Molecular orientations in flat-elongated and helical lamellar crystals of a main-chain nonracemic chiral polyester

Single flat-elongated and helical lamellar crystals have been grown thermot ropically in a main-chain nonracemic chiral liquid crystalline polymer that was synthesized from (R)-(-)-4'-{omega-[2-(p-hydroxy-o-nitrophenyloxy)-1-p ropyloxy]-1-nonyloxy}-4-biphenyl carboxylic acid, PET(R*)-9. The crystals p ossess the identical orthorhombic lattice dimensions of a = 1.07 nm, b = 0. 48 nm, and c = 5.96 nm.(1,2) Dark field (DF) image, bright field image, and selective area electron diffraction (SAED) experiments using transmission electron microscopy (TEM) provide chain orientation information in both of these crystals. In the flat-elongated lamellar crystals, the chain directio n is perpendicular to the substrate surface in a center zone along the long (b) axis of the crystals. Moving away from this zone along the short (a) a xis of the crystal, the chain direction continuously tilts in the nc-plane. A small tilt of approximately 0.002 degrees per molecular layer is estimat ed using the SAED results. In the helical lamellar crystals, the main twist direction is parallel to the helical axis, and the rotation angle for each molecular layer is approximately 0.05 degrees. However, specifically desig ned DF experiments using the entire and partial (205) and (206) diffraction arcs show that the chain orientation direction is also twisted along the s hort helical axis of the lamellar crystal. The rotation angle is approximat ely 0.01 degrees per molecular layer. Therefore a second twist direction wi th a changing molecular orientation exists in addition to the long helical axis of the crystal. Based on these experimental observations, the concept of a double-twisted molecular orientation in the helical lamellar crystal c an be established, although in principle, the macroscopic translational sym metry is broken dong both of the long and short axes of the helical lamella r crystals in Euclidean space.