Chasteen S V, Carter S A, Rumbles G
Physics Department, University of California-Santa Cruz, Santa Cruz, California 95064, USA.
J Chem Phys. 2006 Jun 7;124(21):214704. doi: 10.1063/1.2196036.
We investigate the effect of broken conjugation on the excited state dynamics of excimers in cyano-substituted phenylene-vinylene polymers. We compare previous studies on the well-characterized poly(2,5,2',5'-tetrahexyloxy-8,7'-dicyano-di-p-phenylene vinylene) (CN-PPV) with poly[oxa-1,4-phenylene-1,2-(1-cyano)-ethenylene-2,5-dioctyloxy-1,4-phenylene-1,2-(2-cyano)-ethenylene-1,4-phenylene] (CN-ether-PPV), in which the conjugation is disrupted by the insertion of an oxygen atom within the polymer backbone. Despite the broken conjugation, the spectroscopic behavior of the two materials is similar, indicating that the cyano group dominates the photophysics in these materials. The emission in CN-ether-PPV is due to a single-chain exciton in solution and due to an interchain excimer in thin film, as previously reported for CN-PPV; however, the excimer absorption and emission in thin film are blueshifted by approximately 0.2 eV relative to CN-PPV, implying that the excimer in CN-ether-PPV is less stable. Furthermore, substitution of an ether group along the chain results in decay times in both solution and film that are twice as long than in CN-PPV due to the broken conjugation which restricts the exciton within a conjugation segment and reduces its access to internal quenching sites. These properties result in a decay time of 14 ns for CN-ether-PPV film, one of the longest decay times observed in a conjugated polymer film. The long lifetime indicates a large exciton diffusion length, making these species particularly vulnerable to quenching by other materials. This work has implications for the design of conjugated polymers for efficient optoelectronic devices, such as photovoltaics.
我们研究了共轭破坏对氰基取代的亚苯基-亚乙烯基聚合物中激基缔合物激发态动力学的影响。我们将之前对特征明确的聚(2,5,2',5'-四己氧基-8,7'-二氰基-对苯撑乙烯)(CN-PPV)的研究与聚[氧杂-1,4-亚苯基-1,2-(1-氰基)-亚乙烯基-2,5-二辛氧基-1,4-亚苯基-1,2-(2-氰基)-亚乙烯基-1,4-亚苯基](CN-醚-PPV)进行了比较,在CN-醚-PPV中,聚合物主链中插入氧原子会破坏共轭。尽管共轭被破坏,但这两种材料的光谱行为相似,表明氰基主导了这些材料中的光物理过程。如之前对CN-PPV的报道,CN-醚-PPV在溶液中的发射归因于单链激子,在薄膜中归因于链间激基缔合物;然而,相对于CN-PPV,薄膜中激基缔合物的吸收和发射发生了约0.2 eV的蓝移,这意味着CN-醚-PPV中的激基缔合物不太稳定。此外,沿着链取代醚基会导致溶液和薄膜中的衰减时间是CN-PPV中的两倍,这是由于共轭破坏将激子限制在共轭段内并减少了其与内部猝灭位点的接触。这些特性导致CN-醚-PPV薄膜的衰减时间为14 ns,这是在共轭聚合物薄膜中观察到的最长衰减时间之一。长寿命表明激子扩散长度较大,使得这些物质特别容易被其他材料猝灭。这项工作对用于高效光电器件(如光伏器件)的共轭聚合物的设计具有启示意义。