4.8 Article

Fullerene-Liquid-Crystal-Induced Micrometer-Scale Charge-Carrier Diffusion in Organic Bulk Heterojunction

Journal

ADVANCED MATERIALS
Volume 35, Issue 9, Pages -

Publisher

WILEY-V C H VERLAG GMBH
DOI: 10.1002/adma.202210463

Keywords

charge-carrier diffusion length; fullerene liquid crystals; high-efficiency thick-film devices; organic solar cells

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The introduction of a fullerene liquid crystal, F1, into the active layer of organic solar cells can effectively increase the charge-carrier diffusion length and improve the power conversion efficiency.
The short charge-carrier diffusion length (L-D) (100-300 nm) in organic bulk heterojunction (BHJ) impedes the further improvement in power conversion efficiency (PCE) of organic solar cells (OSCs), especially for thick-film (>400 nm) devices matching with industrial solution processing. Here a facile method is developed to efficiently increase L-D and then improve PCEs of OSCs via introducing a fullerene liquid crystal, F1, into the active layer. F1 combines the inherent high electron mobility of fullerene and strong self-assembly capacity of liquid crystal, providing a fast channel for charge-carrier transport and reducing energetic disorder and trap density in BHJ film via enhancing crystallization. Typically, in PM6:Y6:F1 BHJ, the enhanced charge-carrier mobility (>10(-2) cm(-2) V-1 s(-1)) and prolonged charge-carrier lifetime (55.3 mu s) are acquired to realize the record L-D of 1.6 or 2.4 mu m for electron or hole, respectively, which are much higher than those of the PM6:Y6 binary sample and comparable to or even better than those values reported for some inorganic/hybrid materials, such as CuInxGa(1-x)Se2 (CIGS) and perovskite thin films. Benefitting from the micrometer-scale L-D, the PM6:Y6:F1 ternary OSCs sustain a remarkable PCE of 15.23% with the active layer thickness approaching 500 nm.

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