| 2 |
|
|
| 3 |
|
\section{\label{liquidCrystalSection:introduction}Introduction} |
| 4 |
|
|
| 5 |
< |
Long range orientational order is one of the most fundamental |
| 6 |
< |
properties of liquid crystal mesophases. This orientational |
| 7 |
< |
anisotropy of the macroscopic phases originates in the shape |
| 8 |
< |
anisotropy of the constituent molecules. Among these anisotropy |
| 9 |
< |
mesogens, rod-like (calamitic) and disk-like molecules have been |
| 10 |
< |
exploited in great detail in the last two decades. Typically, these |
| 11 |
< |
mesogens consist of a rigid aromatic core and one or more attached |
| 12 |
< |
aliphatic chains. For short chain molecules, only nematic phases, in |
| 13 |
< |
which positional order is limited or absent, can be observed, |
| 14 |
< |
because the entropy of mixing different parts of the mesogens is |
| 15 |
< |
paramount to the dispersion interaction. In contrast, formation of |
| 16 |
< |
the one dimension lamellar sematic phase in rod-like molecules with |
| 17 |
< |
sufficiently long aliphatic chains has been reported, as well as the |
| 18 |
< |
segregation phenomena in disk-like molecules. |
| 5 |
> |
Rod-like (calamitic) and disk-like anisotropy liquid crystals have |
| 6 |
> |
been investigated in great detail in the last two |
| 7 |
> |
decades\cite{Huh2004}. Typically, these mesogens consist of a rigid |
| 8 |
> |
aromatic core and one or more attached aliphatic chains. For short |
| 9 |
> |
chain molecules, only nematic phases, in which positional order is |
| 10 |
> |
limited or absent, can be observed, because the entropy of mixing |
| 11 |
> |
different parts of the mesogens is larger than the dispersion |
| 12 |
> |
interaction. In contrast, formation of one dimension lamellar |
| 13 |
> |
smectic phase in rod-like molecules with sufficiently long aliphatic |
| 14 |
> |
chains has been reported, as well as the segregation phenomena in |
| 15 |
> |
disk-like molecules\cite{McMillan1971}. Recently, banana-shaped or |
| 16 |
> |
bent-core liquid crystals have became one of the most active |
| 17 |
> |
research areas in mesogenic materials and supramolecular |
| 18 |
> |
chemistry\cite{Niori1996, Link1997, Pelzl1999}. Unlike rods and |
| 19 |
> |
disks, the polarity and biaxiality of the banana-shaped molecules |
| 20 |
> |
allow the molecules organize into a variety of novel liquid |
| 21 |
> |
crystalline phases which show interesting material properties. Of |
| 22 |
> |
particular interest is the spontaneous formation of macroscopic |
| 23 |
> |
chiral layers from achiral banana-shaped molecules, where polar |
| 24 |
> |
molecule orientational ordering exhibited layered plane as well as |
| 25 |
> |
the tilted arrangement of the molecules relative to the polar axis. |
| 26 |
> |
As a consequence of supramolecular chirality, the spontaneous |
| 27 |
> |
polarization arises in ferroelectric (FE) and antiferroelectic (AF) |
| 28 |
> |
switching of smectic liquid crystal phases, demonstrating some |
| 29 |
> |
promising applications in second-order nonlinear optical devices. |
| 30 |
> |
The most widely investigated mesophase formed by banana-shaped |
| 31 |
> |
moleculed is the $\text{B}_2$ phase, which is also referred to as |
| 32 |
> |
$\text{SmCP}$\cite{Link1997}. Of the most important discoveries in |
| 33 |
> |
this tilt lamellar phase is the four distinct packing arrangements |
