Figures & data
Figure 1 Discotic star oligomer1 composed of three radial pentayne groups linked to a central benzene moiety by alkyl spacers.
![Figure 1 Discotic star oligomer1 composed of three radial pentayne groups linked to a central benzene moiety by alkyl spacers.](/cms/asset/adf4bdb9-1500-4d04-828b-b48e7b23d18e/tlcy_a_10329406_o_tlcy0001fig001.gif)
Figure 2 Structure model of the nematic columnar(NCol) bulk mesophase formed by the star‐shaped pentayne oligomer 1.
![Figure 2 Structure model of the nematic columnar(NCol) bulk mesophase formed by the star‐shaped pentayne oligomer 1.](/cms/asset/e7523c97-b360-4073-8fbe-55ee25495f61/tlcy_a_10329406_o_tlcy0001fig002.gif)
Figure 3 Schlieren texture of a spin‐coated pentayne 1 film on glass substrate between crossed polarizers after thermal treatment within the mesophase and cooling down to room temperature.
![Figure 3 Schlieren texture of a spin‐coated pentayne 1 film on glass substrate between crossed polarizers after thermal treatment within the mesophase and cooling down to room temperature.](/cms/asset/6e47208f-d763-41a5-b2de-b9a462fedff8/tlcy_a_10329406_o_tlcy0001fig003.gif)
Figure 4 Optical textures of spin‐coated films of the star‐shaped oligomesogen 1 on polyimide alignment layers at room temperature after annealing within the mesophase; a) Polyimide SE‐3140. The disclination lines run predominantly parallel to the rubbing direction of the orientation layer; b) Polyimide ZLI‐2650; c) after rotation of the sample in b) by 45° arround the optical axis.
![Figure 4 Optical textures of spin‐coated films of the star‐shaped oligomesogen 1 on polyimide alignment layers at room temperature after annealing within the mesophase; a) Polyimide SE‐3140. The disclination lines run predominantly parallel to the rubbing direction of the orientation layer; b) Polyimide ZLI‐2650; c) after rotation of the sample in b) by 45° arround the optical axis.](/cms/asset/8f2e7c78-bc9d-4324-93fe-88b90e27a2f1/tlcy_a_10329406_o_tlcy0001fig004.gif)
Figure 5 (x) Retardation of a 1.1 µm thick film of compound 1 depending on the incidence angle after thermal treatment on ZLI‐2650 polyimide layer. (+) is a fit of a negatively uniaxial tilted model to the data. The values for incidence angles from 35°–50° were determined at a azimuth differing by 6° from the linear eigenpolarisation and were excluded from the fitting procedure.
![Figure 5 (x) Retardation of a 1.1 µm thick film of compound 1 depending on the incidence angle after thermal treatment on ZLI‐2650 polyimide layer. (+) is a fit of a negatively uniaxial tilted model to the data. The values for incidence angles from 35°–50° were determined at a azimuth differing by 6° from the linear eigenpolarisation and were excluded from the fitting procedure.](/cms/asset/44848099-28e3-4b53-bfcb-f5d1c2d82908/tlcy_a_10329406_o_tlcy0001fig005.gif)
Figure 6 Schematic presentation of possible molecular orientations of the discotic pentayne cores of the star‐shaped oligomesogen 1 after annealing on top of a rubbed polyimide layer; a) Alignment with a uniform tilt angle; b) Splayed orientation with continuous alteration of the tilt angle. The macroscopic orientation is frozen in a glassy state at room temperature.
![Figure 6 Schematic presentation of possible molecular orientations of the discotic pentayne cores of the star‐shaped oligomesogen 1 after annealing on top of a rubbed polyimide layer; a) Alignment with a uniform tilt angle; b) Splayed orientation with continuous alteration of the tilt angle. The macroscopic orientation is frozen in a glassy state at room temperature.](/cms/asset/b245c14c-ebf8-4ffc-904f-49a8c2912f1c/tlcy_a_10329406_o_tlcy0001fig006.gif)