Fig. 4: The optical textures of compound 1 as observed between crossed polarizers on cooling from ColhexΔ via ColhexΔ/□ phases to ColsquT. | Communications Chemistry

Fig. 4: The optical textures of compound 1 as observed between crossed polarizers on cooling from ColhexΔ via ColhexΔ/□ phases to ColsquT.

From: A periodic dodecagonal supertiling by self-assembly of star-shaped molecules in the liquid crystalline state

Fig. 4

ad The birefringent planar textures (columns parallel to the surface) and areas with an alignment of the columns perpendicular to the substrate surfaces (optically isotropic dark areas at the bottom). The optical indicatrices of the distinct phases are shown on the right. The scale bars are 100 μm. The insets show the planar textures with additional λ-retarder plate. In d the orientation of the polarizers (arrows) and the slow indicatrix axis orientation (dotted line) are shown, which are identical for ad. In the ColhexΔ and ColhexΔ/□ phases (a, b) the birefringence is negative (the blue shifted fans with λ-retarder plate are parallel to the indicatrix direction), i.e. the main intramolecular π-conjugation pathway is on average perpendicular to the column long axis with no visible change in birefringence at the phase transition ColhexΔ − ColhexΔ/□ (a → b). At the first order phase transition to ColsquT the birefringence suddenly becomes Δn = 0 (c and inset) and then weakly positive (d the yellow shifted fans are now parallel to the indicatrix direction, see inset in d). This indicates that the π-conjugation pathway crosses a certain angle at which it changes from being perpendicular to the column direction to predominately parallel. On further cooling the birefringence in the ColsquT phase remains smaller than in the Colhex phases, indicating that the π-conjugated rods retain a tilt by a certain angle with respect to the column long axis. The bright spots and lines in c are residues of the coexisting ColhexΔ/□ phase at this strongly first order phase transition.

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