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Update pseudo documentation

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Anthony Scemama 2023-03-28 10:40:49 +02:00
parent bd7374ebe3
commit 1adaec0da0

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@ -386,20 +386,22 @@ prim_factor =
\[ \[
V_A^{\text{ECP}} = V_A^{\text{ECP}} =
V_{A \ell_{\max}+1} + V_{A \ell_{\max}+1} +
\sum_{\ell=0}^{\ell_{\max}} V_{A \ell} \sum_{\ell=0}^{\ell_{\max}}
\sum_{m=-\ell}^{\ell} | Y_{\ell m} \rangle \langle Y_{\ell m} | \delta V_{A \ell}\sum_{m=-\ell}^{\ell} | Y_{\ell m} \rangle \langle Y_{\ell m} |
\] \]
The first term in the equation above is sometimes attributed to the local channel, The first term in this equation is attributed to the local channel, while
while the remaining terms correspond to the non-local channel projections. the remaining terms correspond to non-local channel projections. $\ell_{\max}$
refers to the maximum angular momentum in the non-local component of the ECP.
All the functions $V_{A\ell}$ are parameterized as: The functions \(\delta V_{A \ell}\) and \(V_{A \ell_{\max}+1}\) are parameterized as:
\[ \begin{eqnarray}
V_{A \ell}(\mathbf{r}) = \delta V_{A \ell}(\mathbf{r}) &=&
\sum_{q=1}^{N_{q \ell}} \sum_{q=1}^{N_{q \ell}}
\beta_{A q \ell}\, |\mathbf{r}-\mathbf{R}_{A}|^{n_{A q \ell}}\, \beta_{A q \ell}\, |\mathbf{r}-\mathbf{R}_{A}|^{n_{A q \ell}}\,
e^{-\alpha_{A q \ell} |\mathbf{r}-\mathbf{R}_{A}|^2 } e^{-\alpha_{A q \ell} |\mathbf{r}-\mathbf{R}_{A}|^2 } \nonumber\\
\]. V_{A \ell_{\max}+1}(\mathbf{r}) &=& -\frac{Z_\text{eff}}{|\mathbf{r}-\mathbf{R}_{A}|}+\delta V_{A \ell_{\max}+1}(\mathbf{r})
\end{eqnarray}
where $Z_\text{eff}$ is the effective nuclear charge of the center.
See http://dx.doi.org/10.1063/1.4984046 or https://doi.org/10.1063/1.5121006 for more info. See http://dx.doi.org/10.1063/1.4984046 or https://doi.org/10.1063/1.5121006 for more info.