Understanding and Mitigating Interfacial Losses at the Perovskite/C60 Interface for Tandem Solar Cells
Eike Köhnen a, Lea Zimmermann a, Florian Scheler a, Dorothee Menzel a, Maxim Simmonds a, Richard Gundermann b, Thomas Gries a, Edgar Edgar Nandayapa a, Florian Matthies a, Silvia Mariotti a, Daniele Mantione c, Sahil Shah b, Hans Köbler a, Wander Max Bernardes de Araujo a, Julius Petrulevicius d, Arman Mahboubi Soufiani a, Suresh Maniyarasu a, Tadas Malinauskas d, Vytautas Getautis d, Felix Lang b, Lars Korte a, Bernd Stannowski a, Eva Unger a, Antonio Abate a, David Mecerreyes c, Steve Albrecht a
a Helmholtz-Zentrum Berlin für Materialien und Energie, Solar Energy Division, 12489 Berlin, Germany
b Soft Matter Physics and Optoelectronics, Institute of Physics and Astronomy, University of Potsdam, Karl-Liebknecht-Str. 24–25, 14476 Potsdam-Golm, Germany.
c Ikerbasque, Basque Foundation for Science, Bilbao, Bizkaia, 48015, Spain.
d Department of Organic Chemistry, Kaunas University of Technology, Kaunas, Lithuania
Proceedings of MATSUS Fall 2025 Conference (MATSUSFall25)
A2 Molecular Interfaces for Emerging Photovoltaics - #InterPero
València, Spain, 2025 October 20th - 24th
Organizers: Vincent M. Le Corre and Esma Ugur
Invited Speaker, Eike Köhnen, presentation 334
Publication date: 21st July 2025

Perovskite based solar cells (single- and multijunction) have emerged as highly promising candidates for next-generation photovoltaic technologies, offering low-cost fabrication, high efficiencies, and tunable bandgaps. In particular, perovskites with a bandgap of 1.68 eV are ideally suited as top cells in perovskite/silicon tandem solar cells, which gained relevance in both research and industry.

A critical challenge on the path to further efficiency improvements and industrial implementation lies at the interface between the perovskite absorber and the electron transport layer, typically C60. In this talk, I will present a detailed analysis of a loss mechanism that occurs when C₆₀ is exposed to air. This degradation process not only impacts device performance but also has important implications for the design of manufacturing environments and for the accurate evaluation of interfacial engineering strategies: For example, the apparent effectiveness of an interlayer can be misinterpreted if C₆₀ degradation is not properly accounted for.

Furthermore, I will demonstrate two approaches to reduce interfacial losses:
(1) The incorporation of functional interlayers between perovskite and C₆₀, reduce non-radiative recombination by passivation and improved bandalignment.
(2) The use of an evaporable industrially relevant alternative to C₆₀ that shows reduced interfacial losses.

The results presented are relevant for both p-i-n single-junction and perovskite-based multi-junction solar cells and offer concrete strategies for improving device architectures and manufacturing processes-paving the way for stable, scalable, and high-efficiency perovskite photovoltaic technologies.

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