Category:Exchange-correlation functionals: Difference between revisions

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</math>
</math>
where <math>T_{\rm s}</math> is the non-interacting kinetic energy of the electrons, <math>J</math> the Hartree energy, the third term is the energy of the electrons-nuclei attraction interaction, and <math>V_{\rm nn}</math> is the nuclei-nuclei repulsion energy.
where <math>T_{\rm s}</math> is the non-interacting kinetic energy of the electrons, <math>J</math> the Hartree energy, the third term is the energy of the electrons-nuclei attraction interaction, and <math>V_{\rm nn}</math> is the nuclei-nuclei repulsion energy.
:<math>
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>
:<math>
U_{\rm H}[\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>
:<math>
:<math>
U_{\rm H}[\rho] = \int v_{\rm ext}({\bf r})\rho({\bf r})d^{3}r
U_{\rm H}[\rho] = \int v_{\rm ext}({\bf r})\rho({\bf r})d^{3}r

Revision as of 10:36, 18 January 2022

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

where is the non-interacting kinetic energy of the electrons, the Hartree energy, the third term is the energy of the electrons-nuclei attraction interaction, and is the nuclei-nuclei repulsion energy.

Theoretical Background

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Pages in category "Exchange-correlation functionals"

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