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Thermoelectric Properties of Bismuth Telluride Thin Films Electrodeposited from a Nonaqueous Solution

[Image: see text] We report the thermoelectric properties of Bi(2)Te(3) thin films electrodeposited from the weakly coordinating solvent dichloromethane (CH(2)Cl(2)). It was found that the oxidation of porous films is significant, causing the degradation of its thermoelectric properties. We show tha...

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Detalles Bibliográficos
Autores principales: Cicvarić, Katarina, Meng, Lingcong, Newbrook, Daniel W., Huang, Ruomeng, Ye, Sheng, Zhang, Wenjian, Hector, Andrew L., Reid, Gillian, Bartlett, Philip N., de Groot, C. H. Kees
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2020
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7315573/
https://www.ncbi.nlm.nih.gov/pubmed/32596605
http://dx.doi.org/10.1021/acsomega.0c01284
Descripción
Sumario:[Image: see text] We report the thermoelectric properties of Bi(2)Te(3) thin films electrodeposited from the weakly coordinating solvent dichloromethane (CH(2)Cl(2)). It was found that the oxidation of porous films is significant, causing the degradation of its thermoelectric properties. We show that the morphology of the film can be improved drastically by applying a short initial nucleation pulse, which generates a large number of nuclei, and then growing the nuclei by pulsed electrodeposition at a much lower overpotential. This significantly reduces the oxidation of the films as smooth films have a smaller surface-to-volume ratio and are less prone to oxidation. X-ray photoelectron spectroscopy (XPS) shows that those films with Te(O) termination show a complete absence of oxygen below the surface layer. A thin film transfer process was developed using polystyrene as a carrier polymer to transfer the films from the conductive TiN to an insulating layer for thermoelectrical characterization. Temperature-dependent Seebeck measurements revealed a room-temperature coefficient of −51.7 μV/K growing to nearly −100 μV/K at 520 °C. The corresponding power factor reaches a value of 88.2 μW/mK(2) at that temperature.