| 34 |
> |
(two conglomerates and two macroscopic racemates), which depend on |
| 35 |
> |
the tilt direction and the polar direction of the molecule in |
| 36 |
> |
adjacent layer (see Fig.~\ref{LCFig:SMCP})\cite{Link1997}. |
| 37 |
|
|
| 20 |
– |
Recently, the banana-shaped or bent-core liquid crystal have became |
| 21 |
– |
one of the most active research areas in mesogenic materials and |
| 22 |
– |
supramolecular chemistry. Unlike rods and disks, the polarity and |
| 23 |
– |
biaxiality of the banana-shaped molecules allow the molecules |
| 24 |
– |
organize into a variety of novel liquid crystalline phases which |
| 25 |
– |
show interesting material properties. Of particular interest is the |
| 26 |
– |
spontaneous formation of macroscopic chiral layers from achiral |
| 27 |
– |
banana-shaped molecules, where polar molecule orientational ordering |
| 28 |
– |
is shown within the layer plane as well as the tilted arrangement of |
| 29 |
– |
the molecules relative to the polar axis. As a consequence of |
| 30 |
– |
supramolecular chirality, the spontaneous polarization arises in |
| 31 |
– |
ferroelectric (FE) and antiferroelectic (AF) switching of smectic |
| 32 |
– |
liquid crystal phases, demonstrating some promising applications in |
| 33 |
– |
second-order nonlinear optical devices. The most widely investigated |
| 34 |
– |
mesophase formed by banana-shaped moleculed is the $\text{B}_2$ |
| 35 |
– |
phase, which is also referred to as $\text{SmCP}$. Of the most |
| 36 |
– |
important discover in this tilt lamellar phase is the four distinct |
| 37 |
– |
packing arrangements (two conglomerates and two macroscopic |
| 38 |
– |
racemates), which depend on the tilt direction and the polar |
| 39 |
– |
direction of the molecule in adjacent layer (see |
| 40 |
– |
Fig.~\cite{LCFig:SMCP}). |
| 41 |
– |
|
| 38 |
|
\begin{figure} |
| 39 |
|
\centering |
| 40 |
|
\includegraphics[width=\linewidth]{smcp.eps} |
| 41 |
< |
\caption[] |
| 42 |
< |
{} |
| 41 |
> |
\caption[SmCP Phase Packing] {Four possible SmCP phase packings that |
| 42 |
> |
are characterized by the relative tilt direction(A and S refer an |
| 43 |
> |
anticlinic tilt or a synclinic ) and the polarization orientation (A |
| 44 |
> |
and F represent antiferroelectric or ferroelectric polar order).} |
| 45 |
|
\label{LCFig:SMCP} |
| 46 |
|
\end{figure} |
| 47 |
|
|
| 48 |
|
Many liquid crystal synthesis experiments suggest that the |
| 49 |
|
occurrence of polarity and chirality strongly relies on the |
| 50 |
< |
molecular structure and intermolecular interaction. From a |
| 51 |
< |
theoretical point of view, it is of fundamental interest to study |
| 52 |
< |
the structural properties of liquid crystal phases formed by |
| 50 |
> |
molecular structure and intermolecular interaction\cite{Reddy2006}. |
| 51 |
> |
From a theoretical point of view, it is of fundamental interest to |
| 52 |
> |
study the structural properties of liquid crystal phases formed by |
| 53 |
|
banana-shaped molecules and understand their connection to the |
| 54 |
|
molecular structure, especially with respect to the spontaneous |
| 55 |
|
achiral symmetry breaking. As a complementary tool to experiment, |
| 60 |
|
smectic arrangements\cite{Cook2000, Lansac2001}, as well as other |
| 61 |
|
bulk properties, such as rotational viscosity and flexoelectric |
| 62 |
|
coefficients\cite{Cheung2002, Cheung2004}. However, due to the |
