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Phase Transitions of Thermoelectric TAGS-85

[Image: see text] The alloys (GeTe)(x)(AgSbTe(2))(100–x), commonly known as TAGS-x, are among the best performing p-type thermoelectric materials for the composition range 80 ≤ x ≤ 90 and in the temperature range 200–500 °C. They adopt a rhombohedrally distorted rocksalt structure at room temperatur...

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Detalles Bibliográficos
Autores principales: Kumar, Anil, Vermeulen, Paul A., Kooi, Bart J., Rao, Jiancun, van Eijck, Lambert, Schwarzmüller, Stefan, Oeckler, Oliver, Blake, Graeme R.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2017
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6150666/
https://www.ncbi.nlm.nih.gov/pubmed/29185723
http://dx.doi.org/10.1021/acs.inorgchem.7b02433
Descripción
Sumario:[Image: see text] The alloys (GeTe)(x)(AgSbTe(2))(100–x), commonly known as TAGS-x, are among the best performing p-type thermoelectric materials for the composition range 80 ≤ x ≤ 90 and in the temperature range 200–500 °C. They adopt a rhombohedrally distorted rocksalt structure at room temperature and are reported to undergo a reversible phase transition to a cubic structure at ∼250 °C. However, we show that, for the optimal x = 85 composition (TAGS-85), both the structural and thermoelectric properties are highly sensitive to the initial synthesis method employed. Single-phase rhombohedral samples exhibit the best thermoelectric properties but can only be obtained after an annealing step at 600 °C during initial cooling from the melt. Under faster cooling conditions, the samples obtained are inhomogeneous, containing multiple rhombohedral phases with a range of lattice parameters and exhibiting inferior thermoelectric properties. We also find that when the room-temperature rhombohedral phase is heated, an intermediate trigonal structure containing ordered cation vacancy layers is formed at ∼200 °C, driven by the spontaneous precipitation of argyrodite-type Ag(8)GeTe(6) which alters the stoichiometry of the TAGS-85 matrix. The rhombohedral and trigonal phases of TAGS-85 coexist up to 380 °C, above which a single cubic phase is obtained and the Ag(8)GeTe(6) precipitates redissolve into the matrix. On subsequent cooling a mixture of rhombohedral, trigonal, and Ag(8)GeTe(6) phases is again obtained. Initially single-phase samples exhibit thermoelectric power factors of up to 0.0035 W m(–1) K(–2) at 500 °C, a value that is maintained on subsequent thermal cycling and which represents the highest power factor yet reported for undoped TAGS-85. Therefore, control over the structural homogeneity of TAGS-85 as demonstrated here is essential in order to optimize the thermoelectric performance.