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# Line 200 | Line 200 | A series of molecular dynamics simulations were perfor
200  
201   \section{Results and Discussion}
202  
203 < A series of molecular dynamics simulations were perform to study the
203 > A series of molecular dynamics simulations were performed to study the
204   phase behavior of banana shaped liquid crystals. In each simulation,
205   every banana shaped molecule has been represented by three GB
206   particles which is characterized by $\mu = 1,~ \nu = 2,
# Line 248 | Line 248 | for the bent-core liquid crystal at different temperat
248   %where $X$, $Y$ and $Z$ are axis of the director frame.
249   The unit vector for the banana shaped molecule was defined by the
250   principle aixs of its middle GB particle. The $P_2$ order parameters
251 < for the bent-core liquid crystal at different temperature is
251 > for the bent-core liquid crystal at different temperature are
252   summarized in Table~\ref{liquidCrystal:p2} which identifies a phase
253   transition temperature range.
254  
# Line 271 | Line 271 | stacking of the banana shaped molecules while the side
271   The molecular organization obtained at temperature $T = 460K$ (below
272   transition temperature) is shown in Figure~\ref{LCFigure:snapshot}.
273   The diagonal view in Fig~\ref{LCFigure:snapshot}(a) shows the
274 < stacking of the banana shaped molecules while the side view in n
274 > stacking of the banana shaped molecules while the side view in
275   Figure~\ref{LCFigure:snapshot}(b) demonstrates formation of a
276   chevron structure. The first peak of the radial distribution
277   function $g(r)$ in Fig.~\ref{LCFigure:gofrz}(a) shows that the
# Line 280 | Line 280 | g(z) =\frac{1}{\pi R^{2} \rho}< \delta (z-z_{ij})>_{ij
280   also important to show the density correlation along the director
281   which is given by :
282   \begin{equation}
283 < g(z) =\frac{1}{\pi R^{2} \rho}< \delta (z-z_{ij})>_{ij}
284 < \end{equation},
283 > g(z) =\frac{1}{\pi R^{2} \rho}< \delta (z-z_{ij})>_{ij},
284 > \end{equation}
285   where $ z_{ij}  = r_{ij}  \cdot \hat Z $ was measured in the
286   director frame and $R$ is the radius of the cylindrical sampling
287   region. The oscillation in density plot along the director in
288   Fig.~\ref{LCFigure:gofrz}(b) implies the existence of the layered
289 < structure, and the peak at 27 \AA is attributed to a defect in the
289 > structure, and the peak at 27 $\rm{\AA}$ is attributed to a defect in the
290   system.
291  
292   \subsection{Rotational Invariants}

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