| Description of
project |
During
the last few years a number of stimulating reports1-9
have revealed mixtures of carbon nanotubes (CNTs) in
liquid crystals (LCs) to be multifaceted and
attractive composites with possible applications in
diverse areas of science and technology. The meeting
between carbon nanotubes—an extreme example of hard
functional anisotropic nanoparticles—and liquid
crystals—self-organizing anisotropic fluid soft
matter—brings up many new intriguing questions of
physics and chemistry. So far, the studies have been
motivated mainly by a number of interesting
observations of potential interest for applications:
on the one hand, the LC host transfers its inherent
orientational order onto the nanotube guests1-6,
which can be well dispersed in the LC4-6,
on the other, the CNTs can modify the properties of
the LC, in some cases improving their performance in
e.g. display devices7-9.
After having given unambiguous proof of the CNT
alignment along the LC director in lyotropic4,6
as well as thermotropic3,5 LCs using
polarized resonant Raman spectroscopy, we are now
broadening the scope of our studies of these
fascinating composite systems. In addition to
monitoring alignment quantitatively and dynamically
while modifying the geometry and type of the LC host
and / or type and concentration of the CNT guests, we
now focus also on the various effects that the CNTs
have on the LC, in particular regarding phase
sequence, switching dynamics and free ion content.
Moreover, we are looking into the interactions between
mesogens / surfactants and CNTs on the molecular to
the mesoscopic scales, of great importance for
understanding the macroscopic behavior of the
composite, as well as the interesting and often
surprising electrical properties of composites of CNTs
and thermotropic LCs.

Uniform dispersion (top left) and uniaxial alignment
(top right) of CNTs in lyotropic liquid crystals. The
cartoon at the bottom schematically illustrates the
alignment concept.
References
[1] M.D.
Lynch, and D.L. Patrick, Nano. Lett., 2002,
2, 1197
[2] I. Dierking, G. Scalia, P. Morales, D. LeClere,
Adv. Mater., 2004, 16, 865
[3] G. Scalia, M. Haluska, U. Dettlaff-Weglikowska,
F. Giesselmann, S. Roth, AIP Conf. Proc., 2005,
786, 114
[4] J. P. F. Lagerwall, G. Scalia, M. Haluska, U. Dettlaff-Weglikowska,
S. Roth, F. Giesselmann, Adv. Mater., 2006, in
press
[5]
G. Scalia, J. P. F. Lagerwall, M.
Haluska, U. Dettlaff-Weglikowska, F. Giesselmann, and
S. Roth,
Phys. Stat. Sol. B,
2006, 243, 3238
[6] J.P.F. Lagerwall, G. Scalia, M. Haluska, U.
Dettlaff-Weglikowska, S. Roth, and F. Giesselmann,
Phys. Stat. Sol. B, 243, 2006, 3046
[7] (a) H.-Y. Chen, W. Lee, Appl. Phys. Lett.,
2006, 88, 222105
[8] H. Duran, B. Gazdecki, A. Yamashita, T. Kyu,
Liq. Cryst., 2005 32, 815
|9] C.-Y. Huang, C.-Y Hu, H.-C. Pan, K.-Y. Lo, Jap.
J. Appl.
Phys.,
2005, 44, 8077
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