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Fig. 6 Molecular structure of poly( p -phenylene) derivatives with a PEO group in their side
chains
Fig. 7 Complexation of PEO-based LC polymers with lithium salts, and their nanostruc-
ture
Kato, Ohno and coworkers have used an in-situ photopolymerization tech-
nique to overcome the problem of the alignment of LC polymers [67-69].
Two-dimensionally ion-conductive polymer films ( 7 )wereobtainedby
photopolymerization of aligned monomer complexes. The monomer self-
assembles into layered nanostructures, in which PEO moieties form nano-
segregated ion transporting channels. The complex of the LC monomer with
LiOSO 2 CF 3 exhibits a smectic A phase. UV irradiation of the homeotrop-
ically aligned complex results in the formation of a free-standing film, as
shown in Fig. 8 [67]. The film shows ionic conductivities in the order of
10 -6 Scm -1 in the direction parallel to the layers, which is approximately
5000-times higher than that perpendicular to the layers. The value of the
conductivity is not so high because the segmental motion of the PEO moi-
ety is restricted between the polymer backbone and the mesogenic parts.
The conductivity can be enhanced to the order of 10 -3 Scm -1 by introducing
a PEO moiety at the terminal of the side chain ( 8 , Fig. 9) [68]. The cor-
responding acrylate monomer complex with LiOSO 2 CF 3 (0.05 mol % to the
oxyethylene) was polymerized in the smectic A phase at 60 CbyUVirradi-
ation. Polymer 8 complexed with LiOSO 2 CF 3 exhibits the glass transition
at -45 C and the solid-smectic A transition at 161 C. The isotropization
temperature is observed at 202 C. At room temperature, conductivity in
the range of 10 -3 Scm -1 to the direction parallel to the layer is observed,
even though the complex forms a solid state. These high ionic conductivi-
ties of the complex of 8 can be ascribed to the liquid-like layers in the solid
oriented film.
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