Light induced degradation in mixed-halide perovskites

Journal of Materials Chemistry C Royal Society of Chemistry (RSC) 7:30 (2019) 9326-9334

Authors:

Shuai Ruan, Maciej-Adam Surmiak, Yinlan Ruan, David P McMeekin, Heike Ebendorff-Heidepriem, Yi-Bing Cheng, Jianfeng Lu, Christopher R McNeill

LiTFSI‐Free Spiro‐OMeTAD‐Based Perovskite Solar Cells with Power Conversion Efficiencies Exceeding 19%

Advanced Energy Materials Wiley 9:32 (2019)

Authors:

Boer Tan, Sonia R Raga, Anthony SR Chesman, Sebastian O Fürer, Fei Zheng, David P McMeekin, Liangcong Jiang, Wenxin Mao, Xiongfeng Lin, Xiaoming Wen, Jianfeng Lu, Yi‐Bing Cheng, Udo Bach

Oxalic Acid Enabled Emission Enhancement and Continuous Extraction of Chloride from Cesium Lead Chloride/Bromide Perovskite Nanocrystals.

Small (Weinheim an der Bergstrasse, Germany) 15:34 (2019) e1901828

Authors:

Shixun Wang, Xinyu Shen, Yu Zhang, Xingwei Zhuang, Dingke Xue, Xiangtong Zhang, Jinlei Wu, Jinyang Zhu, Zhifeng Shi, Stephen V Kershaw, William W Yu, Andrey L Rogach

Abstract:

All-inorganic cesium lead halide perovskite nanocrystals (NCs) have demonstrated excellent optical properties and an encouraging potential for optoelectronic applications; however, mixed-halide perovskites, especially CsPb(Cl/Br)3 NCs, still show lower photoluminescence quantum yields (PL QY) than the corresponding single-halide materials. Herein, anhydrous oxalic acid is used to post-treat CsPb(Cl/Br)3 NCs in order to initially remove surface defects and halide vacancies, and thus, to improve their PL QY from 11% to 89% for the emission of 451 nm. Furthermore, due to the continuous chelating reaction with the oxalate ion, chloride anions from the mixed-halide CsPb(Cl/Br)3 perovskite NCs could be extracted, and green emitting CsPbBr3 NCs with PL QY of 85% at 511 nm emission are obtained. Besides being useful to improve the emission of CsPb(Cl/Br)3 NCs, the oxalic acid treatment strategy introduced here provides a further tool to adjust the distribution of halide anions in mixed-halide perovskites without using any halide additives.

Crystallographic characterization of Er 3 N@C 2n (2 n = 80, 82, 84, 88): the importance of a planar Er 3 N cluster

Nanoscale Royal Society of Chemistry (RSC) 11:28 (2019) 13415-13422

Authors:

Shuaifeng Hu, Pei Zhao, Wangqiang Shen, Pengyuan Yu, Wenhuan Huang, Masahiro Ehara, Yunpeng Xie, Takeshi Akasaka, Xing Lu

Impurity tracking enables enhanced control and reproducibility of hybrid perovskite vapour deposition

ACS Applied Materials and Interfaces American Chemical Society 11:32 (2019) 28851-28857

Authors:

Juliane Borchert, I Levchuk, Lavina Snoek, Mathias Rothmann, Renée Haver, Henry Snaith, CJ Brabec, Laura Herz, Michael Johnston

Abstract:

Metal halide perovskite semiconductors have the potential to enable low-cost, flexible and efficient solar cells for a wide range of applications. Physical vapour deposition by co-evaporation of precursors is a method which results in very smooth and pin-hole-free perovskite thin films and allows excellent control over film thickness and composition. However, for a deposition method to become industrially scalable, reproducible process control and high device yields are essential. Unfortunately, to date the control and reproducibility of evaporating organic precursors such as methylammonium iodide (MAI) has proved extremely challenging. We show that the established method of controlling the evaporation-rate of MAI with quartz micro balances (QMBs) is critically sensitive to the concentration of the impurities MAH2PO3 and MAH2PO2 that are usually present in MAI after synthesis. Therefore, controlling the deposition rate of MAI with QMBs is unreliable since the concentration of such impurities typically varies from MAI batch-to-batch and even during the course of a deposition. However once reliable control of MAI deposition is achieved, we find that the presence of precursor impurities during perovskite deposition does not degrade solar cell performance. Our results indicate that as long as precursor deposition rates are well controlled, physical vapour deposition will allow high solar cell device yields even if the purity of precursors change from run to run.