Proceedings of International Conference on Perovskite Thin Film Photovoltaics and Perovskite Photonics and Optoelectronics (NIPHO23)
DOI: https://doi.org/10.29363/nanoge.nipho.2023.005
Publication date: 3rd April 2023
In back-contact electrode (BCE) perovskite solar cells (PSCs) architecture, the anode, cathode and selective layers coexist in the bottom perovskite interface while the top surface remains exposed. This results in two main advantages; first, it eliminates the parasitic light-absorption losses that are inherent to conventional sandwich-architecture devices and, second, it enables the use of in-situ characterization of the perovskite layer with techniques that are limited by the opaque metal electrode or top selective layers. However, the fabrication methods for these unconventional architectures rely heavily on expensive photolithography, which limits scalability. We present an alternative cost-effective microfabrication technique in which the conventional photolithography process is replaced by microsphere lithography in which a close-packed polystyrene microsphere monolayer acts as the patterning mask for the honeycomb-shaped electrodes.[1] Using microsphere lithography, we achieve highly efficient devices having a stabilized power conversion efficiency (PCE) of 8.6%, twice the reported value using photolithography. Microsphere lithography also enabled the fabrication of the largest back-contact PSC to date, with an active area of 0.75 cm2 and a stabilized PCE of 2.44%. We will provide a comprehensive overview of the particularities of BCE on the device optoelectronic performance and suggest applications for in-situ/operando measurements.
This work was financially supported by the Australian Government through the Australian Renewable Energy Agency (ARENA) the
Australian Centre for Advanced Photovoltaics (ACAP) and the Australian Research Council (ARC, DE220100154). This work was performed in part at the Melbourne Centre for Nanofabrication (MCN) in the Victorian Node of the Australian National Fabrication Facility (ANFF). The authors acknowledge use of facilities within the Monash Centre for Electron Microscopy (MCEM). The authors acknowledge use of facilities within the Flexible Electronics Laboratory (FEL) at the Commonwealth Scientific and Industrial Research Organisation (CSIRO), Clayton site. S.R.R. acknowledges the support from “la Caixa” Foundation (ID 100010434) with fellowship code LCF/BQ/PI20/11760024 and Grant [PID2021-122349OA-I00] funded by MCIN/AEI/ 10.13039/501100011033 and by “ERDF A way of making Europe”.