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Cubic AgMnSbTe3 Semiconductor with a High Thermoelectric Performance
Author(s) -
Yubo Luo,
Tian Xu,
Zheng Ma,
Dan Zhang,
Zhongnan Guo,
Qinghui Jiang,
Junyou Yang,
Qingyu Yan,
Mercouri G. Kanatzidis
Publication year - 2021
Publication title -
journal of the american chemical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 7.115
H-Index - 612
eISSN - 1520-5126
pISSN - 0002-7863
DOI - 10.1021/jacs.1c07522
Subject(s) - chemistry , semiconductor , band gap , thermoelectric effect , valence (chemistry) , condensed matter physics , band offset , lattice (music) , seebeck coefficient , electronic band structure , crystallography , valence band , thermodynamics , materials science , optoelectronics , physics , organic chemistry , acoustics
The reaction of MnTe with AgSbTe 2 in an equimolar ratio (ATMS) provides a new semiconductor, AgMnSbTe 3 . AgMnSbTe 3 crystallizes in an average rock-salt NaCl structure with Ag, Mn, and Sb cations statistically occupying the Na sites. AgMnSbTe 3 is a p-type semiconductor with a narrow optical band gap of ∼0.36 eV. A pair distribution function analysis indicates that local distortions are associated with the location of the Ag atoms in the lattice. Density functional theory calculations suggest a specific electronic band structure with multi-peak valence band maxima prone to energy convergence. In addition, Ag 2 Te nanograins precipitate at grain boundaries of AgMnSbTe 3 . The energy offset of the valence band edge between AgMnSbTe 3 and Ag 2 Te is ∼0.05 eV, which implies that Ag 2 Te precipitates exhibit a negligible effect on the hole transmission. As a result, ATMS exhibits a high power factor of ∼12.2 μW cm -1 K -2 at 823 K, ultralow lattice thermal conductivity of ∼0.34 W m -1 K -1 (823 K), high peak ZT of ∼1.46 at 823 K, and high average ZT of ∼0.87 in the temperature range of 400-823 K.

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