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 + \int v_{\rm ext}({\bf r})\rho({\bf r})d^{3}r + E_{\rm xc} + \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' + \frac{1}{2}\sum_{A\ne B}\frac{Z_{A}Z_{B}}{\left\vert{\bf R}_{A}-{\bf R}_{B}\right\vert} }[/math]

where

[math]\displaystyle{ T_{\rm s}[\{\psi_{i}\}]=-\frac{1}{2}\sum_{i=1}^{N}\int \psi_{i}^{*}({\bf r})\nabla^{2}\psi_{i}({\bf r})d^{3}r }[/math]

is the non-interacting kinetic energy of the electrons,

[math]\displaystyle{ U_{\rm H}[\rho] = \int v_{\rm ext}({\bf r})\rho({\bf r})d^{3}r }[/math]

is the Classical Coulomb Hartree term,

[math]\displaystyle{ V_{\rm en}[\rho] = \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', }[/math]

is the electrons-nuclei attraction energy and

[math]\displaystyle{ V_{\rm nn} = \frac{1}{2}\sum_{A\ne B} \frac{Z_{A}Z_{B}}{\left\vert{\bf R}_{A}-{\bf R}_{B}\right\vert} }[/math]

is the nuclei-nuclei repulsion energy.

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Pages in category "Exchange-correlation functionals"

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