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Self-Consistent Equations Including Exchange and Correlation Effects

Why this mattered

Kohn and Sham turned the Hohenberg–Kohn existence theorem for density functional theory into a practical computational framework. The key move was to replace the many-electron interacting problem with self-consistent one-electron equations for a fictitious noninteracting system having the same ground-state density. All difficult many-body effects were gathered into an exchange-correlation potential, approximated in the paper using properties of the uniform electron gas. This made density, rather than the many-electron wavefunction, the central object of electronic-structure calculation.

The paradigm shift was practical as much as conceptual: after this paper, electronic structure could be computed for real solids, molecules, surfaces, and later nanostructures without explicitly tracking the exponentially complex many-electron wavefunction. The resulting Kohn–Sham equations gave researchers a tractable route between simple Hartree-like mean-field models and full many-body theory, enabling calculations accurate enough for chemistry and materials science while remaining scalable enough for broad use.

Subsequent breakthroughs in local, gradient-corrected, hybrid, and more specialized exchange-correlation functionals all grew from the structure this paper defined. Modern computational materials discovery, quantum chemistry workflows, surface catalysis modeling, semiconductor and metal physics, and much of first-principles condensed-matter simulation rely on the Kohn–Sham formulation. Its enormous citation count reflects that it did not merely improve an existing method; it established the standard language in which interacting-electron ground-state problems are still most often made computable.

Abstract

From a theory of Hohenberg and Kohn, approximation methods for treating an inhomogeneous system of interacting electrons are developed. These methods are exact for systems of slowly varying or high density. For the ground state, they lead to self-consistent equations analogous to the Hartree and Hartree-Fock equations, respectively. In these equations the exchange and correlation portions of the chemical potential of a uniform electron gas appear as additional effective potentials. (The exchange portion of our effective potential differs from that due to Slater by a factor of $\frac{2}{3}$.) Electronic systems at finite temperatures and in magnetic fields are also treated by similar methods. An appendix deals with a further correction for systems with short-wavelength density oscillations.

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