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Atoms, molecules, solids, and surfaces: Applications of the generalized gradient approximation for exchange and correlation

John P. PerdewDepartment of Physics and Quantum Theory Group, Tulane University, New Orleans, Louisiana 70118J. A. ChevaryDepartment of Physics and Quantum Theory Group, Tulane University, New Orleans, Louisiana 70118S. H. VoskoDepartment of Physics, University of Toronto, Toronto, Ontario, Canada M5S 1A7Koblar Alan JacksonDepartment of Physics and Quantum Theory Group, Tulane University, New Orleans, Louisiana 70118Mark R. PedersonDepartment of Physics and Quantum Theory Group, Tulane University, New Orleans, Louisiana 70118David J. SinghComplex Systems Theory Branch, Naval Research Laboratory, Washington, D.C. 20375-5000Carlos FiolhaisDepartment of Physics, University of Coimbra, 3000 Coimbra, Portugal
1992en
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Generalized gradient approximations (GGA's) seek to improve upon the accuracy of the local-spin-density (LSD) approximation in electronic-structure calculations. Perdew and Wang have developed a GGA based on real-space cutoff of the spurious long-range components of the second-order gradient expansion for the exchange-correlation hole. We have found that this density functional performs well in numerical tests for a variety of systems: (1) Total energies of 30 atoms are highly accurate. (2) Ionization energies and electron affinities are improved in a statistical sense, although significant interconfigurational and interterm errors remain. (3) Accurate atomization energies are found for seven hydrocarbon molecules, with a rms error per bond of 0.1 eV, compared with 0.7 eV for the LSD approximation and 2.4 eV for the Hartree-Fock approximation. (4) For atoms and molecules, there is a cancellation of error between density functionals for exchange and correlation, which is most striking whenever the Hartree-Fock result is furthest from experiment. (5) The surprising LSD underestimation of the lattice constants of Li and Na by 3--4 % is corrected, and the magnetic ground state of solid Fe is restored. (6) The work function, surface energy (neglecting the long-range contribution), and curvature energy of a metallic surface are all slightly reduced in comparison with LSD. Taking account of the positive long-range contribution, we find surface and curvature energies in good agreement with experimental or exact values. Finally, a way is found to visualize and understand the nonlocality of exchange and correlation, its origins, and its physical effects.

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