307 publications from this institution
Altering the sample temperature in a photorefractive material changes the rotational mobility of the chromophores. A change of three orders of magnitude in the response times over a temperature change of 12 K has been observed. In the photorefractive experiment, however, the chromophore orientation is induced by the non-instantaneous change of the space charge field. The finite speed of the latter causes the chromophore answer to be different from their normal relaxation behaviour to an instantaneous change. This effect is most pronounced when both time constants are in the same range.
We describe two methods by which discotic liquid crystalline (LC) triphenylene materials can be sensitized for wavelengths of the visible spectrum and the near IR. One way of doping is more conventional and uses bi-layers between the LC-system and an adjacent pigment layer. The second doping is achieved by a molecular doping with C<sub>70</sub>. Here the influence of doping on the measured mobilities is much smaller as compared to the influence of doping measured in amorphous systems. We attribute this smaller influence of the C<sub>70</sub>-doping on the mobility to a partial phase separation occuring between the LC-host material and the C<sub>70</sub>-guest molecules. In our comparative experiments on doped dimethyl-triphenyldiamines we can show taht the magnitude of the trap depths for hole-trapping has a very large influence on the measured transport parameters.
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Herein we report the application of supramolecular dyes to control charge recombination between photo-injected electrons and oxidized hole-transporting material, resulting in an enhancement in the performance of dye sensitized solar cell devices based upon such dyes.
A systematic study of the influence of the chemical substitution pattern of side chain polymers carrying perylene bisimide (PBI) pendants is presented. To achieve a high comparability, the modular approach of copper-catalyzed azide–alkyne cycloaddition (CuAAC, “click” chemistry) was chosen to attach six differently substituted PBI azide moieties to a poly(propargyloxystyrene) backbone to obtain poly(perylene bisimides), PPBIs. The N, N′ substituted PPBIs differ structurally in two ways. On the one hand, the N-swallow-tail substituent was varied between hydrophilic oligoethyleneglycol and hydrophobic alkyl groups. On the other hand, the length of the N′-alkyl spacer, connecting PBI moiety and polymer backbone, was varied from (CH2)6 to (CH2)8 and to (CH2)11. The polymer analogous reactions between PBI-azides and poly(propargyloxystyrene) were monitored by 1H NMR and were found to be nearly quantitative in all cases. The resulting PPBIs exhibit Mn around 60 000 g mol−1 and narrow PDIs of 1.1. Structure–property relationships of all polymers were elucidated by studying their thermal behaviour using DSC and their structural properties with XRD measurements.
Polythiophene-based conjugated polyelectrolytes (CPE) are attracting increasing attention as sensor or interface materials in chemistry and biology. While cationic polythiophenes are better understood, limited structural information is available on their anionic counterparts. Limited access to well-defined polymers has made the study of structure-property relationships difficult and clear correlations have remained elusive. By combining controlled Kumada catalyst transfer polymerization with a polymer-analog substitution, regioregular and narrowly distributed poly(6-(thiophen-3-yl)hexane-1-sulfonate)s (PTHS) with tailored chain length are prepared. Analysis of their aqueous solution structures by small-angle neutron scattering (SANS) revealed a cylindrical conformation for all polymers tested, with a length close to the contour length of the polymer chains, while the estimated radii remain too small (<1.5 nm) for extensive π-stacking of the chains. The latter is particularly interesting as the longest polymer exhibits a concentration-independent structured absorption typical of crystalline polythiophenes. Increasing the ionic strength of the solution diminishes these features as the Coulomb repulsion between the charged repeat units is shielded, allowing the polymer to adopt a more coiled conformation. The extended π-conjugation, therefore, appears to be a key parameter for these unique optical features, which are not present in the corresponding cationic polythiophenes.
Abstract Summary: Rapid materials screening and combinatorial development of thin film multilayer electro‐optical devices is essential for fast research and development progress and the implementation of device structures into commercial products. A well‐established and reliable film preparation technique within the required nanometer film thickness range is vapor deposition. The combinatorial approach underlying this feature article is based on the preparation of linear or step gradient and the preparation of sectors of material combinations or device structures by using mask movements in combination with a rotation of the substrate. Both of the two principles are combined to obtain an infinite number of possible libraries with different complexity, which may differ in each sector by the layer thickness, the sequence of layers, and the material selection. In addition by simultaneous evaporation using two or more sources and varying the deposition rate, material compositions can also be created. In this feature article we review our work on combinatorial material screening and combinatorial optimization of multilayer thin film organic electro‐optical devices prepared by vapor deposition. This article covers results on organic light emitting devices (OLEDs), organic solar cells, the orientation behavior of formanisotropic functional molecules on alignment layers and the in situ preparation and orientation of rodlike and thermally stable aromatic polyimides. Example of a combinatorial vapor deposition technique, which is a powerful tool to screen efficiently new materials and configurations in thin film multilayer electro‐optical devices. magnified image Example of a combinatorial vapor deposition technique, which is a powerful tool to screen efficiently new materials and configurations in thin film multilayer electro‐optical devices.