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 29:28 (2019)

Authors:

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

Inverted perovskite solar cells with air stable diketopyrrolopyrrole-based electron transport layer

Solar Energy Elsevier 186 (2019) 9-16

Authors:

Shikha Sharma, Nobuya Sakai, Suman Ray, Satyaprasad P Senanayak, Henning Sirringhaus, Henry J Snaith, Satish Patil

Overcoming zinc oxide interface instability with a methylammonium-free perovskite for high performance solar cells

Advanced Functional Materials Wiley 29:47 (2019) 1900466

Authors:

Kelly Schutt, P Nayak, A Ramadan, B Wenger, Y-H Lin, H Snaith

Abstract:

Perovskite solar cells have achieved the highest power conversion efficiencies on metal oxide n‐type layers, including SnO2 and TiO2. Despite ZnO having superior optoelectronic properties to these metal oxides, such as improved transmittance, higher conductivity, and closer conduction band alignment to methylammonium (MA)PbI3, ZnO is largely overlooked due to a chemical instability when in contact with metal halide perovskites, which leads to rapid decomposition of the perovskite. While surface passivation techniques have somewhat mitigated this instability, investigations as to whether all metal halide perovskites exhibit this instability with ZnO are yet to be undertaken. Experimental methods to elucidate the degradation mechanisms at ZnO–MAPbI3 interfaces are developed. By substituting MA with formamidinium (FA) and cesium (Cs), the stability of the perovskite–ZnO interface is greatly enhanced and it is found that stability compares favorably with SnO2‐based devices after high‐intensity UV irradiation and 85 °C thermal stressing. For devices comprising FA‐ and Cs‐based metal halide perovskite absorber layers on ZnO, a 21.1% scanned power conversion efficiency and 18% steady‐state power output are achieved. This work demonstrates that ZnO appears to be as feasible an n‐type charge extraction layer as SnO2, with many foreseeable advantages, provided that MA cations are avoided.

Carboxylate-Substituted Polythiophenes for Efficient Fullerene-Free Polymer Solar Cells: The Effect of Chlorination on Their Properties

Macromolecules American Chemical Society (ACS) 52:12 (2019) 4464-4474

Authors:

Qi Wang, Miaomiao Li, Xiaowei Zhang, Yunpeng Qin, Junke Wang, Jidong Zhang, Jianhui Hou, René AJ Janssen, Yanhou Geng

Charge-carrier dynamics, mobilities and diffusion lengths of 2D-3D hybrid butylammonium-caesium-formamidinium lead halide perovskites

Advanced Functional Materials Wiley (2019)

Authors:

Leonardo Buizza, Timothy Crothers, Zhiping Wang, Patel Jay, R Milot, Henry Snaith, Michael Johnston, Laura Herz

Abstract:

Perovskite solar cells (PSCs) have improved dramatically over the past decade, increasing in efficiency and gradually overcoming hurdles of temperature‐ and humidity‐induced instability. Materials that combine high charge‐carrier lifetimes and mobilities, strong absorption, and good crystallinity of 3D perovskites with the hydrophobic properties of 2D perovskites have become particularly promising candidates for use in solar cells. In order to fully understand the optoelectronic properties of these 2D–3D hybrid systems, the hybrid perovskite BAx(FA0.83Cs0.17)1‐xPb(I0.6Br0.4)3 is investigated across the composition range 0 ≤ x ≤ 0.8. Small amounts of butylammonium (BA) are found that help to improve crystallinity and appear to passivate grain boundaries, thus reducing trap‐mediated charge‐carrier recombination and enhancing charge‐carrier mobilities. Excessive amounts of BA lead to poor crystallinity and inhomogeneous film formation, greatly reducing effective charge‐carrier mobility. For low amounts of BA, the benevolent effects of reduced recombination and enhanced mobilities lead to charge‐carrier diffusion lengths up to 7.7 µm for x = 0.167. These measurements pave the way for highly efficient, highly stable PSCs and other optoelectronic devices based on 2D–3D hybrid materials.