1188 Ting et al.
Macromolecules, Vol. 35, No. 4, 2002
However, it overlapped with the aromatic protons.
Similar result was reported by Matsunami et al.32 Since
polymer 1P has a very rigid polyacetylene backbone and
contains no spacer, it is very difficult for the mesogenic
side groups to form a mesophase. Polymer 1P under-
went decomposition and other aromatization side reac-
tion at over 300 °C, which agrees with the thermo-
gravimetry measurement.
at all. However, polymers 4P -9P present two UV-vis
absorption peaks at about 226 and 279 nm and emit a
luminescence peak at 500 nm. Figure 10 shows the
representative UV-vis and photoluminescent spectra
of polymer 9P . The photoluminescent intensity of
polymer 9P is quite weak due to strong intermolecular
interactions which give rise to self-quenching. Never-
theless, when 9P was blended with PMMA, its photo-
luminescent intensity increases dramatically (Figure ll).
The photoluminescent intensity increases as the weight
percentage of PMMA increases from 25 to 50. The
results demonstrate that the addition of a nonemissive
polymer as diluent for the LC polyacetylene reduces its
interchain interaction and therefore enhances its pho-
toluminescent intensity.
Figure 6 presents representative DSC thermograms
of polymer 6P . It displays two smectic phases on both
heating and cooling scans. The mesophase identification
have been achieved by optical polarizing microscopic
observation and X-ray diffraction. Figure 7A shows a
focal-conic fan, and Figure 7B shows a broken fan
textures exhibited by polymer 6P . Figure 8 presents the
temperature-dependent X-ray diffraction diagrams ob-
tained from powder samples of 6P at 175 and 90 °C. At
175 °C, the diffraction diagram presents a diffuse
reflection at 5.21 Å, which corresponds to the lateral
spacing of two mesogenic side groups, and a sharp first-
order reflection at 39.03 Å and a second-order reflection
at 19.30 Å, which correspond to smectic layers. The
optical polarizing micrograph reveals a focal-conic fan
texture at this temperature range. Both results are
consistent with a smectic A structure. When the mea-
suring temperature is lowered from 175 to 90 °C, the d
spacing of the first-order reflection decreases from 39.03
to 38.58 Å. The optical polarizing micrograph (Figure
7B) shows a broken fan texture at this temperature
range. The results indicate the formation of a tilted
smectic phase, probably a smectic C phase. The detailed
structure of the smectic phase showed be further studied
by X-ray diffraction pattern of an aligned monodomain
sample.
Con clu sion
A new series of side-chain LC polyacetylenes contain-
ing 4-alkanyloxyphenyl trans-4-alkylcyclohexanoate side
groups were synthesized using simple metal halide
initiators. Polymers 1P -3P without flexible spacer,
show no mesomorphic behavior, while polymers 4P -
9P containing three or four methylene units in their
spacers, display both smectic A and smectic C phases.
Compared to the corresponding polyoxetanes, the LC
polyacetylenes have much higher glass transition and
isotropization temperatures. X-ray diffraction results
also demonstrate that the LC polyacetylenes tend to
form an interdigitated bilayer structure for the smectic
phases. Polymers 4P -9P have a weak photolumines-
cence emission at about 500 nm. After blending with
PMMA, their photoluminescence intensities increase
dramatically.
Ack n ow led gm en t. The authors are grateful to the
National Science Council of the Republic of China for
financial support of this work (NSC 89-2216-E009-023).
Com p a r ison of th e Effect of Rigid a n d F lexible
P olym er Ba ck bon es on Th eir Mesom or p h ic P r op -
er ties. Since polyacetylene is a very rigid polymer
backbone, we can investigate the effect of a rigid
polymer backbone on their mesomorphic properties. In
a previous publication,29 we reported a series of poly-
oxetanes containing the same 4-alkanyloxyphenyl trans-
4-alkylcyclohexanoate side groups. The polyacetylenes
synthesized in this study have much higher glass
transition and isotropization temperatures than the
corresponding polyoxetanes. The reason could be due
to the rigidity of the polyacetylene backbones. As far as
the mesomorphic behavior, polymers 4P -9P reveal
smectic A and smectic C phases, while the polyoxetanes
display a nematic phase and two smectic phases. The
LC polymers with rigid polymer backbones have a
tendency to form smectic phases. The d spacing of
smectic layer for LC polyacetylene is 39.03 Å at 175 °C.
According to molecular calculation, the layer spacing is
considerably greater than molecular length of the side
group in a LC polyacetylene. The LC polyacetylenes
obviously tend to form an interdigitated bilayer struc-
ture (Figure 9A). According to our previous report,29 the
smectic layer spacing of a LC polyoxetane is about 29.7
Å which is very close to the molecular length of its side
groups. Thus, the LC polyoxetane which contain a more
flexible backbone form only the single layer smectic
arrangement (Figure 9B).
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9P . Table 7 summarizes the results of UV-vis and
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