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documentation:standard_operators:coulomb_repulsion [2017/02/27 12:42] – Maurits W. Haverkort | documentation:standard_operators:coulomb_repulsion [2017/02/27 12:43] – Maurits W. Haverkort | ||
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===== Two shells, shell occupation conserving ===== | ===== Two shells, shell occupation conserving ===== | ||
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- | The Coulomb repulsion between two shells which does not change the number of electrons is given by a direct term ($l_1=l_3$ and $l_2=l_4$) and an indirect or exchange term ($l_1=l_4$ and $l_2=l_3$). The direct term is given by the Slater integrals: | + | {{: |
\begin{equation} | \begin{equation} | ||
F^{(k)}=e^2\int_0^{\infty}\int_0^{\infty}\frac{\mathrm{Min}[r_i, | F^{(k)}=e^2\int_0^{\infty}\int_0^{\infty}\frac{\mathrm{Min}[r_i, | ||
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===== General case of 4 different shells ===== | ===== General case of 4 different shells ===== | ||
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