X-Git-Url: https://hackdaworld.org/gitweb/?p=lectures%2Flatex.git;a=blobdiff_plain;f=posic%2Ftalks%2Fupb-ua-xc.tex;h=23aff0777d5909a7b080b423d63a0713daa26105;hp=2e8d15b90b5070c2896127c9a3d56245aaf252e0;hb=d6b64d4be7e48f04395e2862f4a53e0f06198e26;hpb=c782b5203ecd1924f4a428b428f301f91cadc828 diff --git a/posic/talks/upb-ua-xc.tex b/posic/talks/upb-ua-xc.tex index 2e8d15b..23aff07 100644 --- a/posic/talks/upb-ua-xc.tex +++ b/posic/talks/upb-ua-xc.tex @@ -1195,7 +1195,8 @@ POTIM = 0.1 fractional & 0.1547 & 0.1676 \\ in \AA & 0.84 & 0.91 \\ \hline - \end{tabular} + \end{tabular}\\[0.2cm] + {\scriptsize\underline{PC (Vasp)}} \includegraphics[width=6.1cm]{c_100_pc_vasp.ps} \end{center} \end{minipage} @@ -1209,7 +1210,8 @@ POTIM = 0.1 Again: C \hkl<1 0 0> interstitial migration (VASP) } - $\hkl<0 0 -1> \rightarrow \hkl<0 0 1>$ migration: + $\hkl<0 0 -1> \rightarrow \hkl<0 0 1>$ migration + ($3\times 3\times 3$ Type 2): \small @@ -1257,7 +1259,8 @@ POTIM = 0.1 Again: C \hkl<1 0 0> interstitial migration (VASP) } - $\hkl<0 0 -1> \rightarrow \hkl<0 -1 0>$ migration: + $\hkl<0 0 -1> \rightarrow \hkl<0 -1 0>$ migration + ($3\times 3\times 3$ Type 2): \small @@ -1286,17 +1289,140 @@ POTIM = 0.1 \Rightarrow \Delta E_{\text{f}} = E_{\text{mig}} = ?.?? \text{ eV} \] - Unexpected \& ({\color{red}more} or {\color{orange}less}) fatal: + \vspace*{0.5cm} + {\large\bf + Intermediate configuration {\color{red}not found} by now! + } + +\end{slide} + +\begin{slide} + + {\large\bf\boldmath + C in Si interstitial configurations (VASP) + } + + Check of Kohn-Sham eigenvalues\\ + + \small + + \begin{minipage}{6cm} + \hkl<1 0 0> interstitial\\ + \end{minipage} + \begin{minipage}{6cm} + Saddle point configuration\\ + \end{minipage} + \underline{$4\times 4\times 3$ Type 1 - fixed border atoms}\\ + \begin{minipage}{6cm} +385: 4.8567 - 2.00000\\ +386: 4.9510 - 2.00000\\ +387: 5.3437 - 0.00000\\ +388: 5.4930 - 0.00000 + \end{minipage} + \begin{minipage}{6cm} +385: 4.8694 - 2.00000\\ +386: {\color{red}4.9917} - 1.92603\\ +387: {\color{red}5.1181} - 0.07397\\ +388: 5.4541 - 0.00000 + \end{minipage}\\[0.2cm] + \underline{$4\times 4\times 3$ Type 1 - no constraints}\\ + \begin{minipage}{6cm} +385: 4.8586 - 2.00000\\ +386: 4.9458 - 2.00000\\ +387: 5.3358 - 0.00000\\ +388: 5.4915 - 0.00000 + \end{minipage} + \begin{minipage}{6cm} +385: 4.8693 - 2.00000\\ +386: {\color{red}4.9879} - 1.92065\\ +387: {\color{red}5.1120} - 0.07935\\ +388: 5.4544 - 0.00000 + \end{minipage}\\[0.2cm] + \underline{$3\times 3\times 3$ Type 2 - no constraints}\\ + \begin{minipage}{6cm} +433: 4.8054 - 2.00000\\ +434: 4.9027 - 2.00000\\ +435: 5.2543 - 0.00000\\ +436: 5.5718 - 0.00000 + \end{minipage} + \begin{minipage}{6cm} +433: 