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Local-density approximationThe local-density approximation (LDA) is an approximation of the exchange-correlation (XC) energy functional in density functional theory (DFT) by taking the XC energy of an electron in a non-interacting homogeneous electron gas of a density equivalent to the density at the electron in the system being calculated. This approximation was applied to DFT by Kohn and Sham in an early paper.[1] Additional recommended knowledgeThe Hohenberg-Kohn theorem states that the energy of the ground state of a system of electrons is a functional of the electronic density, in particular the exchange and correlation energy is also a functional of the density (this energy can be seen as the quantum part of the electron-electron interaction). This XC functional is not known exactly and must be approximated.[2] LDA is the simplest approximation for this functional, it is local in the sense that the electron exchange and correlation energy at any point in space is a function of the electron density at that point only.[3] The LDA functional assumes that the per-electron exchange-correlation energy at every point in space is equal to the per-electron exchange-correlation energy of a homogeneous electron gas.[1] The XC correlation functional is the sum of a correlation functional and an exchange functional[1] ExchangeLDA uses the exchange for the uniform electron gas of a density equal to the density at the point where the exchange is to be evaluated, in SI units where CorrelationThere are several forms of correlation:
Wigner correlation is gotten by using equally spaced electrons and applying perturbation theory.[5] VWN, PZ and PW92 are fit to a quantum Monte Carlo calculation[12] of the electron gas at varying densities.[11] LYP is based on data fit to the helium atom.[10] References
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This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Local-density_approximation". A list of authors is available in Wikipedia. |