Crystallographic Characterization of Er2C2@C80–88: Cluster Stretching with Cage Elongation

Inorganic Chemistry American Chemical Society (ACS) 59:3 (2020) 1940-1946

Authors:

Shuaifeng Hu, Pei Zhao, Wangqiang Shen, Masahiro Ehara, Yunpeng Xie, Takeshi Akasaka, Xing Lu

Light absorption and recycling in hybrid metal halide perovskites photovoltaic devices

Advanced Energy Materials Wiley 10:10 (2020) 1903653

Authors:

Jay Patel, Adam Wright, Kilian Lohmann, Kun Peng, Chelsea Xia, James Ball, Nakita Noel, Timothy Crothers, Henry Snaith, Laura Herz, Michael Johnston

Abstract:

The production of highly efficient single‐ and multijunction metal halide perovskite (MHP) solar cells requires careful optimization of the optical and electrical properties of these devices. Here, precise control of CH3NH3PbI3 perovskite layers is demonstrated in solar cell devices through the use of dual source coevaporation. Light absorption and device performance are tracked for incorporated MHP films ranging from ≈67 nm to ≈1.4 µm thickness and transfer‐matrix optical modeling is utilized to quantify optical losses that arise from interference effects. Based on these results, a device with 19.2% steady‐state power conversion efficiency is achieved through incorporation of a perovskite film with near‐optimum predicted thickness (≈709 nm). Significantly, a clear signature of photon reabsorption is observed in perovskite films that have the same thickness (≈709 nm) as in the optimized device. Despite the positive effect of photon recycling associated with photon reabsorption, devices with thicker (>750 nm) MHP layers exhibit poor performance owing to competing nonradiative charge recombination in a “dead‐volume” of MHP. Overall, these findings demonstrate the need for fine control over MHP thickness to achieve the highest efficiency cells, and accurate consideration of photon reabsorption, optical interference, and charge transport properties.

High Responsivity and Response Speed Single‐Layer Mixed‐Cation Lead Mixed‐Halide Perovskite Photodetectors Based on Nanogap Electrodes Manufactured on Large‐Area Rigid and Flexible Substrates

Advanced Functional Materials Wiley 30:6 (2020)

Authors:

Dimitra G Georgiadou, Yen‐Hung Lin, Jongchul Lim, Sinclair Ratnasingham, Martyn A McLachlan, Henry J Snaith, Thomas D Anthopoulos

Low-temperature solution-combustion-processed Zn-Doped Nb2O5 as an electron transport layer for efficient and stable perovskite solar cells

Journal of Power Sources Elsevier 448 (2020) 227419

Authors:

Xiaoqin Ye, Hanbing Ling, Rui Zhang, Zhiyue Wen, Shuaifeng Hu, Takeshi Akasaka, Jiangbin Xia, Xing Lu

CsI-antisolvent adduct formation in all-inorganic metal halide perovskites

Advanced Energy Materials Wiley 10:9 (2020) 1903365

Authors:

Taylor Moot, Ashley Marshall, Lance Wheeler, Severin Habisreutinger, Tracey Schloemer, Caleb C Boyd, Desislava Dikova, Greg Pach, Michael McGehee, Abhijit Hazarika, Henry Snaith, Joseph Luther

Abstract:

The excellent optoelectronic properties demonstrated by hybrid organic/inorganic metal halide perovskites are all predicated on precisely controlling the exact nucleation and crystallization dynamics that occur during film formation. In general, high‐performance thin films are obtained by a method commonly called solvent engineering (or antisolvent quench) processing. The solvent engineering method removes excess solvent, but importantly leaves behind solvent that forms chemical adducts with the lead‐halide precursor salts. These adduct‐based precursor phases control nucleation and the growth of the polycrystalline domains. There has not yet been a comprehensive study comparing the various antisolvents used in different perovskite compositions containing cesium. In addition, there have been no reports of solvent engineering for high efficiency in all‐inorganic perovskites such as CsPbI3. In this work, inorganic perovskite composition CsPbI3 is specifically targeted and unique adducts formed between CsI and precursor solvents and antisolvents are found that have not been observed for other A‐site cation salts. These CsI adducts control nucleation more so than the PbI2–dimethyl sulfoxide (DMSO) adduct and demonstrate how the A‐site plays a significant role in crystallization. The use of methyl acetate (MeOAc) in this solvent engineering approach dictates crystallization through the formation of a CsI–MeOAc adduct and results in solar cells with a power conversion efficiency of 14.4%.