Unverified Commit b25f7810 authored by Axel Kohlmeyer's avatar Axel Kohlmeyer
Browse files

convert docs for more fixes

parent fd8cd6fa
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doc/src/Eqs/fix_nh1.jpg

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doc/src/Eqs/fix_nh1.tex

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\documentclass[24pt]{article}

\pagestyle{empty}
\Huge

\begin{document}

\mathchardef\mhyphen="2D

% The imaginary unit
\providecommand*{\iu}%
	{\ensuremath{{\rm i}}}


\begin{eqnarray*}
\exp \left(\iu{} L \Delta t \right) &=&
\exp \left(\iu{} L_{\rm T\mhyphen baro} \frac{\Delta t}{2} \right)
\exp \left(\iu{} L_{\rm T\mhyphen part} \frac{\Delta t}{2} \right)
\exp \left(\iu{} L_{\epsilon , 2} \frac{\Delta t}{2} \right)
\exp \left(\iu{} L_{2}^{(2)} \frac{\Delta t}{2} \right) \\
&&\times \left[ 
\exp \left(\iu{} L_{2}^{(1)} \frac{\Delta t}{2n} \right)
\exp \left(\iu{} L_{\epsilon , 1} \frac{\Delta t}{2n} \right)
\exp \left(\iu{} L_1 \frac{\Delta t}{n} \right)
\exp \left(\iu{} L_{\epsilon , 1} \frac{\Delta t}{2n} \right)
\exp \left(\iu{} L_{2}^{(1)} \frac{\Delta t}{2n} \right)
\right]^n \\
&&\times
\exp \left(\iu{} L_{2}^{(2)} \frac{\Delta t}{2} \right)
\exp \left(\iu{} L_{\epsilon , 2} \frac{\Delta t}{2} \right) 
\exp \left(\iu{} L_{\rm T\mhyphen part} \frac{\Delta t}{2} \right) 
\exp \left(\iu{} L_{\rm T\mhyphen baro} \frac{\Delta t}{2} \right) \\
&&+ \mathcal{O} \left(\Delta t^3 \right)
\end{eqnarray*}

\end{document}

doc/src/Eqs/fix_orient_fcc.jpg

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doc/src/Eqs/fix_orient_fcc.tex

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\newcommand{\br}{\mathbf{r}}

\documentclass[12pt]{article}

\begin{document}

\begin{equation}
  \xi_{i} = \sum_{j=1}^{12} \left| \br_{j} - \br_{j}^{\rm I} \right|
\end{equation}

\begin{equation}
  \xi_{\rm IJ} = \sum_{j=1}^{12} \left| \br_{j}^{\rm J} - \br_{j}^{\rm I} \right|
\end{equation}

\begin{eqnarray}
  \xi_{\rm low} &=& {\rm cutlo} \, \xi_{\rm IJ}  \\
  \xi_{\rm high} &=& {\rm cuthi} \, \xi_{\rm IJ}
\end{eqnarray}

\begin{eqnarray}
  \omega_{i} &=& \frac{\pi}{2} 
       \frac{\xi_{i} - \xi_{\rm low}}{\xi_{\rm high} - \xi_{\rm low}} \\
      \mbox{\hspace*{72pt}}  \nonumber \\
  u_{i} &=& 0 \mbox{\hspace{84pt} for } \xi_{i} < \xi_{\rm low}  \nonumber \\
        &=& {\rm dE}\,\frac{1 - \cos(2 \omega_{i})}{2}
              \mbox{\hspace{10pt}  for } \xi_{\rm low} < \xi_{i} < \xi_{\rm high}  \\
        &=& {\rm dE} \mbox{\hspace{80pt} for } \xi_{\rm high} < \xi_{i}
                                                                \nonumber
\end{eqnarray}
\end{document}
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