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Revision 2882 by tim, Fri Jun 23 21:33:52 2006 UTC vs.
Revision 2888 by tim, Mon Jun 26 13:34:46 2006 UTC

# Line 43 | Line 43 | Fig.~\ref{LCFig:SMCP}).
43   \begin{figure}
44   \centering
45   \includegraphics[width=\linewidth]{smcp.eps}
46 < \caption[]
47 < {}
46 > \caption[SmCP Phase Packing] {Four possible SmCP phase packings that
47 > are characterized by the relative tilt direction(A and S refer an
48 > anticlinic tilt or a synclinic ) and the polarization orientation (A
49 > and F represent antiferroelectric or ferroelectric polar order).}
50   \label{LCFig:SMCP}
51   \end{figure}
52  
# Line 181 | Line 183 | ratio between \textit{end-to-end} well depth $\epsilon
183   \begin{figure}
184   \centering
185   \includegraphics[width=\linewidth]{banana.eps}
186 < \caption[]{} \label{LCFig:BananaMolecule}
186 > \caption[Schematic representation of a typical banana shaped
187 > molecule]{Schematic representation of a typical banana shaped
188 > molecule.} \label{LCFig:BananaMolecule}
189   \end{figure}
190  
191   %\begin{figure}
# Line 271 | Line 275 | scatting\cite{Blum1971}. Latterly, expansion of the or
275   As a useful set of correlation functions to describe
276   position-orientation correlation, rotation invariants were first
277   applied in a spherical symmetric system to study x-ray and light
278 < scatting\cite{Blum1971}. Latterly, expansion of the orientation pair
278 > scatting\cite{Blum1972}. Latterly, expansion of the orientation pair
279   correlation in terms of rotation invariant for molecules of
280   arbitrary shape was introduce by Stone\cite{Stone1978} and adopted
281 < by other researchers in liquid crystal studies\cite{Berardi2000}.
281 > by other researchers in liquid crystal studies\cite{Berardi2003}.
282  
283   \begin{eqnarray}
284   S_{22}^{220} (r) & = & \frac{1}{{4\sqrt 5 }} \left< \delta (r -

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