4.8160 - 2.00000\\ +434: {\color{green}5.0109} - 1.00264\\ +435: {\color{green}5.0111} - 0.99736\\ +436: 5.5364 - 0.00000 + \end{minipage} + +\end{slide} + +\begin{slide} + + {\large\bf\boldmath + Once again: C \hkl<1 0 0> interstitial migration (VASP) + } + + Method: \begin{itemize} - \renewcommand\labelitemi{{\color{orange}$\bullet$}} - \item Difference in formation energy (0.02 eV) - of the initial and final configuration - \renewcommand\labelitemi{{\color{red}$\bullet$}} - \item Huge discrepancy (0.3 - 0.4 eV) to the migration barrier - of Type 1 (198+1 atoms) calculations - \renewcommand\labelitemi{{\color{black}$\bullet$}} + \item Start in fully relaxed (assumed) saddle point configuration + \item Move towards \hkl<1 0 0> configuration using updated values + for $\Delta x$, $\Delta y$ and $\Delta z$ + \item \hkl<1 1 0> constraints applied, 1 Si atom fixed + \item $4\times 4\times 3$ Type 1 supercell \end{itemize} - + + Results: + + \begin{minipage}{6.2cm} + \includegraphics[width=6.0cm]{c_100_110sp-i_vasp.ps} + \end{minipage} + \begin{minipage}{6.2cm} + \includegraphics[width=6.0cm]{c_100_110sp-i_rc_vasp.ps} + \end{minipage} + + Reaction coordinate: + $r_{i+1}=r_i+\sum_{\text{atoms j}} \left| r_{j,i+1}-r_{j,i} \right|$ + +\end{slide} + +\begin{slide} + + {\large\bf\boldmath + Investigation of the migration path along \hkl<1 1 0> (VASP) + } + + \small + + \underline{Minimum:}\\ + \begin{minipage}{4cm} + \includegraphics[width=3.5cm]{c_100_mig_vasp/110_c-si_split.eps} + \end{minipage} + \begin{minipage}{8cm} + \begin{itemize} + \item Starting conf: 35 \% displacement results + \item \hkl<1 1 0> constraint disabled + \end{itemize} + \begin{center} + $\Downarrow$ + \end{center} + \begin{itemize} + \item C-Si \hkl<1 1 0> split interstitial + \item Stable configuration + \item $E_{\text{f}}=4.13\text{ eV}$ + \end{itemize} + \end{minipage}\\[0.1cm] + + \underline{Maximum:}\\ + \begin{minipage}{6cm} + \begin{center} + \includegraphics[width=2.3cm]{c_100_mig_vasp/100-110_01.eps} + \includegraphics[width=2.3cm]{c_100_mig_vasp/100-110_02.eps}\\ + 20 \% $\rightarrow$ 25 \%\\ + Breaking of Si-C bond + \end{center} + \end{minipage} + \begin{minipage}{6cm} + \includegraphics[width=6.2cm]{c_100_110sp-i_upd_vasp.ps} + \end{minipage} + \end{slide} \begin{slide} @@ -1305,7 +1431,7 @@ POTIM = 0.1 Molecular dynamics simulations (VASP) } - 2 C atoms in $2\times 2\times 2$ Type 2 supercell + 2 C atoms in $2\times 2\times 2$ Type 2 supercell at $450\,^{\circ}\text{C}$ \small @@ -1336,7 +1462,7 @@ POTIM = 0.1 Molecular dynamics simulations (VASP) } - 10 C atoms in $3\times 3\times 3$ Type 2 supercell + 10 C atoms in $3\times 3\times 3$ Type 2 supercell at $450\,^{\circ}\text{C}$ \small