trunk/5cb/5CB.tex

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\title{Nitrile vibrations as reporters of field-induced phase
  transitions in liquid crystals}  
\author{James M. Marr} 
\author{J. Daniel Gezelter} 
\email{gezelter@nd.edu} 
\affiliation[University of Notre Dame]{251 Nieuwland Science Hall\\ 
Department of Chemistry and Biochemistry\\ 
University of Notre Dame\\ 
Notre Dame, Indiana 46556}

\date{\today}

\begin{document}

\maketitle 

\begin{doublespace}

\begin{abstract}
  The behavior of the spectral lineshape of the nitrile group in
  4-Cyano-4'-pentylbiphenyl (5CB) in response to an applied electric
  field has been simulated using both classical molecular dynamics
  simulations and {\it ab initio} quantum mechanical calculations of
  liquid-like clusters.  This nitrile group is a well-known reporter
  of local field effects in other condensed phase settings, and our
  simulations suggest that there is a significant response when 5CB
  liquids are exposed to a relatively large external field.  However,
  this response is due largely to the field-induced phase transition.
  We observe a peak shift to the red of nearly 40
  cm\textsuperscript{-1}. These results indicate that applied fields
  can play a role in the observed peak shape and position even if
  those fields are significantly weaker than the local electric fields
  that are normally felt within polar liquids.
\end{abstract}

\newpage

\section{Introduction}

The fundamental characteristic of liquid crystal mesophases is that
they maintain some degree of orientational order while translational
order is limited or absent. This orientational order produces a
complex direction-dependent response to external perturbations like
electric fields and mechanical distortions.  The anisotropy of the
macroscopic phases originates in the anisotropy of the constituent
molecules, which typically have highly non-spherical structures with a
significant degree of internal rigidity.  In nematic phases, rod-like
molecules are orientationally ordered with isotropic distributions of
molecular centers of mass, while in smectic phases, the molecules
arrange themselves into layers with their long (symmetry) axis normal
($S_{A}$) or tilted ($S_{C}$) with respect to the layer planes.

The behavior of the $S_{A}$ phase can be partially explained with
models mainly based on geometric factors and van der Waals
interactions.  However, these simple models are insufficient to
describe liquid crystal phases which exhibit more complex polymorphic
nature.  X-ray diffraction studies have shown that the ratio between
lamellar spacing ($s$) and molecular length ($l$) can take on a wide
range of values.\cite{Gray:1984hc,Leadbetter:1976vf,Hardouin:1980yq}
Typical $S_{A}$ phases have $s/l$ ratios on the order of $0.8$, while
for some compounds, e.g. the 4-alkyl-4'-cyanobiphenyls, the $s/l$
ratio is on the order of $1.4$.  Molecules which form $S_{A}$ phases
can exhibit a wide variety of subphases like monolayers ($S_{A1}$),
uniform bilayers ($S_{A2}$), partial bilayers ($S_{\tilde A}$) as well
as interdigitated bilayers ($S_{A_{d}}$), and often have a terminal
cyano or nitro group.  In particular lyotropic liquid crystals (those
exhibiting liquid crystal phase transition as a function of water
concentration) often have polar head groups or zwitterionic charge
separated groups that result in strong dipolar
interactions.\cite{Collings97} Because of their versatile polymorphic
nature, polar liquid crystalline materials have important
technological applications in addition to their immense relevance to
biological systems.\cite{Collings97}

Experimental studies by Levelut {\it et al.}~\cite{Levelut:1981eu}
revealed that terminal cyano or nitro groups usually induce permanent
longitudinal dipole moments on the molecules.

Liquid crystalline materials with dipole moments located at the ends
of the molecules have important applications in display technologies
in addition to their relevance in biological systems.\cite{LCapp}

Many of the technological applications of the lyotropic mesogens
manipulate the orientation and structuring of the liquid crystal
through application of local electric fields.\cite{?}
Macroscopically, this restructuring is visible in the interactions the
bulk phase has with scattered or transmitted light.\cite{?}  

4-Cyano-4'-pentylbiphenyl (5CB), has been a model for field-induced
phase changes due to the known electric field response of the liquid
crystal\cite{Hatta:1991ee}.  It was discovered (along with three
similar compounds) in 1973 in an effort to find a LC that had a
melting point near room temperature.\cite{Gray:1973ca} It's known to
have a crystalline to nematic phase transition at 18 C and a nematic
to isotropic transition at 35 C.\cite{Gray:1973ca}

