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Analysis of the Voltage Losses in CZTSSe Solar Cells of Varying Sn Content

[Image: see text] The performance of kesterite (Cu(2)ZnSn(S,Se)(4), CZTSSe) solar cells is hindered by low open circuit voltage (V(oc)). The commonly used metric for V(oc)-deficit, namely, the difference between the absorber band gap and qV(oc), is not well-defined for compositionally complex absorb...

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Detalles Bibliográficos
Autores principales: Azzouzi, Mohammed, Cabas-Vidani, Antonio, Haass, Stefan G., Röhr, Jason A., Romanyuk, Yaroslav E., Tiwari, Ayodhya N., Nelson, Jenny
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2019
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6558638/
https://www.ncbi.nlm.nih.gov/pubmed/31070031
http://dx.doi.org/10.1021/acs.jpclett.9b00506
Descripción
Sumario:[Image: see text] The performance of kesterite (Cu(2)ZnSn(S,Se)(4), CZTSSe) solar cells is hindered by low open circuit voltage (V(oc)). The commonly used metric for V(oc)-deficit, namely, the difference between the absorber band gap and qV(oc), is not well-defined for compositionally complex absorbers like kesterite where the bandgap is hard to determine. Here, nonradiative voltage losses are analyzed by measuring the radiative limit of V(oc), using external quantum efficiency (EQE) and electroluminescence (EL) spectra, without relying on precise knowledge of the bandgap. The method is applied to a series of Cu(2)ZnSn(S,Se)(4) devices with Sn content variation from 27.6 to 32.9 at. % and a corresponding V(oc) range from 423 to 465 mV. Surprisingly, the lowest nonradiative loss, and hence the highest external luminescence efficiency (QE(LED)), were obtained for the device with the lowest V(oc). The trend is assigned to better interface quality between absorber and CdS buffer layer at lower Sn content.