| 63 |
< |
limitation of time scale required for phase |
| 64 |
< |
transition\cite{Wilson1999} and the length scale required for |
| 65 |
< |
representing bulk behavior, the dominant models in the field of |
| 66 |
< |
liquid crystal phase behavior are generic |
| 67 |
< |
models\cite{Lebwohl1972,Perram1984, Gay1981}, which are based on the |
| 68 |
< |
observation that liquid crystal order is exhibited by a range of |
| 69 |
< |
non-molecular bodies with high shape anisotropies. Previous |
| 70 |
< |
simulation studies using hard spherocylinder dimer |
| 71 |
< |
model\cite{Camp1999} produce nematic phases, while hard rod |
| 72 |
< |
simulation studies identified a Landau point\cite{Bates2005}, at |
| 73 |
< |
which the isotropic phase undergoes a direct transition to the |
| 74 |
< |
biaxial nematic, as well as some possible liquid crystal |
| 75 |
< |
phases\cite{Lansac2003}. Other anisotropic models using |
| 78 |
< |
Gay-Berne(GB) potential, which produce interactions that favor local |
| 79 |
< |
alignment, give the evidence of the novel packing arrangements of |
| 80 |
< |
bent-core molecules\cite{Memmer2002,Orlandi2006}. |
| 63 |
> |
limitation of time scales required for phase transition and the |
| 64 |
> |
length scale required for representing bulk behavior, |
| 65 |
> |
models\cite{Perram1985, Gay1981}, which are based on the observation |
| 66 |
> |
that liquid crystal order is exhibited by a range of non-molecular |
| 67 |
> |
bodies with high shape anisotropies, have become the dominant models |
| 68 |
> |
in the field of liquid crystal phase behavior. Previous simulation |
| 69 |
> |
studies using a hard spherocylinder dimer model\cite{Camp1999} |
| 70 |
> |
produced nematic phases, while hard rod simulation studies |
| 71 |
> |
identified a direct transition to the biaxial nematic and other |
| 72 |
> |
possible liquid crystal phases\cite{Lansac2003}. Other anisotropic |
| 73 |
> |
models using the Gay-Berne(GB) potential, which produces |
| 74 |
> |
interactions that favor local alignment, give evidence of the novel |
| 75 |
> |
packing arrangements of bent-core molecules\cite{Memmer2002}. |
| 76 |
|
|
| 77 |
|
Experimental studies by Levelut {\it et al.}~\cite{Levelut1981} |
| 78 |
|
revealed that terminal cyano or nitro groups usually induce |
| 79 |
|
permanent longitudinal dipole moments, which affect the phase |
| 80 |
< |
behavior considerably. A series of theoretical studies also drawn |
| 81 |
< |
equivalent conclusions. Monte Carlo studies of the GB potential with |
| 82 |
< |
fixed longitudinal dipoles (i.e. pointed along the principal axis of |
| 83 |
< |
rotation) were shown to enhance smectic phase |
| 80 |
> |
behavior considerably. Equivalent conclusions have also been drawn |
| 81 |
> |
from a series of theoretical studies. Monte Carlo studies of the GB |
| 82 |
> |
potential with fixed longitudinal dipoles (i.e. pointed along the |
| 83 |
> |
principal axis of rotation) were shown to enhance smectic phase |
| 84 |
|
stability~\cite{Berardi1996,Satoh1996}. Molecular simulation of GB |
| 85 |
|
ellipsoids with transverse dipoles at the terminus of the molecule |
| 86 |
|
also demonstrated that partial striped bilayer structures were |
| 93 |
|
bent-core molecules, could be modeled more accurately by |
| 94 |
|
incorporating electrostatic interaction. |
| 95 |
|
|
| 96 |
< |