Nitrile groups can serve as very precise electric field reporters via
their distinctive Raman and IR signatures.\cite{Boxer:2009xw} The
triple bond between the nitrogen and the carbon atom is very sensitive
to local field changes and is observed to have a direct impact on the
peak position within the spectrum.  The Stark shift in the spectrum
can be quantified and mapped into a field value that is impinging upon
the nitrile bond. This has been used extensively in biological systems
like proteins and enzymes.\cite{Tucker:2004qq,Webb:2008kn} 

To date, the nitrile electric field response of
4-Cyano-4'-n-alkylbiphenyl liquid crystals has not been investigated.
While macroscopic electric fields applied across macro electrodes show
the phase change of the molecule as a function of electric
field,\cite{Lim:2006xq} the effect of a microscopic field application
has not been probed. These previous studies have shown the nitrile
group serves as an excellent indicator of the molecular orientation
within the field applied. Blank showed the 180 degree change in field
direction could be probed with the nitrile peak intensity as it
decreased and increased with molecule alignment in the
field.\cite{Lee:2006qd,Leyte:97}

While these macroscopic fields worked well at showing the bulk
response, the atomic scale response has not been studied. With the
advent of nano-electrodes and coupling them with atomic force
microscopy, control of electric fields applied across nanometer
distances is now possible\cite{citation1}. This application of
nanometer length is interesting in the case of a nitrile group on the
molecule. While macroscopic fields are insufficient to cause a Stark
effect, small fields across nanometer-sized gaps are of sufficient
strength. If one were to assume a gap of 5 nm between a lower
electrode having a nanoelectrode placed near it via an atomic force
microscope, a field of 1 V applied across the electrodes would
translate into a field of 2x10\textsuperscript{8} $\frac{V}{M}$. This
field is theoretically strong enough to cause a phase change from
isotropic to nematic, as well as Stark tuning of the nitrile
bond. This should be readily visible experimentally through Raman or
IR spectroscopy.

Herein, we show the computational investigation of these electric field effects through atomistic simulations. These are then coupled with ab intio and classical spectrum calculations to predict changes experiments should be able to replicate.

\section{Computational Details}
The force field was mainly taken from Guo et al.\cite{Zhang:2011hh} A
deviation from this force field was made to create a rigid body from
the phenyl rings. Bond distances within the rigid body were taken from
equilibrium bond distances. While the phenyl rings were held rigid,
bonds, bends, torsions and inversion centers still included the rings.

Simulations were with boxes of 270 molecules locked at experimental
densities with periodic boundaries. The molecules were thermalized
from 0 kelvin to 300 kelvin. To equilibrate, each was first run in NVT
for 1 ns. This was followed by NVE for simulations used in the data
collection.

External electric fields were applied in a simplistic charge-field
interaction. Forces were calculated by multiplying the electric field
being applied by the charge at each atom. For the potential, the
origin of the box was used as a point of reference. This allows for a
potential value to be added to each atom as the molecule move in space
within the box. Fields values were applied in a manner representing
those that would be applable in an experimental set-up. The assumed
electrode seperation was 5 nm and the field was input as
$\frac{V}{\text{\AA}}$. The three field environments were, 1) no field
  applied, 2) 0.01 $\frac{V}{\text{\AA}}$ (0.5 V) and 3) 0.024
    $\frac{V}{\text{\AA}}$ (1.2 V). Each field was applied in the
    Z-axis of the simulation box. For the simplicity of this paper,
    each field will be called zero, partial and full, respectively.

For quantum calculation of the nitrile bond frequency, Gaussian 09 was
used. A single 5CB molecule was selected for the center of the
cluster. For effects from molecules located near the chosen nitrile
group, parts of molecules nearest to the nitrile group were
included. For the body not including the tail, any atom within 6~\AA 
of the midpoint of the nitrile group was included. For the tail
structure, the whole tail was included if a tail atom was within 4~\AA 
of the midpoint. If the tail did not include any atoms from the ring
structure, it was considered a propane molecule and included as
such. Once the clusters were generated, input files were created that
stretched the nitrile bond along its axis from 0.87 to 1.52~\AA at
increments of 0.05~\AA. This generated 13 single point energies to be
calculated. The Gaussian files were run with B3LYP/6-311++G(d,p) with
no other keywords for the zero field simulation. Simulations with
fields applied included the keyword ''Field=Z+5'' to match the
external field applied in molecular dynamic runs. Once completed, the central nitrile bond frequency
was calculated with a Morse fit. Using this fit and the solved energy
levels for a Morse oscillator, the frequency was found. Each set of
frequencies were then convolved together with a lorezian lineshape
function over each value. The width value used was 1.5. For the zero
field spectrum, 67 frequencies were used and for the full field, 59
frequencies were used.

