ALD Zinc Tin Oxide Buffers for Chalcopyrite Solar Cells: Electrical Barriers and Conduction Band Cliffs
Boaz Koren, Francesco Lodola, Zhuangyi Zhou, Trong Tien Le, Kulwinder Kaur, Simon Backes, Michele Melchiorre, Susanne Siebentritt

TL;DR
This study explores atomic layer deposition of ZnSnO as a buffer layer in chalcopyrite solar cells, analyzing how tin content influences conduction band offsets and impacts device performance.
Contribution
It demonstrates how varying tin content in ZnSnO buffers affects conduction band alignment and electron transport in chalcopyrite solar cells.
Findings
Low tin buffers create conduction band cliffs reducing voltage.
High tin buffers introduce electron transport barriers, lowering fill factor.
Sn content correlates positively with the buffer's conduction band minimum.
Abstract
Sulfide chalcopyrite, Cu(In,Ga)S2, having wide bandgap (larger than 1.5 eV), favorable optoelectronic properties, and high stability, is a promising top-cell absorber for tandem applications. Adapting device structures optimized for 1.0 - 1.2 eV absorbers to wide bandgap absorbers requires modification of the buffer layer. This work investigates atomic layer deposition of ZnSnO as an alternative buffer layer to conventional CdS. A critical parameter for bufferperformance is the conduction band offsets on both sides of the buffer. To investigate these buffers we electrically characterize solar cells utilizing different compositions of ZnSnO. The Sn/(Sn+Zn) atomic ratio is controlled by the ratio of ZnO to SnO cycles during atomic layer deposition. Solar cells were fabricated utilizing CuInSe2, Cu(In,Ga)Se2, and Cu(In,Ga)S2 absorbers, allowing cross-comparison with a variety of conduction…
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