In this chapter, we consider system consisting of banana-shaped |
| 97 |
< |
molecule represented by three rigid GB particles with one or two |
| 98 |
< |
point dipoles at different location. Performing a series of |
| 99 |
< |
molecular dynamics simulations, we explore the structural properties |
| 100 |
< |
of tilted smectic phases as well as the effect of electrostatic |
| 106 |
< |
interactions. |
| 96 |
> |
In this chapter, we consider a system consisting of banana-shaped |
| 97 |
> |
molecule represented by three rigid GB particles with two point |
| 98 |
> |
dipoles. Performing a series of molecular dynamics simulations, we |
| 99 |
> |
explore the structural properties of tilted smectic phases as well |
| 100 |
> |
as the effect of electrostatic interactions. |
| 101 |
|
|
| 102 |
|
\section{\label{liquidCrystalSection:model}Model} |
| 103 |
|
|
| 110 |
|
potential used to mimic the apolar characteristics of liquid crystal |
| 111 |
|
molecules takes the familiar form of Lennard-Jones function with |
| 112 |
|
orientation and position dependent range ($\sigma$) and well depth |
| 113 |
< |
($\epsilon$) parameters. It can can be expressed as, |
| 113 |
> |
($\epsilon$) parameters. The potential between a pair of three-site |
| 114 |
> |
banana-shaped molecules $a$ and $b$ is given by |
| 115 |
|
\begin{equation} |
| 116 |
+ |
V_{ab}^{GB} = \sum\limits_{i \in a,j \in b} {V_{ij}^{GB} }. |
| 117 |
+ |
\end{equation} |
| 118 |
+ |
Every site-site interaction can can be expressed as, |
| 119 |
+ |
\begin{equation} |
| 120 |
|
V_{ij}^{GB} = 4\epsilon (\hat u_i ,\hat u_j ,\hat r_{ij} )\left[ |
| 121 |
|
{\left( {\frac{{\sigma _0 }}{{r_{ij} - \sigma (\hat u_i ,\hat u_j |
| 122 |
|
,\hat r_{ij} )}}} \right)^{12} - \left( {\frac{{\sigma _0 |
| 124 |
|
} \right] \label{LCEquation:gb} |
| 125 |
|
\end{equation} |
| 126 |
|
where $\hat u_i,\hat u_j$ are unit vectors specifying the |
| 127 |
< |
orientation of two molecules $i$ and $j$ separated by intermolecular |
| 128 |
< |
vector $r_{ij}$. $\hat r_{ij}$ is the unit vector along the |
| 129 |
< |
intermolecular vector. A schematic diagram of the orientation |
| 130 |
< |
vectors is shown in Fig.\ref{LCFigure:GBScheme}. The functional form |
| 131 |
< |
for $\sigma$ is given by |
| 127 |
> |
orientation of two ellipsoids $i$ and $j$ separated by |
| 128 |
> |
intermolecular vector $r_{ij}$. $\hat r_{ij}$ is the unit vector |
| 129 |
> |
along the inter-ellipsoid vector. A schematic diagram of the |
| 130 |
> |
orientation vectors is shown in Fig.\ref{LCFigure:GBScheme}. The |
| 131 |
> |
functional form for $\sigma$ is given by |
| 132 |
|
\begin{equation} |
| 133 |
|
\sigma (\hat u_i ,\hat u_i ,\hat r_{ij} ) = \sigma _0 \left[ {1 - |
| 134 |
|
\frac{\chi }{2}\left( {\frac{{(\hat r_{ij} \cdot \hat u_i + \hat |
| 145 |
|
\label{LCEquation:chi} |
| 146 |
|
\end{equation} |
| 147 |
|
Here, $\sigma_ s$ and $\sigma_{e}$ refer to the side-by-side breadth |
| 148 |
< |
and the end-to-end length of the ellipsoid, respectively. Twell |
| 148 |
> |
and the end-to-end length of the ellipsoid, respectively. The well |
| 149 |
|
depth parameters takes the form |
| 150 |
|
\begin{equation} |
| 151 |
|
\epsilon (\hat u_i ,\hat u_j ,\hat r_{ij} ) = \epsilon _0 \epsilon |
| 168 |
|
where the well depth anisotropy parameter $\chi '$ depends on the |
| 169 |
|
ratio between \textit{end-to-end} well depth $\epsilon _e$ and |
| 170 |
|
