 115 (1997).
  8. A. D. Becke, A new inhomogeneity parameter in density-functional theory, J. Chem. Phys. 109, 2092 (1998); J. P. Perdew, S. Kurth, A. Zupan and P. Blaha, Accurate density functional with correct formal properties: A step beyond the generalized gradient approximation, Phys. Rev. Lett. 82, 2544 (1999).
  9. J. F. Dobson and J. Wang, Energy-optimized local exchange-correlation kernel for the electron gas: Application to van der Waals forces, Phys. Rev. B 62, 10 038 (2000); W. Kohn, Y. Meir and D. E. Makarov, Van der Waals energies in density functional theory, Phys. Rev. Lett. 80, 4153 (1998).

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