Improved Optics in Monolithic Perovskite/Silicon Tandem Solar Cells with a Nanocrystalline Silicon Recombination Junction

Florent Sahli(École Polytechnique Fédérale de Lausanne), Brett A. Kamino(Swiss Center for Electronics and Microtechnology (Switzerland)), Jérémie Werner(École Polytechnique Fédérale de Lausanne), Matthias Bräuninger(École Polytechnique Fédérale de Lausanne), Bertrand Paviet‐Salomon(Swiss Center for Electronics and Microtechnology (Switzerland)), Loris Barraud(Swiss Center for Electronics and Microtechnology (Switzerland)), R. Monnard(École Polytechnique Fédérale de Lausanne), Johannes P. Seif(École Polytechnique Fédérale de Lausanne), Andrea Tomasi(École Polytechnique Fédérale de Lausanne), Quentin Jeangros(University of Basel), Aïcha Hessler‐Wyser(École Polytechnique Fédérale de Lausanne), Stefaan De Wolf(École Polytechnique Fédérale de Lausanne), Matthieu Despeisse(Swiss Center for Electronics and Microtechnology (Switzerland)), Sylvain Nicolay(Swiss Center for Electronics and Microtechnology (Switzerland)), Bjoern Niesen(Swiss Center for Electronics and Microtechnology (Switzerland)), Christophe Ballif(Swiss Center for Electronics and Microtechnology (Switzerland))
Advanced Energy Materials
October 9, 2017
Cited by 252Open Access
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Abstract

Abstract Perovskite/silicon tandem solar cells are increasingly recognized as promi­sing candidates for next‐generation photovoltaics with performance beyond the single‐junction limit at potentially low production costs. Current designs for monolithic tandems rely on transparent conductive oxides as an intermediate recombination layer, which lead to optical losses and reduced shunt resistance. An improved recombination junction based on nanocrystalline silicon layers to mitigate these losses is demonstrated. When employed in monolithic perovskite/silicon heterojunction tandem cells with a planar front side, this junction is found to increase the bottom cell photocurrent by more than 1 mA cm −2 . In combination with a cesium‐based perovskite top cell, this leads to tandem cell power‐conversion efficiencies of up to 22.7% obtained from J – V measurements and steady‐state efficiencies of up to 22.0% during maximum power point tracking. Thanks to its low lateral conductivity, the nanocrystalline silicon recombination junction enables upscaling of monolithic perovskite/silicon heterojunction tandem cells, resulting in a 12.96 cm 2 monolithic tandem cell with a steady‐state efficiency of 18%.


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