Promoted thermoelectric performance in cubic-phase GeTe via grain-boundary phase elimination under phase diagram guidance

Eliminating the ferroelectric phase transition to obtain a cubic phase under ambient conditions is deemed an ultimate goal for p-type GeTe-based materials to be feasible for thermoelectric generator applications at mid-temperature range. Alloying stoichiometric AgSbTe 2 or non-stoichiometric Ag 1− δ...

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Veröffentlicht in:Energy & environmental science 2024-11, Vol.17 (22), p.8691-8701
Hauptverfasser: Zhang, Fudong, Ma, Baopeng, Luo, Yiyuan, Zhu, Lujun, Wang, Weishuai, Shi, Yalin, Jia, Beiquan, Ge, Zhen-Hua, Yang, Zupei, Wu, Di, He, Jiaqing
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Sprache:eng
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Zusammenfassung:Eliminating the ferroelectric phase transition to obtain a cubic phase under ambient conditions is deemed an ultimate goal for p-type GeTe-based materials to be feasible for thermoelectric generator applications at mid-temperature range. Alloying stoichiometric AgSbTe 2 or non-stoichiometric Ag 1− δ Sb 1+ δ Te 2+ δ into GeTe can regulate its cubic-rhombohedral phase transition temperature well below 300 K; nevertheless, the existence of the high-resistivity Ag 8 GeTe 6 grain boundary phase impeded the further improvement of thermoelectric performance in both cases. In this work, as guided by the phase equilibrium diagram, we successfully eliminated the Ag 8 GeTe 6 grain boundary phase by meticulously tailoring the alloying ratio x and regulating Ag/Sb ratio δ in (GeTe) x (Ag 1− δ Sb 1+ δ Te 2+ δ ) 100− x while retaining its cubic crystalline structure. Furthermore, the formation of Ge 2 Sb 2 Te 5 imbedded in GeTe grains involved discrete van der Waals planar gaps, which can further help reduce the lattice thermal conductivity. As a result, a peak figure of merit ZT max. ∼2.0 at 673 K and average ZT ave. of ∼1.5 at 323–773 K were obtained in our cubic-phase (GeTe) 78 (Ag 0.77 Sb 1.23 Te 2.23 ) 22 , and the fabricated eight-pair thermoelectric power generator exhibited an outstanding conversion efficiency of ∼6.3% with output power of ∼1.32 W at a temperature difference of 480 K. This work demonstrated that eliminating the high-resistivity grain boundary phase is a facile way to realize enhanced thermoelectric performance, and could shed light on further research on other thermoelectric materials.
ISSN:1754-5692
1754-5706
DOI:10.1039/D4EE03090G