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Understanding the Interfacial Energy Structure and Electron Extraction Process in Inverted Organic Solar Cells with <scp>Phosphine‐Doped</scp> Cathode Interlayers

Yi YangState Key Laboratory of Polymer Physics and Chemistry, Beijing National Laboratory for Molecular Sciences Institute of Chemistry, Chinese Academy of Sciences Beijing 100190 ChinaJingwen WangState Key Laboratory of Polymer Physics and Chemistry, Beijing National Laboratory for Molecular Sciences Institute of Chemistry, Chinese Academy of Sciences Beijing 100190 ChinaYang XiaoState Key Laboratory of Polymer Physics and Chemistry, Beijing National Laboratory for Molecular Sciences Institute of Chemistry, Chinese Academy of Sciences Beijing 100190 ChinaBowei XuState Key Laboratory of Chemical Resource Engineering, College of Materials Science and Engineering Beijing University of Chemical Technology Beijing 100029 ChinaJianhui HouState Key Laboratory of Polymer Physics and Chemistry, Beijing National Laboratory for Molecular Sciences Institute of Chemistry, Chinese Academy of Sciences Beijing 100190 China
2024en
ABI

Аннотация

Comprehensive Summary Cathode interlayers (CILs) play an essential role in achieving efficient organic solar cells (OSCs). However, the electronic structure at the electrode/CIL/active layer interfaces and the underlying mechanisms for electron collection remain unclear, which becomes a major obstacle to develop high‐performance CILs. Herein, we investigate the relationship of the electron collection abilities of four cross‐linked and n ‐doped CILs ( c ‐NDI:P 0 , c ‐NDI:P 1 , c ‐NDI:P 2 , c ‐NDI:P 3 ) with their electronic structure of space charge region at heterojunction interface. By accurately calculating the depletion region width according to the barrier height, doping density and permittivity, we put forward that the optimal thickness of CIL should be consistent with the depletion region width to realize the minimum energy loss. As a result, the depletion region width is largely reduced from 13 nm to 0.8 nm at the indium tin oxide (ITO)/ c ‐NDI:P 0 interface, resulting in a decent PCE of 17.7% for the corresponding inverted OSCs.

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