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Adjusting Interfacial Chemistry and Electronic Properties of Photovoltaics Based on a Highly Pure Sb(2)S(3) Absorber by Atomic Layer Deposition

[Image: see text] The combination of oxide and heavier chalcogenide layers in thin film photovoltaics suffers limitations associated with oxygen incorporation and sulfur deficiency in the chalcogenide layer or with a chemical incompatibility which results in dewetting issues and defect states at the...

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Detalles Bibliográficos
Autores principales: Büttner, Pascal, Scheler, Florian, Pointer, Craig, Döhler, Dirk, Barr, Maïssa K. S., Koroleva, Aleksandra, Pankin, Dmitrii, Hatada, Ruriko, Flege, Stefan, Manshina, Alina, Young, Elizabeth R., Mínguez-Bacho, Ignacio, Bachmann, Julien
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2019
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6931240/
https://www.ncbi.nlm.nih.gov/pubmed/31894204
http://dx.doi.org/10.1021/acsaem.9b01721
Descripción
Sumario:[Image: see text] The combination of oxide and heavier chalcogenide layers in thin film photovoltaics suffers limitations associated with oxygen incorporation and sulfur deficiency in the chalcogenide layer or with a chemical incompatibility which results in dewetting issues and defect states at the interface. Here, we establish atomic layer deposition (ALD) as a tool to overcome these limitations. ALD allows one to obtain highly pure Sb(2)S(3) light absorber layers, and we exploit this technique to generate an additional interfacial layer consisting of 1.5 nm ZnS. This ultrathin layer simultaneously resolves dewetting and passivates defect states at the interface. We demonstrate via transient absorption spectroscopy that interfacial electron recombination is one order of magnitude slower at the ZnS-engineered interface than hole recombination at the Sb(2)S(3)/P3HT interface. The comparison of solar cells with and without oxide incorporation in Sb(2)S(3), with and without the ultrathin ZnS interlayer, and with systematically varied Sb(2)S(3) thickness provides a complete picture of the physical processes at work in the devices.