Synergistically optimized electronic and phonon transport properties in cubic SnSe thermoelectric materials via Pb doping

被引:0
|
作者
Wang, Wen-Ying [1 ]
Zhu, Jun-Liang [1 ]
Bo, Lin [1 ]
Zhou, Wen-Ying [1 ]
Liu, Xing-Shuo [1 ]
Li, Chang-Cun [1 ]
Zhang, Zheng [2 ]
Zhao, De-Gang [1 ]
机构
[1] Univ Jinan, Sch Mat Sci & Engn, Jinan 250022, Peoples R China
[2] Univ Orleans, CNRS, CEMHTI UPR3079, F-45071 Orleans, France
来源
RARE METALS | 2025年
关键词
Cubic SnSe; Thermoelectric; Doping; Internal microstrain; <italic>ZT</italic>; POLYCRYSTALLINE SNSE; THERMAL-CONDUCTIVITY; PERFORMANCE; FIGURE; MERIT;
D O I
10.1007/s12598-024-03070-4
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The rock-salt cubic SnSe compound with multiple valleys and inherent low thermal conductivity is considered to be a promising thermoelectric compound. In this study, heterogeneous Pb atoms were strategically introduced into the lattice of cubic SnSe matrix, synergistically adjusting the thermoelectric transport properties of samples by optimizing hole carrier concentration (n) and suppressing thermal conductivity (kappa tot). When the doping content reached 0.08 mol, the peak power factor (PF) at 300 K increased to 20.00 mu W<middle dot>cm-1<middle dot>K-2. The growing internal microstrain induced by the differences in atomic size strengthened the phonon scattering and effectively reduced the lattice thermal conductivity (kappa L). With further decoupling of the electrical and thermal transport properties, a peak thermoelectric figure of merit (ZT) of 0.82 and an average ZT of 0.42 (300-750 K) were achieved in the samples doped with 0.10 mol Pb. These findings highlight the effectiveness of the selected dopants and demonstrate their synergy in improving the performance of thermoelectric materials. (sic)(sic)(sic)(sic)(sic)(sic)(sic)SnSe(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic), (sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic).(sic)(sic)(sic)(sic)(sic)(sic)(sic)Pb(sic)(sic)(sic)(sic)(sic)(sic)SnSe(sic)(sic)(sic)(sic)(sic), (sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic).(sic)(sic)(sic)(sic), (sic)Pb(sic)(sic)(sic)(sic)(sic)(sic)(sic)0.08(sic), (sic)(sic)(sic)300 K(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic), (sic)(sic)(sic)20 mu W<middle dot>cm(-)(1)<middle dot>K--(2).(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic), (sic)(sic)(sic)(sic)(sic)(sic)(sic), (sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic).(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic), (sic)(sic)0.10 mol Pb(sic)(sic)(sic)(sic)(sic)ZT(sic)0.82, (sic)(sic)ZTave(sic)0.42 (300-750 K).(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic), (sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic)(sic).
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