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5-nm LiF as an Efficient Cathode Buffer Layer in Polymer Solar Cells Through Simply Introducing a C(60) Interlayer

Lithium fluoride (LiF) is an efficient and widely used cathode buffer layer (CBL) in bulk heterojunction polymer solar cells (PSCs). The LiF thickness is normally limited to 1 nm due to its insulting property. Such small thickness is difficult to precise control during thermal deposition, and more i...

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Detalles Bibliográficos
Autores principales: Liu, Xiaodong, Guo, L. Jay, Zheng, Yonghao
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Springer US 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5608655/
https://www.ncbi.nlm.nih.gov/pubmed/28936728
http://dx.doi.org/10.1186/s11671-017-2299-y
Descripción
Sumario:Lithium fluoride (LiF) is an efficient and widely used cathode buffer layer (CBL) in bulk heterojunction polymer solar cells (PSCs). The LiF thickness is normally limited to 1 nm due to its insulting property. Such small thickness is difficult to precise control during thermal deposition, and more importantly, 1-nm-thick LiF cannot provide sufficient protection for the underlying active layer. Herein, we demonstrated the application of a very thick LiF as CBL without sacrificing the device efficiency by simply inserting a C(60) layer between the active layer and LiF layer. The devices with the C(60)/LiF (5 nm) double CBLs exhibit a peak power conversion efficiency (PCE) of 3.65%, which is twofold higher than that (1.79%) of LiF (5 nm)-only device. The superior performance of the C(60)/LiF (5 nm)-based devices is mainly attributed to the good electrical conductivity of the C(60)/LiF (5 nm) bilayer, arising from the intermixing occurred at the C(60)/LiF interface. Besides, the formation of a P3HT/C(60) subcell and the optical spacer effect of C(60) also contribute to the increase in short-circuit current density (J (sc)) of the device. With further increase of LiF thickness to 8 nm, a PCE of 1.10% is attained for the C(60)/LiF-based device, while the negligible photovoltaic performance is observed for the LiF-only device. All in all, our results show that C(60)/LiF bilayer is a promising alternative to LiF single layer due to its high tolerance to the LiF thickness variations. ELECTRONIC SUPPLEMENTARY MATERIAL: The online version of this article (10.1186/s11671-017-2299-y) contains supplementary material, which is available to authorized users.