Combining Efficiency and Stability in Mixed Tin–Lead Perovskite Solar Cells by Capping Grains with an Ultrathin 2D Layer

Mingyang Wei(University of Toronto), Ke Xiao(Collaborative Innovation Center of Advanced Microstructures), Grant Walters(University of Toronto), Renxing Lin(Collaborative Innovation Center of Advanced Microstructures), Yong‐Biao Zhao(University of Toronto), Makhsud I. Saidaminov(University of Toronto), Petar Todorović́(University of Toronto), Andrew Johnston(University of Toronto), Ziru Huang(University of Toronto), Haijie Chen(University of Toronto), Aidong Li(Collaborative Innovation Center of Advanced Microstructures), Jia Zhu(Collaborative Innovation Center of Advanced Microstructures), Zhenyu Yang(University of Toronto), Ya‐Kun Wang(University of Toronto), Andrew H. Proppe(University of Toronto), Shana O. Kelley(University of Toronto), Yi Hou(University of Toronto), Oleksandr Voznyy(University of Toronto), Hairen Tan(Collaborative Innovation Center of Advanced Microstructures), Edward H. Sargent(University of Toronto)
Advanced Materials
February 7, 2020
Cited by 202Open Access
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Abstract

Abstract The development of narrow‐bandgap ( E g ≈ 1.2 eV) mixed tin–lead (Sn–Pb) halide perovskites enables all‐perovskite tandem solar cells. Whereas pure‐lead halide perovskite solar cells (PSCs) have advanced simultaneously in efficiency and stability, achieving this crucial combination remains a challenge in Sn–Pb PSCs. Here, Sn–Pb perovskite grains are anchored with ultrathin layered perovskites to overcome the efficiency‐stability tradeoff. Defect passivation is achieved both on the perovskite film surface and at grain boundaries, an approach implemented by directly introducing phenethylammonium ligands in the antisolvent. This improves device operational stability and also avoids the excess formation of layered perovskites that would otherwise hinder charge transport. Sn–Pb PSCs with fill factors of 79% and a certified power conversion efficiency (PCE) of 18.95% are reported—among the highest for Sn–Pb PSCs. Using this approach, a 200‐fold enhancement in device operating lifetime is achieved relative to the nonpassivated Sn–Pb PSCs under full AM1.5G illumination, and a 200 h diurnal operating time without efficiency drop is achieved under filtered AM1.5G illumination.


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