\textit{side-by-side} well depth $\epsilon_s$, |
| 171 |
< |
\begin{eqaution} |
| 171 |
> |
\begin{equation} |
| 172 |
|
\chi ' = \frac{{1 - (\epsilon _e /\epsilon _s )^{1/\mu} }}{{1 + |
| 173 |
|
(\epsilon _e /\epsilon _s )^{1/\mu} }}. |
| 174 |
|
\end{equation} |
| 176 |
|
\begin{figure} |
| 177 |
|
\centering |
| 178 |
|
\includegraphics[width=\linewidth]{banana.eps} |
| 179 |
< |
\caption[]{} \label{LCFig:BananaMolecule} |
| 179 |
> |
\caption[Schematic representation of a typical banana shaped |
| 180 |
> |
molecule]{Schematic representation of a typical banana shaped |
| 181 |
> |
molecule.} \label{LCFig:BananaMolecule} |
| 182 |
|
\end{figure} |
| 183 |
+ |
\begin{figure} |
| 184 |
+ |
\centering |
| 185 |
+ |
\includegraphics[width=\linewidth]{gb_scheme.eps} |
| 186 |
+ |
\caption[Schematic diagram showing definitions of the orientation |
| 187 |
+ |
vectors for a pair of Gay-Berne molecules]{Schematic diagram showing |
| 188 |
+ |
definitions of the orientation vectors for a pair of Gay-Berne |
| 189 |
+ |
ellipsoids} \label{LCFigure:GBScheme} |
| 190 |
+ |
\end{figure} |
| 191 |
+ |
To account for the permanent dipolar interactions, there should be |
| 192 |
+ |
an electrostatic interaction term of the form |
| 193 |
+ |
\begin{equation} |
| 194 |
+ |
V_{ab}^{dp} = \sum\limits_{i \in a,j \in b} {\frac{1}{{4\pi |
| 195 |
+ |
\epsilon _{fs} }}\left[ {\frac{{\mu _i \cdot \mu _j }}{{r_{ij}^3 }} |
| 196 |
+ |
- \frac{{3\left( {\mu _i \cdot r_{ij} } \right)\left( {\mu _i \cdot |
| 197 |
+ |
r_{ij} } \right)}}{{r_{ij}^5 }}} \right]} |
| 198 |
+ |
\end{equation} |
| 199 |
+ |
where $\epsilon _{fs}$ is the permittivity of free space. |
| 200 |
|
|
| 201 |
+ |
\section{Results and Discussion} |
| 202 |
+ |
|
| 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 $\mu = 1,~ \nu = 2, |
| 207 |
+ |
~\epsilon_{e}/\epsilon_{s} = 1/5$ and $\sigma_{e}/\sigma_{s} = 3$. |
| 208 |
+ |
All of the simulations begin with same equilibrated isotropic |
| 209 |
+ |
configuration where 1024 molecules without dipoles were confined in |
| 210 |
+ |
a $160\times 160 \times 120$ box. After the dipolar interactions are |
| 211 |
+ |
switched on, 2~ns NPTi cooling run with themostat of 2~ps and |
| 212 |
+ |
barostat of 50~ps were used to equilibrate the system to desired |
| 213 |
+ |
temperature and pressure. NPTi Production runs last for 40~ns with |
| 214 |
+ |
time step of 20~fs. |
| 215 |
+ |
|
| 216 |
+ |
\subsection{Order Parameters} |
| 217 |
+ |
|
| 218 |
+ |
To investigate the phase structure of the model liquid crystal, we |
| 219 |
+ |
calculated various order parameters and correlation functions. |
| 220 |
+ |
Particulary, the $P_2$ order parameter allows us to estimate average |
| 221 |
+ |
alignment along the director axis $Z$ which can be identified from |
| 222 |
+ |
the largest eigenvalue obtained by diagonalizing the order parameter |
| 223 |
+ |
tensor |
| 224 |
+ |
\begin{equation} |
| 225 |
+ |
\overleftrightarrow{\mathsf{Q}} = \frac{1}{N}\sum_i^N % |
| 226 |
+ |
\begin{pmatrix} % |
| 227 |
+ |
u_{ix}u_{ix}-\frac{1}{3} & u_{ix}u_{iy} & u_{ix}u_{iz} \\ |
| 228 |
+ |
u_{iy}u_{ix} & u_{iy}u_{iy}-\frac{1}{3} & u_{iy}u_{iz} \\ |
| 229 |
+ |
u_{iz}u_{ix} & u_{iz}u_{iy} & u_{iz}u_{iz}-\frac{1}{3} % |
| 230 |
+ |
\end{pmatrix}, |
| 231 |
+ |
\label{lipidEq:p2} |
| 232 |
+ |
\end{equation} |
| 233 |
+ |
where the $u_{i\alpha}$ is the $\alpha$ element of the unit vector |
