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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...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2018
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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 |
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). |
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