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Comparing trunk/multipole/multipole1.tex (file contents):
Revision 4183 by gezelter, Sat Jun 14 15:24:30 2014 UTC vs.
Revision 4189 by gezelter, Mon Jun 16 12:33:42 2014 UTC

# Line 233 | Line 233 | forces and torques go smoothly to zero at the cutoff d
233   forces and torques go smoothly to zero at the cutoff distance.
234  
235   \begin{figure}
236 < \includegraphics[width=3in]{SM}
236 > \includegraphics[width=3in]{SM.eps}
237   \caption{Reversed multipoles are projected onto the surface of the
238    cutoff sphere. The forces, torques, and potential are then smoothly
239    shifted to zero as the sites leave the cutoff region.}
# Line 1459 | Line 1459 | $10^9$) are given in the supplemental information.
1459   $10^9$) are given in the supplemental information.
1460  
1461   \begin{figure}
1462 < \includegraphics[width=\linewidth]{Dipoles_rCutNew.pdf}
1462 > \includegraphics[width=\linewidth]{Dipoles_rCutNew.eps}
1463   \caption{Convergence of the lattice energy constants as a function of
1464    cutoff radius (normalized by the lattice constant, $a$) for the new
1465    real-space methods.  Three dipolar crystal structures were sampled,
# Line 1471 | Line 1471 | $10^9$) are given in the supplemental information.
1471   \end{figure}
1472  
1473   \begin{figure}
1474 < \includegraphics[width=\linewidth]{Dipoles_alphaNew.pdf}
1474 > \includegraphics[width=\linewidth]{Dipoles_alphaNew.eps}
1475   \caption{Convergence to the lattice energy constants as a function of
1476    the reduced damping parameter ($\alpha^* = \alpha a$) for the
1477    different real-space methods in the same three dipolar crystals in
# Line 1530 | Line 1530 | Figs.~\ref{fig:Quadrupoles_rCut} and \ref{fig:Quadrupo
1530   Figs.~\ref{fig:Quadrupoles_rCut} and \ref{fig:Quadrupoles_alpha}.
1531  
1532   \begin{figure}
1533 < \includegraphics[width=\linewidth]{Quadrupoles_rcutConvergence.pdf}
1533 > \includegraphics[width=\linewidth]{Quadrupoles_rcutConvergence.eps}
1534   \caption{Convergence of the lattice energy constants as a function of
1535    cutoff radius (normalized by the lattice constant, $a$) for the new
1536    real-space methods.  Three quadrupolar crystal structures were
# Line 1542 | Line 1542 | Figs.~\ref{fig:Quadrupoles_rCut} and \ref{fig:Quadrupo
1542   \end{figure}
1543  
1544  
1545 < \begin{figure}[!htbp]  
1546 < \includegraphics[width=\linewidth]{Quadrupoles_newAlpha.pdf}
1545 > \begin{figure}
1546 > \includegraphics[width=\linewidth]{Quadrupoles_newAlpha.eps}
1547   \caption{Convergence to the lattice energy constants as a function of
1548    the reduced damping parameter ($\alpha^* = \alpha a$) for the
1549    different real-space methods in the same three quadrupolar crystals

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