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root/group/trunk/COonPt/COonPtAu.tex
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Revision 3813 by jmichalk, Fri Dec 14 05:35:49 2012 UTC vs.
Revision 3814 by jmichalk, Fri Dec 14 19:19:04 2012 UTC

# Line 213 | Line 213 | mechanical predictions (-2.46 D~\AA)\cite{QuadrupoleCO
213   \hline
214   \multicolumn{5}{|c|}{\textbf{Self-Interactions}}\\
215   \hline
216 < &  r & $\sigma$ & $\epsilon$ & q\\
216 > &  {\it z} & $\sigma$ & $\epsilon$ & q\\
217   \hline
218 < \textbf{C} & 0.0 &  0.0262  & 3.83   &   -0.75 \\
219 < \textbf{O} &  1.13 &   0.1591 &   3.12 &   -0.85 \\
220 < \textbf{M} & 0.6457 & -  &  -  &    1.6 \\
218 > \textbf{C} & -0.6457 &  0.0262  & 3.83   &   -0.75 \\
219 > \textbf{O} &  0.4843 &   0.1591 &   3.12 &   -0.85 \\
220 > \textbf{M} & 0.0 & -  &  -  &    1.6 \\
221   \hline
222   \end{tabular}
223   \end{table}
# Line 341 | Line 341 | While an ideal metallic surface is unlikely to experie
341   %Table of Diffusion Constants
342   %Add gold?M
343   \begin{table}[H]
344 < \caption{Platinum diffusion constants parallel and perpendicular to the 557 step edge. As the coverage increases, the diffusion constants parallel and  perpendicular to the step edge both initially increase and then decrease slightly. There were two approaches of analysis. One looking at the surface atoms that had moved more than a prescribed amount over the run time and the other looking at all surface atoms. Units are \AA\textsuperscript{2}/ns}
344 > \caption{Platinum and gold diffusion constants parallel and perpendicular to the 557 step edge. As the coverage increases, the diffusion constants parallel and  perpendicular to the step edge both initially increase and then decrease slightly. Units are \AA\textsuperscript{2}/ns}
345   \centering
346 < \begin{tabular}{| c | ccc | ccc | c |}
346 > \begin{tabular}{| c | cc | cc | c |}
347   \hline
348 < \textbf{System Coverage} & $\mathbf{D}_{\parallel}$ & $\mathbf{D}_{\perp}$ & \textbf{Atoms} & $\mathbf{D}_{\parallel}$ & $\mathbf{D}_{\perp}$ & \textbf{Atoms} & \textbf{Time (ns)}\\
348 > \textbf{System Coverage} & $\mathbf{D}_{\parallel}$ & $\mathbf{D}_{\perp}$ & $\mathbf{D}_{\parallel}$ & $\mathbf{D}_{\perp}$  & \textbf{Time (ns)}\\
349   \hline
350 < &\multicolumn{3}{c|}{\textbf{Mobile}}&\multicolumn{3}{c|}{\textbf{Surface Atoms}} & \\
350 > &\multicolumn{2}{c|}{\textbf{Platinum}}&\multicolumn{2}{c|}{\textbf{Gold}} & \\
351   \hline
352 < 50\% & 3.74 & 0.89 & 497 & 2.05 & 0.49 & 912 & 116 \\
353 < 50\% & 5.81 & 1.59 & 365 & 2.41 & 0.68 & 912 & 46   \\
354 < 33\% & 6.73 & 2.47 & 332 & 2.51 & 0.93 & 912 & 46   \\
355 < 25\% & 5.38 & 2.04 & 361 & 2.18 & 0.84 & 912 & 46  \\
356 < 5\% & 5.54 & 0.63 & 230 & 1.44 & 0.19 & 912 & 46  \\
357 < 0\% & 3.53 & 0.61 & 282 & 1.11 & 0.22 & 912 & 56  \\
358 < \hline
359 < 50\%-r & 6.91 & 2.00 & 198 & 2.23 & 0.68  & 925 & 25\\
360 < 0\%-r  & 4.73 & 0.27 & 128 & 0.72 & 0.05 & 925 & 43\\
352 > 50\% & 4.32 $\pm$ 0.02 & 1.185 $\pm$ 0.008 & 1.72 $\pm$ 0.02 & 0.455 $\pm$ 0.006 & 40 \\
353 > 33\% & 5.18 $\pm$ 0.03 & 1.999 $\pm$ 0.005 & 1.95 $\pm$ 0.02 & 0.337 $\pm$ 0.004 & 40   \\
354 > 25\% & 5.01 $\pm$ 0.02 & 1.574 $\pm$ 0.004 & 1.26 $\pm$ 0.03 & 0.377 $\pm$ 0.006 & 40  \\
355 > 5\%   & 3.61 $\pm$ 0.02 & 0.355 $\pm$ 0.002 & 1.84 $\pm$ 0.03 & 0.169 $\pm$ 0.004 & 40  \\
356 > 0\%   & 3.27 $\pm$ 0.02 & 0.147 $\pm$ 0.004 & 1.50 $\pm$ 0.02 & 0.194 $\pm$ 0.002  & 40  \\
357   \hline
358   \end{tabular}
359   \end{table}

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