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Preservation of Photoluminescence Efficiency in the Ordered phases of Poly(2,3-diphenyl-1,4-phenylenevinylene) via Disturbing the Intermolecular π-π Interactions with Dendritic Aliphatic Side Chains
Preservation of Photoluminescence Efficiency in the Ordered phases of Poly(2,3-diphenyl-1,4-phenylenevinylene) via Disturbing the Intermolecular π-π Interactions with Dendritic Aliphatic Side Chains
To understand the relation between the solid-state phase structures and the photophysical properties of poly(2,3-diphenyl-1,4-phenylenevinylene) (DP-PPV) derivatives, three DP-PPV derivatives, P1?P3, were designed, synthesized via Gilchpolymerization and characterized. Among the polymers, P1 is a reported highly emissive poly(2,3-diphenyl-5-hexyl-pphenylenevinylene),and P2 and P3 are novel DP-PPV derivatives, which are purposely designed to bear hydrophobic andhydrophilic Percec-type dendrons as side chains. The bulkiness and hydrophobic?hydrophilic natures of the side chains showstrong effects on photophysical properties of the polymers. The solutions and as-casted films of P1?P3 all show remarkably highphotoluminescence (PL) efficiency (ΦPL) (>80% in chloroform solution, and >63% for the as-casted films). However, ΦPL of P1and P3 decrease significantly to 30% after cooled their polymer melts to room temperature. Through the phase behavior analysisby differential scanning calorimetry (DSC), and phase structure analysis by wide-angle X-ray diffraction (WAXD), the decrease ofΦPL can be elucidated and attributed to the ordering of the solid-state structures of P1 and P3. To our surprise, ΦPL of P2 ispreserved even in an ordered solid-state phase, and it is insensitive to the structural ordering. Structural analysis of P2 revealedthat the aliphatic dendritic side chains of P2 effectively disturbing the intermolecular π?π interactions among the conjugatedbackbones, which allows the preservation of ΦPL in the environment with ordered packing of DP-PPV molecules. The results oftime-resolved PL decay experiments also confirmed that P2 possesses long-lived decay time because of excitons confined moreeffectively for emissive relaxation.
