Category:Exchange-correlation functionals: Difference between revisions

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E_{\rm tot} = -\frac{1}{2}\sum_{i}\int\psi_{i}^{*}({\bf r})\nabla^{2}\psi_{i}({\bf r})d^{3}r - \sum_{A}\int\frac{Z_{A}}{\left\vert{\bf r}-{\bf R}_{A}\right\vert}\rho({\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} + \frac{1}{2}\sum_{A\ne B}\frac{Z_{A}Z_{B}}{\left\vert{\bf R}_{A}-{\bf R}_{B}\right\vert}
E_{\rm tot} = -\frac{1}{2}\sum_{i}\int\psi_{i}^{*}({\bf r})\nabla^{2}\psi_{i}({\bf r})d^{3}r - \sum_{A}\int\frac{Z_{A}}{\left\vert{\bf r}-{\bf R}_{A}\right\vert}\rho({\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} + \frac{1}{2}\sum_{A\ne B}\frac{Z_{A}Z_{B}}{\left\vert{\bf R}_{A}-{\bf R}_{B}\right\vert}
</math>
</math>
where the terms on the right-hand side represent the non-interacting kinetic energy of the electrons, the electrons-nuclei attraction energy, the classical Coulomb electron-electron repulsive energy, the exchange-correlation energy and the nuclei-nuclei repulsion energy. The orbitals <math>\psi_{i}</math> and the electron density <math>\rho=\sum_{i}\left\vert\psi_{i}\right\vert^{2}</math> are calculated by solving the KS equations
where the terms on the right-hand side represent the non-interacting kinetic energy of the electrons, the electrons-nuclei attraction energy, the classical Coulomb electron-electron repulsive energy, the exchange-correlation energy and the nuclei-nuclei repulsion energy. The orbitals <math>\psi_{i}</math> and the electron density <math>\rho=\sum_{i}\left\vert\psi_{i}\right\vert^{2}</math> that are used to evaluate <math>E_{\rm tot}</math> are obtained by solving self-consistently the KS equations
:<math>
:<math>
\left(-\frac{1}{2}\nabla^{2} -\sum_{A}\frac{Z_{A}}{\left\vert{\bf r}-{\bf R}_{A}\right\vert} + \int\frac{\rho({\bf r'})}{\left\vert{\bf r}-{\bf r'}\right\vert}d^{3}r' + v_{\rm xc}({\bf r})\right)\psi_{i}({\bf r}) = \epsilon_{i}\psi_{i}({\bf r})
\left(-\frac{1}{2}\nabla^{2} -\sum_{A}\frac{Z_{A}}{\left\vert{\bf r}-{\bf R}_{A}\right\vert} + \int\frac{\rho({\bf r'})}{\left\vert{\bf r}-{\bf r'}\right\vert}d^{3}r' + v_{\rm xc}({\bf r})\right)\psi_{i}({\bf r}) = \epsilon_{i}\psi_{i}({\bf r})
</math>
</math>
The only term in <math>E_{\rm tot}</math> and in the KS equations that is not know exactly is the exchange-correlation energy <math>E_{\rm xc}</math> and potential <math>v_{\rm xc}=\delta E_{\rm xc}\delta\rho</math>
In the KS-DFT method, the accuracy of the calculated properties depends mainly on the approximations used


== Theoretical Background ==
== Theoretical Background ==

Revision as of 13:37, 18 January 2022

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

where the terms on the right-hand side represent the non-interacting kinetic energy of the electrons, the electrons-nuclei attraction energy, the classical Coulomb electron-electron repulsive energy, the exchange-correlation energy and the nuclei-nuclei repulsion energy. The orbitals and the electron density that are used to evaluate are obtained by solving self-consistently the KS equations

The only term in and in the KS equations that is not know exactly is the exchange-correlation energy and potential In the KS-DFT method, the accuracy of the calculated properties depends mainly on the approximations used

Theoretical Background

How to


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