Bias‐Dependent Quantum Efficiency Reveals Recombination Pathways in Thin Film Solar Cells

Abstract Identifying where recombination predominantly occurs—whether at the front interface, back interface, or throughout the bulk—is crucial for optimizing CdSeTe solar cells and many other photovoltaic device architectures. Here, a simple and effective diagnostic is demonstrated: measuring external quantum efficiency (QE) under varying forward biases. The drift–diffusion simulations reveal that each recombination pathway leaves a distinct bias‐induced signature in the normalized QE: a progressive drop at long wavelengths for back‐limited devices, a short‐wavelength decline for front‐limited devices, and a relatively uniform decrease across all wavelengths for bulk‐limited devices. These predictions are validated with experiments on As‐doped and Cu‐doped CdSeTe devices, with and without passivation layers or different front buffers. In each case, the observed bias‐dependent QE spectral changes align with the simulated recombination map. Because this method uses standard QE instrumentation, it offers a broadly accessible and cost‐efficient means to diagnose recombination pathways—extending beyond CdSeTe to other thin‐film and emerging solar cell technologies. By pinpointing recombination bottlenecks, researchers and manufacturers can strategically refine doping profiles, passivation schemes, and interface designs to further improve device performance.

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Institutions

Publication Details

Journal
Advanced Energy Materials
Published
2025-07-21
DOI
https://doi.org/10.1002/aenm.202501709
Citations
4
Primary Topic
Chalcogenide Semiconductor Thin Films
Type
article
Field-Weighted Citation Impact
2.92

Funders

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article

Bias‐Dependent Quantum Efficiency Reveals Recombination Pathways in Thin Film Solar Cells

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4 citations
Advanced Energy Materials
Chalcogenide Semiconductor Thin Films
2.92
article

Bias‐Dependent Quantum Efficiency Reveals Recombination Pathways in Thin Film Solar Cells

Tyler Brau, Michael J. Heben, Zachary W. Zawisza, Deng‐Bing Li, Scott Lambright, Sabin Neupane, Vijay C. Karade, Nadeesha Katakumbura, Abasi Abudulimu, Scott Wenner, Randy J. Ellingson, Aesha P. Patel, Ebin Bastola, Yanfa Yan, Chungho Lee, Adam B. Phillips, Manoj K. Jamarkkatel
article en
4 citations

Abstract

Abstract Identifying where recombination predominantly occurs—whether at the front interface, back interface, or throughout the bulk—is crucial for optimizing CdSeTe solar cells and many other photovoltaic device architectures. Here, a simple and effective diagnostic is demonstrated: measuring external quantum efficiency (QE) under varying forward biases. The drift–diffusion simulations reveal that each recombination pathway leaves a distinct bias‐induced signature in the normalized QE: a progressive drop at long wavelengths for back‐limited devices, a short‐wavelength decline for front‐limited devices, and a relatively uniform decrease across all wavelengths for bulk‐limited devices. These predictions are validated with experiments on As‐doped and Cu‐doped CdSeTe devices, with and without passivation layers or different front buffers. In each case, the observed bias‐dependent QE spectral changes align with the simulated recombination map. Because this method uses standard QE instrumentation, it offers a broadly accessible and cost‐efficient means to diagnose recombination pathways—extending beyond CdSeTe to other thin‐film and emerging solar cell technologies. By pinpointing recombination bottlenecks, researchers and manufacturers can strategically refine doping profiles, passivation schemes, and interface designs to further improve device performance.

Advanced Energy MaterialsVol. 15(36)
First Solar (United States) (US), University of Toledo (US)
U.S. Department of Defense, U.S. Department of Energy, Office of Energy Efficiency and Renewable Energy, Solar Energy Technologies Office, Office of Energy Efficiency, National Renewable Energy Laboratory, Air Force Research Laboratory
Openalex Percentile: Top 9%
Chalcogenide Semiconductor Thin Films
2.92
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