Classical nitrile bond frequencies were found by replacing the rigid
cyanide bond with a flexible Morse oscillator bond
($r_0= 1.157437$ \AA , $D_0 = 212.95$ and
$\beta = 2.67566$) . Once replaced, the
systems were allowed to re-equilibrate in NVT for 100 ps. After
re-equilibration, the system was run in NVE for 20 ps with a snapshot
spacing of 1 fs. These snapshot were then used in bond correlation
calculation to find the decay structure of the bond in time using the
average bond displacement in time,
\begin{equation}
C(t) = \langle \left(r(t) - r_0 \right) \cdot \left(r(0) - r_0 \right) \rangle
\end{equation}
%
where $r_0$ is the equilibrium bond distance and $r(t)$ is the
instantaneous bond displacement at time $t$. Once calculated,
smoothing was applied by adding an exponential decay on top of the
decay with a $\tau$ of 3000 (have to check this). Further smoothing
was applied by padding 20,000 zeros on each side of the symmetric
data. This was done five times by allowing the systems to run 1 ns
with a rigid bond followed by an equilibrium run with the bond
switched back on and the short production run.

\section{Results}

In order to characterize the orientational ordering of the system, the
primary quantity of interest is the nematic (orientational) order
parameter. This is determined using the tensor
\begin{equation}
Q_{\alpha \beta} = \frac{1}{2N} \sum_{i=1}^{N} \left(3 \hat{e}_{i
    \alpha} \hat{e}_{i \beta} - \delta_{\alpha \beta} \right)
\end{equation}
where $\alpha, \beta = x, y, z$, and $\hat{e}_i$ is the molecular
end-to-end unit vector for molecule $i$. The nematic order parameter
$S$ is the largest eigenvalue of $Q_{\alpha \beta}$, and the
corresponding eigenvector defines the director axis for the phase.
$S$ takes on values close to 1 in highly ordered phases, but falls to
zero for isotropic fluids. In the context of 5CB, this value would be
close to zero for its isotropic phase and raise closer to one as it
moved to the nematic and crystalline phases.

This value indicates phases changes at temperature boundaries but also
when a phase changes occurs due to external field applications. In
Figure 1, this phase change can be clearly seen over the course of 60
ns. Each system starts with an ordering paramter near 0.1 to 0.2,
which is an isotropic phase. Over the course 10 ns, the full external field
causes a shift in the ordering of the system to 0.5, the nematic phase
of the liquid crystal. This change is consistent over the full 50 ns
with no drop back into the isotropic phase. This change is clearly
field induced and stable over a long period of simulation time.
\begin{figure}
  \includegraphics[trim = 5mm 10mm 3mm 10mm, clip, width=3.25in]{P2}
  \caption{Ordering of each external field application over the course
    of 60 ns with a sampling every 100 ps. Each trajectory was started
    after equilibration with zero field applied.}
  \label{fig:orderParameter}
\end{figure}

Interestingly, the field that is needed to switch the phase of 5CB
macroscopically is larger than 1 V. However, in this case, only a
voltage of 1.2 V was need to induce a phase change. This is impart due
to the distance the field is being applied across. At such a small
distance, the field is much larger than the macroscopic and thus
easily induces a field dependent phase change.

In the figure below, this phase change is represented nicely as
ellipsoids that are created by the vector formed between the nitrogen
of the nitrile group and the tail terminal carbon atom. These
illistrate the change from isotropic phase to nematic change. Both the
zero field and partial field images look mostly disordered. The
partial field does look somewhat orded but without any overall order
of the entire system. This is most likely a high point in the ordering
for the trajectory. The full field image on the other hand looks much
more ordered when compared to the two lower field simulations.
\begin{figure}
  \includegraphics[width=7in]{Elip_3}
  \caption{Ellipsoid reprsentation of 5CB at three different
    field strengths, Zero Field (Left), Partial Field (Middle), and Full
    Field (Right) Each image was created by taking the final
    snapshot of each 60 ns run}
  \label{fig:Cigars}
\end{figure}

This change in phase was followed by two courses of further
analysis. First was the replacement of the static nitrile bond with a
morse oscillator bond. This was then simulated for a period of time
and a classical spetrum was calculated. Second, ab intio calcualtions were performe to investigate
if the phase change caused any change spectrum through quantum
effects.

