Pressure induced amorphization and recrystallization of thermoelectric material AgSbTe2
Baihong Sun1,2,3, Sergei Grazhdannikov2, Yaron Amouyal*2, Elissaios Stavrou*1,2,3
1Guangdong Technion-Institute of Technology GTIIT, Department of Material Science and Engineering, Shantou, People’s republic of China
2Technion-Institute of Technology, Department of Material Science and Engineering, Haifa, State of Israel
3Guangdong Provincial Key Laboratory of Materials and Technologies for Energy Conversion, Shantou, People’s republic of China
sun06604@gtiit.edu.cn, amouyal@technion.ac.il, elissaios.stavrou@gtiit.edu.cn
Thermoelectric (TE) materials, which can directly convert thermal energy to produce electrical energy and vice-versa, emerging with considerable promise. The thermoelectric performance of material is characterized by dimensionless figure of merit ZT [1-3].
AgSbTe
2 attracts a lot of attention in recent years for its high ZT value 2.6 at 573K by cadmium doping [4]. A promising, yet relatively unexplored, avenue for advancing TE materials involves optimizing their parameters through applied stress or pressure. High-pressure methods provide access to a unique realm where variable pressure can be applied to tailor thermoelectric properties.
Previous studies of AgSbTe
2 under pressure contradicted on the overall structural evolution, mainly about the exact structure of the higher-pressure phase [5,6]. In this study, we performed a synchrotron X-ray powder diffraction study using a Diamond anvil cell (DAC) and Neon as the pressure transmission medium (PTM) to apply pressure on AgSbTe
2. The pressure was increased from ambient to 60 GPa. At ambient conditions, AgSbTe
2 crystalizes in a FCC-like partial solid solution, in which Ag and Sb atoms occupy the 4a Wyckoff positions (WP) with 50% occupancy. Upon pressure increase, a pressure induced amorphization was observed at 19.2 GPa, and AgSbTe
2 remained amorphous up to 37 GPa. Above 37 GPa, a pressure induced crystallization was observed towards a BCC-like structure. At room temperature, the XRD patterns of the BCC phase strongly indicated a total solid solution, with all elements occupying the 2a WP with relevant partial occupancies (25, 25 and 50% for Ag, Sb and Te, respectively). In order to further explore the validity of this structural model, after AgSbTe
2 crystalized into the BCC-like structure, we used laser heating to examine the possible ordering of the structure at elevated temperatures. A previous study on Bi-Te alloys documented that temperature could induced some atomic ordering [7]. However, in our study even the temperature was increased to 1700K which decomposed the material into Sb
2Te
3 and Ag
2Te, we didn’t observe the characteristic Bragg peak of a partial solid solution (B2 structure). Therefore, in contrast to the pervious report by Kumar
et al. [6] we conclude that the BCC structure is a total solid solution (A2 structure), as opposed to a partial solid solution B2 structure.
Upon decreasing pressure, a clear kinetic effect was observed. In details, the rate of releasing pressure dictates if the phase transitions are fully reversible towards the FCC-like structure or the amorphous phase persists after full pressure release. Molecular dynamics calculations aiming to fully elucidate the overall structural evolution under pressure are ongoing.
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