| 234 |
+ |
$\mathbf{\hat{u}}_i$, and the sum over $i$ averages over the whole |
| 235 |
+ |
collection of unit vectors. The $P_2$ order parameter for uniaxial |
| 236 |
+ |
phase is then simply given by |
| 237 |
+ |
\begin{equation} |
| 238 |
+ |
\langle P_2 \rangle = \frac{3}{2}\lambda_{\text{max}}. |
| 239 |
+ |
\label{lipidEq:po3} |
| 240 |
+ |
\end{equation} |
| 241 |
+ |
%In addition to the $P_2$ order parameter, $ R_{2,2}^2$ order |
| 242 |
+ |
%parameter for biaxial phase is introduced to describe the ordering |
| 243 |
+ |
%in the plane orthogonal to the director by |
| 244 |
+ |
%\begin{equation} |
| 245 |
+ |
%R_{2,2}^2 = \frac{1}{4}\left\langle {(x_i \cdot X)^2 - (x_i \cdot |
| 246 |
+ |
%Y)^2 - (y_i \cdot X)^2 + (y_i \cdot Y)^2 } \right\rangle |
| 247 |
+ |
%\end{equation} |
| 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 are |
| 252 |
+ |
summarized in Table~\ref{liquidCrystal:p2} which identifies a phase |
| 253 |
+ |
transition temperature range. |
| 254 |
+ |
|
| 255 |
+ |
\begin{table} |
| 256 |
+ |
\caption{LIQUID CRYSTAL STRUCTURAL PROPERTIES AS A FUNCTION OF |
| 257 |
+ |
TEMPERATURE} \label{liquidCrystal:p2} |
| 258 |
+ |
\begin{center} |
| 259 |
+ |
\begin{tabular}{cccccc} |
| 260 |
+ |
\hline |
| 261 |
+ |
Temperature (K) & 420 & 440 & 460 & 480 & 600\\ |
| 262 |
+ |
\hline |
| 263 |
+ |
$\langle P_2\rangle$ & 0.984 & 0.982 & 0.975 & 0.967 & 0.067\\ |
| 264 |
+ |
\hline |
| 265 |
+ |
\end{tabular} |
| 266 |
+ |
\end{center} |
| 267 |
+ |
\end{table} |
| 268 |
+ |
|
| 269 |
+ |
\subsection{Structural Properties} |
| 270 |
+ |
|
| 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 |
| 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 |
| 278 |
+ |
minimum distance for two in plane banana shaped molecules is 4.9 |
| 279 |
+ |
\AA, while the second split peak implies the biaxial packing. It is |
| 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} |
| 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 $\rm{\AA}$ is attributed to a defect in the |
| 290 |
+ |
system. |
| 291 |
+ |
|
| 292 |
+ |
\subsection{Rotational Invariants} |
| 293 |
+ |
|
| 294 |
+ |
As a useful set of correlation functions to describe |
| 295 |
+ |
position-orientation correlation, rotation invariants were first |
| 296 |
+ |
applied in a spherical symmetric system to study x-ray and light |
| 297 |
+ |
scatting\cite{Blum1972}. Latterly, expansion of the orientation pair |
| 298 |
+ |
correlation in terms of rotation invariant for molecules of |
| 299 |
+ |
arbitrary shape has been introduced by Stone\cite{Stone1978} and |
| 300 |
+ |
adopted by other researchers in liquid crystal |
| 301 |
+ |
studies\cite{Berardi2003}. In order to study the correlation between |
| 302 |
+ |
biaxiality and molecular separation distance $r$, we calculate a |
| 303 |
+ |
rotational invariant function $S_{22}^{220} (r)$, which is given by |
| 304 |
+ |
: |
| 305 |
+ |
\begin{eqnarray} |
| 306 |
+ |
S_{22}^{220} (r) & = & \frac{1}{{4\sqrt 5 }} \left< \delta (r - |
| 307 |
+ |
r_{ij} )((\hat x_i \cdot \hat x_j )^2 - (\hat x_i \cdot \hat y_j |
| 308 |
+ |
)^2 - (\hat y_i \cdot \hat x_j )^2 + (\hat y_i \cdot \hat y_j |
| 309 |
+ |
)^2 ) \right. \notag \\ |
| 310 |
+ |
& & \left. - 2(\hat x_i \cdot \hat y_j )(\hat y_i \cdot \hat x_j ) - |
| 311 |
+ |
2(\hat x_i \cdot \hat x_j )(\hat y_i \cdot \hat y_j )) \right>. |
| 312 |
+ |
\end{eqnarray} |
