材料科学
钙钛矿(结构)
单层
光电子学
重组
光致发光
X射线光电子能谱
图层(电子)
自发辐射
工作(物理)
硅
半导体
太阳能电池
化学物理
光伏系统
钙钛矿太阳能电池
纳米技术
化学工程
光学
热力学
物理
化学
工程类
基因
生物
生物化学
激光器
生态学
作者
Jonathan Warby,Fengshuo Zu,Stefan Zeiske,Emilio Gutierrez‐Partida,Lennart Frohloff,Simon Kahmann,Kyle Frohna,Edoardo Mosconi,Eros Radicchi,Felix Lang,Sahil Shah,Francisco Peña‐Camargo,Hannes Hempel,Thomas Unold,Norbert Koch,Ardalan Armin,Filippo De Angelis,Samuel D. Stranks,Dieter Neher,Martin Stolterfoht
标识
DOI:10.1002/aenm.202103567
摘要
Abstract Perovskite semiconductors are an attractive option to overcome the limitations of established silicon based photovoltaic (PV) technologies due to their exceptional opto‐electronic properties and their successful integration into multijunction cells. However, the performance of single‐ and multijunction cells is largely limited by significant nonradiative recombination at the perovskite/organic electron transport layer junctions. In this work, the cause of interfacial recombination at the perovskite/C 60 interface is revealed via a combination of photoluminescence, photoelectron spectroscopy, and first‐principle numerical simulations. It is found that the most significant contribution to the total C 60 ‐induced recombination loss occurs within the first monolayer of C 60 , rather than in the bulk of C 60 or at the perovskite surface. The experiments show that the C 60 molecules act as deep trap states when in direct contact with the perovskite. It is further demonstrated that by reducing the surface coverage of C 60 , the radiative efficiency of the bare perovskite layer can be retained. The findings of this work pave the way toward overcoming one of the most critical remaining performance losses in perovskite solar cells.
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