An Amorphous Mesophase Generated by Thermal Annealing for High-Performance Organic Photovoltaic Devices
An Amorphous Mesophase Generated by Thermal Annealing for High-Performance Organic Photovoltaic Devices
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DOI:
10.1002/adma.201200490
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发表时间:
2012-07-10
影响因子:
29.4
通讯作者:
Nakamura, Eiichi
中科院分区:
文献类型:
--
作者:
Tanaka, Hideyuki;Abe, Yoko;Nakamura, Eiichi
Printable thin-film organic photovoltaic (OPV) devices using organofullerene acceptors are attracting tremendous attention with regard to energy and chemical resources issues,[1, 2] and also because of a record performance of 10% power conversion efficiency (PCE) reported recently by Mitsubishi Chemical.[3, 4] Device fabrication often calls for an annealing process, in which the device is exposed to heat or solvent vapor during fabrication to improve its performance.[5, 6] Possible origins of the beneficial effects of thermal and solvent annealing are morphological changes in the active layer, consisting of donor (p-type) or acceptor (n-type), by the removal or introduction of solvent, respectively.[7–19] However, the molecular understanding of such effects remains unclear, because the active layers of OPV devices are generally too ill-defined to carry out detailed studies. We considered that a pin device (the-imeaning an inter-layer consisting of a mixture of donor and acceptor),[20–22] formed using tetrabenzoporphyrin donor (BP; green in Figure 1)[22–24] and silylmethyl [60] fullerene acceptor (SIMEF; blue in Figure 1), would be suitable for molecular-level studies of annealing, because the highly insoluble and thermally stable BP is entirely phase-separated from the fullerene layer.[22] For this study, we developed new fullerene derivatives,(o-anisylsilylmethyl)(phenylsilylmethyl)[60] fullerene (2, SIMEF-Ph, o-An) and its congeners 3 and 4 (SIMEF-Ph, m-and p-An), and studied their crystal structures, thermotropic properties, and photovoltaic performance. We found that heat-driven desolvation of the active layer containing toluene or chlorobenzene co-crystals of 2 creates a new amorphous mesophase that maximizes the short-circuit current density (JSC), as well as the overall device performance. Heating of benzene-containing devices, on the other hand, resulted in a molten phase of 2 and lowering of the fill factor (FF). The active layer made of pristine crystals of 2–4 was found to be inferior. This counterintuitive result suggests that the amorphous mesophase of the fullerene can maximize the BP/fullerene interfacial contact and hence the charge-carrier generation, which appears to be the performance-limiting factor of our pin device, while the molten phase destroys the surface of fullerene layer and decreases the shunt resistance (Rsh).To study the effects of heat-induced desolvation of the active layer, we screened our fullerene derivatives [25] to find that the new SIMEF compound 2 is a suitable substrate because of its ability to co-crystallize with a wide variety of aromatic solvents. On the other hand, the m-and p-An isomers 3 and 4 form only solvent-free crystals. These molecules were synthesized as reported for a simpler analog (Scheme 1).[26] A monosilylmethylfullerene 1 was obtained in 86% isolated yield by the reaction of [60] fullerene in 1, 2-dichlorobenzene with 3 equiv. of a dimethylphenylsilylmethyl Grignard reagent in the presence of 30 equiv. of N, N-dimethylformamide. The second silylmethyl