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More caption cleanup
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paper/basic_training.tex

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@@ -1063,13 +1063,13 @@ \subsubsection{ Ewald Summation}
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\end{figure}
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Unlike the original, full potential, the direct space screened interaction (Figure~\ref{fig:screening}, top) decays rapidly (Figure~\ref{fig:charges_ewald}).
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In fact, it decays even faster than Van der Waals interactions ($1/r^{6}$) and hence relative short cutoffs, comparable to those used for Van der Waals interactions, can be used for handling direct-space Coulomb interactions.
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In fact, it decays even faster than van der Waals interactions ($1/r^{6}$) and hence relative short cutoffs, comparable to those used for van der Waals interactions, can be used for handling direct-space Coulomb interactions.
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\begin{figure}[h]
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\centering
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\includegraphics[width=\linewidth]{decay_comparison.pdf}
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\caption{Comparison of decay of original $r^{-1}$ term(blue,*), erfc(r) in direct space(black,-) and $r^{-6}$ in van der waals term (red, -.). }
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\caption{Comparison of decay of the original $r^{-1}$ term for Coulomb interactions (blue,*), the resulting direct-space term after Gaussian screening (black,-) and the $r^{-6}$ in van der Waals term (red, -.). }
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\label{decay}
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\end{figure}
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