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Fig. 5 Local polymer chain conformation of nematic side chain elastomers (with respect to the
nematic director
n
) and resulting global chain conformation in the cholesteric phase structure (with
respect to the cholesteric helix axis
h
)
with respect to the local director. In the helicoidal phase structure of chiral nematic
elastomers, however, this orientation corresponds to an overall oblate chain confor-
mation with respect to the helix axis as the local director rotates continuously along
this axis (Fig.
5
). Therefore a globally oblate chain conformation has to be
established in order to achieve a cholesteric monodomain. Using biaxial stretching
or uniaxial compression, elastomers with homeotropically aligned helix axes can be
obtained [
72
]. In the case of a chiral nematic polymer with even spacer length and
thus locally oblate chain conformation with respect to the local director, a prolate
chain conformation exists with respect to the helix axis. Uniaxial mechanical
stretching induces a macroscopic orientation of the helix axis along the stretching
Smectic side-chain polymers prefer locally oblate chain conformations, indepen-
dent of the spacer length or attachment geometry. Analogous to oblate nematic
polydomain elastomers, biaxial mechanical stretching or uniaxial compression can
be used to orient S
A
polydomain elastomers. This achieves a simultaneous orientation
Upon uniaxial stretching a polydomain elastomer in the smectic-A phase,
the layer planes usually couple to the mechanical field. This process does not
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