Spectroscopic Investigation of the Effect of Microstructure and Energetic Offset on the Nature of Interfacial Charge Transfer States in Polymer: Fullerene Blends

光致发光 化学 富勒烯 化学物理 电致发光 激子 激发态 光谱学 光诱导电荷分离 有机太阳能电池 分子物理学 聚合物 材料科学 原子物理学 光电子学 凝聚态物理 人工光合作用 物理 有机化学 催化作用 光催化 图层(电子) 量子力学
作者
Stoichko Dimitrov,Mohammed Azzouzi,Jiaying Wu,Jianguo Yao,Yifan Dong,Pabitra Shakya Tuladhar,Bob C. Schroeder,Eric R. Bittner,Iain McCulloch,Jenny Nelson,James R. Durrant
出处
期刊:Journal of the American Chemical Society [American Chemical Society]
卷期号:141 (11): 4634-4643 被引量:43
标识
DOI:10.1021/jacs.8b11484
摘要

Despite performance improvements of organic photovoltaics, the mechanism of photoinduced electron-hole separation at organic donor-acceptor interfaces remains poorly understood. Inconclusive experimental and theoretical results have produced contradictory models for electron-hole separation in which the role of interfacial charge-transfer (CT) states is unclear, with one model identifying them as limiting separation and another as readily dissociating. Here, polymer-fullerene blends with contrasting photocurrent properties and enthalpic offsets driving separation were studied. By modifying composition, film structures were varied from consisting of molecularly mixed polymer-fullerene domains to consisting of both molecularly mixed and fullerene domains. Transient absorption spectroscopy revealed that CT state dissociation generating separated electron-hole pairs is only efficient in the high energy offset blend with fullerene domains. In all other blends (with low offset or predominantly molecularly mixed domains), nanosecond geminate electron-hole recombination is observed revealing the importance of spatially localized electron-hole pairs (bound CT states) in the electron-hole dynamics. A two-dimensional lattice exciton model was used to simulate the excited state spectrum of a model system as a function of microstructure and energy offset. The results could reproduce the main features of experimental electroluminescence spectra indicating that electron-hole pairs become less bound and more spatially separated upon increasing energy offset and fullerene domain density. Differences between electroluminescence and photoluminescence spectra could be explained by CT photoluminescence being dominated by more-bound states, reflecting geminate recombination processes, while CT electroluminescence preferentially probes less-bound CT states that escape geminate recombination. These results suggest that apparently contradictory studies on electron-hole separation can be explained by the presence of both bound and unbound CT states in the same film, as a result of a range of interface structures.

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