Category:Exchange-correlation functionals

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In the Kohn-Sham (KS) formulation of density functional theory (DFT)[1][2], the total energy is given by

[math]\displaystyle{ E_{\rm tot}^{\rm KS} = -\frac{1}{2}\sum_{i}\int\psi_{i}^{*}({\bf r})\nabla^{2}\psi_{i}({\bf r})d^{3}r + \frac{1}{2}\int\int\frac{\rho({\bf r})\rho({\bf r'})}{\left\vert{\bf r}-{\bf r'}\right\vert}d^{3}rd^{3}r' + E_{\rm xc} + \int v_{\rm en}({\bf r})\rho({\bf r})d^{3}r + \frac{1}{2}\sum_{A\ne B}\frac{Z_{A}Z_{B}}{\left\vert{\bf R}_{A}-{\bf R}_{B}\right\vert} }[/math]

where the terms on the left-hand side represent the non-interacting kinetic energy of the electrons, the Classical Coulomb Hartree term, the exchange-correlation energy, the electrons-nuclei attraction energy and the nuclei-nuclei repulsion energy. The orbitals [math]\displaystyle{ \psi_{i} }[/math] and the electron density [math]\displaystyle{ \rho=\sum_{i}\left\vert\psi_{i}\right\vert^{2} }[/math] a

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Pages in category "Exchange-correlation functionals"

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