Category:Exchange-correlation functionals: Difference between revisions

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\hat{V}_{\rm nn} = \sum_{A=1}^{M-1}\sum_{B=A+1}^{M}
V_{\rm nn} = \frac{1}{2}\sum_{A\noteq B}^{M-1}
\frac{e^{2}}{4\pi\epsilon_{0}}
\frac{Z_{A}Z_{B}}{\left\vert{\bf R}_{A}-{\bf R}_{B}\right\vert}
\frac{Z_{A}Z_{B}}{\left\vert{\bf R}_{A}-{\bf R}_{B}\right\vert}
</math>
</math>

Revision as of 10:48, 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.

Failed to parse (Conversion error. Server ("cli") reported: "[INVALID]"): {\displaystyle V_{\rm nn} = \frac{1}{2}\sum_{A\noteq B}^{M-1} \frac{Z_{A}Z_{B}}{\left\vert{\bf R}_{A}-{\bf R}_{B}\right\vert} }

Theoretical Background

How to


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Pages in category "Exchange-correlation functionals"

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