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Phase Transitions of Thermoelectric TAGS-85.
Kumar, Anil; Vermeulen, Paul A; Kooi, Bart J; Rao, Jiancun; van Eijck, Lambert; Schwarzmüller, Stefan; Oeckler, Oliver; Blake, Graeme R.
  • Kumar A; Zernike Institute for Advanced Materials, University of Groningen , Nijenborgh 4, 9747AG Groningen, The Netherlands.
  • Vermeulen PA; Zernike Institute for Advanced Materials, University of Groningen , Nijenborgh 4, 9747AG Groningen, The Netherlands.
  • Kooi BJ; Zernike Institute for Advanced Materials, University of Groningen , Nijenborgh 4, 9747AG Groningen, The Netherlands.
  • Rao J; School of Materials Science and Engineering, Harbin Institute of Technology , 150001 Harbin, P. R. China.
  • van Eijck L; AIM Lab, Maryland NanoCenter, University of Maryland , College Park, Maryland 20742, United States.
  • Schwarzmüller S; Department of Radiation Science and Technology, Delft University of Technology , Mekelweg 15, 2629JB Delft, The Netherlands.
  • Oeckler O; Institute for Mineralogy, Crystallography and Materials Science, Leipzig University , Scharnhorststrasse 20, 04275 Leipzig, Germany.
  • Blake GR; Institute for Mineralogy, Crystallography and Materials Science, Leipzig University , Scharnhorststrasse 20, 04275 Leipzig, Germany.
Inorg Chem ; 56(24): 15091-15100, 2017 Dec 18.
Article en En | MEDLINE | ID: mdl-29185723
The alloys (GeTe)x(AgSbTe2)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 Ag8GeTe6 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 Ag8GeTe6 precipitates redissolve into the matrix. On subsequent cooling a mixture of rhombohedral, trigonal, and Ag8GeTe6 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.