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Revision 2613 by chrisfen, Tue Mar 14 13:52:06 2006 UTC vs.
Revision 2615 by chrisfen, Tue Mar 14 14:17:07 2006 UTC

# Line 334 | Line 334 | where $S(r)$ is a switching function that smoothly zer
334   \begin{figure}
335   \centering
336   \includegraphics[width = 3.25in]{./comboSquare.pdf}
337 < \caption{Normal modes for an NaCl crystal at 1000 K when using SPME and a simple damped Coulombic sum with damping coefficients ($\alpha$)ranging from 0.15 to 0.3 \AA$^{-1}$.  As $\alpha$ increases, the peaks are red-shifted toward and eventually beyond the values given by SPME.  The larger $\alpha$ values weaken the real-space electrostatics, explaining this shift towards less strongly correlated motions in the crystal.}
337 > \caption{Upper: Zoomed inset from figure \ref{fig:methodPS}.  As the damping value for the Shifted-Force potential increases, the low-frequency peaks red-shift.  Lower: Low-frequency correlated motions for NaCl crystals at 1000 K when using SPME and a simple damped Coulombic sum with damping coefficients ($\alpha$) ranging from 0.15 to 0.3 \AA$^{-1}$.  As $\alpha$ increases, the peaks are red-shifted toward and eventually beyond the values given by SPME.  The larger $\alpha$ values weaken the real-space electrostatics, explaining this shift towards less strongly correlated motions in the crystal.}
338   \label{fig:dampInc}
339   \end{figure}
340  

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