| 313 |
+ |
The long range behavior of second rank orientational correlation |
| 314 |
+ |
$S_{22}^{220} (r)$ in Fig~\ref{LCFigure:S22220} also confirm the |
| 315 |
+ |
biaxiality of the system. |
| 316 |
+ |
|
| 317 |
|
\begin{figure} |
| 318 |
|
\centering |
| 319 |
< |
\includegraphics[width=\linewidth]{bananGB_grained.eps} |
| 320 |
< |
\caption[]{} \label{LCFigure:BananaGB} |
| 319 |
> |
\includegraphics[width=4.5in]{snapshot.eps} |
| 320 |
> |
\caption[Snapshot of the molecular organization in the layered phase |
| 321 |
> |
formed at temperature T = 460K and pressure P = 1 atm]{Snapshot of |
| 322 |
> |
the molecular organization in the layered phase formed at |
| 323 |
> |
temperature T = 460K and pressure P = 1 atm. (a) diagonal view; (b) |
| 324 |
> |
side view.} \label{LCFigure:snapshot} |
| 325 |
|
\end{figure} |
| 326 |
|
|
| 327 |
|
\begin{figure} |
| 328 |
|
\centering |
| 329 |
< |
\includegraphics[width=\linewidth]{gb_scheme.eps} |
| 330 |
< |
\caption[]{Schematic diagram showing definitions of the orientation |
| 331 |
< |
vectors for a pair of Gay-Berne molecules} |
| 332 |
< |
\label{LCFigure:GBScheme} |
| 329 |
> |
\includegraphics[width=\linewidth]{gofr_gofz.eps} |
| 330 |
> |
\caption[Correlation Functions of a Bent-core Liquid Crystal System |
| 331 |
> |
at Temperature T = 460K and Pressure P = 10 atm]{Correlation |
| 332 |
> |
Functions of a Bent-core Liquid Crystal System at Temperature T = |
| 333 |
> |
460K and Pressure P = 10 atm. (a) radial correlation function |
| 334 |
> |
$g(r)$; and (b) density along the director $g(z)$.} |
| 335 |
> |
\label{LCFigure:gofrz} |
| 336 |
|
\end{figure} |
| 337 |
|
|
| 338 |
< |
\section{\label{liquidCrystalSection:methods}Methods} |
| 338 |
> |
\begin{figure} |
| 339 |
> |
\centering |
| 340 |
> |
\includegraphics[width=\linewidth]{s22_220.eps} |
| 341 |
> |
\caption[Average orientational correlation Correlation Functions of |
| 342 |
> |
a Bent-core Liquid Crystal System at Temperature T = 460K and |
| 343 |
> |
Pressure P = 10 atm]{Average orientational correlation Correlation |
| 344 |
> |
Functions of a Bent-core Liquid Crystal System at Temperature T = |
| 345 |
> |
460K and Pressure P = 10 atm.} \label{LCFigure:S22220} |
| 346 |
> |
\end{figure} |
| 347 |
|
|
| 348 |
< |
\section{\label{liquidCrystalSection:resultDiscussion}Results and Discussion} |
| 348 |
> |
\section{Conclusion} |
| 349 |
> |
|
| 350 |
> |
We have presented a simple dipolar three-site GB model for banana |
| 351 |
> |
shaped molecules which are capable of forming smectic phases from |
| 352 |
> |
isotropic configuration. Various order parameters and correlation |
| 353 |
> |
functions were used to characterized the structural properties of |
| 354 |
> |
these smectic phase. However, the forming layered structure still |
| 355 |
> |
had some defects because of the mismatching between the layer |
| 356 |
> |
structure spacing and the shape of simulation box. This mismatching |
| 357 |
> |
can be broken by using NPTf integrator in further simulations. The |
| 358 |
> |
role of terminal chain in controlling transition temperatures and |
| 359 |
> |
the type of mesophase formed have been studied |
| 360 |
> |
extensively\cite{Pelzl1999}. The lack of flexibility in our model |
| 361 |
> |
due to the missing terminal chains could explain the fact that we |
| 362 |
> |
did not find evidence of chirality. |