The classical nitrile spectrum can be seen in Figure 2. Most noticably
is the position of the two peaks. Obviously the experimental peak
position is near 2226 cm\textsuperscript{-1}. However, in this case
the peak position is shifted to the blue at a position of 2375
cm\textsuperscript{-1}. This shift is due solely to the choice of
oscillator strength in the Mores oscillator parameters. While this
shift makes the two spectra differ, it does not affect the ability to
compare peak changes to experimental peak changes.
With this important fact out of the way, differences between the two
states are subtle but are very much present. The first and
most notable is the apperance for a strong band near 2300
cm\textsuperscript{-1}.
\begin{figure}
  \includegraphics[width=3.25in]{2Spectra}
  \caption{The classically calculated nitrile bond spetrum for no
    external field application (black) and full external field
    application (red)}
  \label{fig:twoSpectra}
\end{figure}

Before Gaussian silumations were carried out, it was attempt to apply
the method developed by Cho et. al. This method involves the fitting
of multiple parameters to However, since these simulations
are done under the presence of external electric fields and in the
absence of water the equations had to be reworked. Originally, the
nitrile bond frequency was related to the potential of water around
the bond via 
\begin{equation}
\phi_{a} = \frac{1}{4\pi \epsilon_{0}} \sum_{m} \sum_{j}
\frac{C^{H_{2}O}_{j \left(m \right) }}{r_{aj \left(m\right)}}
\end{equation}
After Gaussian calculations were performed on a set of snapshots for
the zero and full field simualtions, they were first investigated for
any dependence on the local, with external field included, electric
field. This was to see if a linear or non-linear relationship between
the two could be utilized for generating spectra. This was done in
part because of previous studies showing the frequency dependence of
nitrile bonds to the electric fields generated locally between
solvating water. It was seen that little to no dependence could be
directly shown. This data is not shown.

Since no explicit dependence was observed between the calculated
frequency and the electric field, it was not a viable route for the
calculation of a nitrile spectrum. Instead, the frequencies were taken
and convolved together. These two spectra are seen below in Figure
4. While the spectrum without a field is lower in intensity and is
almost bimodel in distrobuiton, the external field spectrum is much
more unimodel. This narrowing has the affect of increasing the
intensity around 2226 cm\textsuperscript{-1} where the peak is
centered. The external field also has fewer frequencies higher to the
blue of the spectra. Unlike the the zero field, where some frequencies reach as high
as 2280 cm\textsuperscript{-1}. 
\begin{figure}
  \includegraphics[width=3.25in]{Convolved}
  \caption{Lorentzian convolved Gaussian frequencies of the zero field
  system (black) and the full field system (red)}
  \label{fig:Con}
\end{figure}
\section{Discussion}
The absence of any electric field dependency of the freuquency with
the Gaussian simulations is strange. A large base of research has been
built upon the known tuning the nitrile bond as local field
changes. This differences may be due to the absence of water. Many of
the nitrile bond fitting maps are done in the presence of
water. Liquid water is known to have a very high internal field which
is much larger than the internal fields of neat 5CB. Even though the
application of running Gaussian simulations followed by mappying to
some classical parameter is easy and straight forward, this system
illistrates how that 'go to' method can break down.

While this makes the application of nitrile Stark effects in
simulations of liquid water absent simulations harder, these data show
that it is not a deal breaker. The classically calculated nitrile
spectrum shows changes in the spectra that will be easily seen through
experimental routes. It indicates a shifted peak lower in energy
should arise. This peak is a few wavenumbers from the larger peak and
almost 75 wavenmubers from the center. This seperation between the two
peaks means experimental results will show a well resolved peak.

The Gaussian derived frequencies and subsiquent spectra also indicate
changes that can be observed experimentally. 
\section{Conclusions}
Jonathan K. Whitmer
cho stuff
\newpage

\bibliography{5CB}

\end{doublespace}
\end{document}
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