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Charge Distribution in Layered Lanthanide-Doped CuCr(0.99)Ln(0.01)S(2) (Ln = Pr–Tb) Thermoelectric Materials

The charge distribution study of metal atoms in CuCr(0.99)Ln(0.01)S(2) (Ln = Pr–Tb) solid solutions was carried out using X-ray photoelectron spectroscopy (XPS). The analysis of the binding energy of S2p, Cu2p, Cr2p, Ln3d and Ln4d levels allows one to determine the oxidation state of atoms. Copper a...

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Detalles Bibliográficos
Autores principales: Korotaev, Evgeniy V., Syrokvashin, Mikhail M., Filatova, Irina Yu., Sotnikov, Aleksandr V., Kalinkin, Alexandr V.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9785115/
https://www.ncbi.nlm.nih.gov/pubmed/36556553
http://dx.doi.org/10.3390/ma15248747
Descripción
Sumario:The charge distribution study of metal atoms in CuCr(0.99)Ln(0.01)S(2) (Ln = Pr–Tb) solid solutions was carried out using X-ray photoelectron spectroscopy (XPS). The analysis of the binding energy of S2p, Cu2p, Cr2p, Ln3d and Ln4d levels allows one to determine the oxidation state of atoms. Copper atoms were found to be monovalent. Chromium and lanthanide atoms were found to be in the trivalent state. Sulfur atoms were found to be in the divalent state. Cationic substitution was found to occur via an isovalent mechanism of Cr(3+) to Ln(3+). The obtained results were used for the interpretation of the Seebeck coefficient increase for CuCr(0.99)Ln(0.01)S(2) solid solutions in contrast to the initial CuCrS(2) matrix. The largest Seebeck coefficient values of 142 and 148 µV/K were observed at 500 K for CuCr(0.99)Sm(0.01)S(2) and CuCr(0.99)Pr(0.01)S(2), respectively. The obtained values are 1.4 times greater in comparison with those for the initial matrix (105 µV/K).