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Improvement of thermoelectric performance of copper-deficient compounds Cu(2.5+δ)In(4.5)Te(8) (δ = 0–0.15) due to a degenerate impurity band and ultralow lattice thermal conductivity

Cu–In–Te ternary chalcogenides have unique crystal and band structures; hence they have received much attention in thermoelectrics. In this work we have observed an enhancement in Hall carrier concentration (n(H)) and ultralow lattice thermal conductivity (κ(L)) when Cu was added to ternary Cu(2.5+δ...

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Detalles Bibliográficos
Autores principales: Ren, Ting, Ying, Pengzhan, Cai, Gemei, Li, Xiaoyan, Han, Zhongkang, Min, Lei, Cui, Jiaolin
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9083297/
https://www.ncbi.nlm.nih.gov/pubmed/35539978
http://dx.doi.org/10.1039/c8ra05188g
Descripción
Sumario:Cu–In–Te ternary chalcogenides have unique crystal and band structures; hence they have received much attention in thermoelectrics. In this work we have observed an enhancement in Hall carrier concentration (n(H)) and ultralow lattice thermal conductivity (κ(L)) when Cu was added to ternary Cu(2.5+δ)In(4.5)Te(8) (δ = 0–0.15) compounds. The enhancement in n(H) is attributed to a degenerate impurity band at the G point in the valence band maximum (VBM), while the extremely low κ(L) results from the increased lattice disorder. We thus obtained the minimum κ(L) value of only 0.23 W K(−1) m(−1) in the sample at δ = 0.1 and 820 K, which is in good agreement with the calculation using the Callaway model. The highest thermoelectric figure of merit ZT is 0.84 for the material at δ = 0.1, which is about 0.38 higher than that of the pristine Cu(2.5)In(4.5)Te(8).