Achievinga High <i>zT</i><sub>avg</sub> in n‑Type Sb-DopedMg<sub>2</sub>Si<sub>0.3</sub>Sn<sub>0.7</sub> via High-Pressure-ModulatedMicrostructures

Mg<sub>2</sub>Si-based compounds are cost-effective and environmentally friendly thermoelectric materials. However, the current Mg<sub>2</sub>(Si,Sn) solid solutions still suffer from the low figure of merit <i>zT</i> (or the low energy conversion efficiency), especially the low averaged <i>zT</i> value (<i>zT</i><sub>avg</sub> < 1.0). In this study, we synthesize the Mg<sub>2</sub>(Si<sub>0.3</sub>Sn<sub>0.7</sub>)<sub>1–<i>x</i></sub>Sb<sub><i>x</i></sub> (<i>x</i> = 0, 0.5, 0.75, 1, and 1.5%) solid solutions through the combination of high-pressure, high-temperature (HPHT) synthesis and spark plasma sintering (SPS). The high-pressure instrument effectively inhibits the unfavorable oxidation of Mg. This HPHT + SPS methodology improves the defect formation efficiency of Sb-doped Mg<sub>2</sub>Si<sub>0.3</sub>Sn<sub>0.7</sub>, leading to an increased carrier concentration and enhanced electrical conductivity. Moreover, as a benefit from the pressure-induced conduction band convergence and Sb-flattened conduction band, the density of states’ effective mass (<i>m</i><sub>d</sub>*) significantly increases to ∼3.3<i>m</i><sub>e</sub>, maintaining high Seebeck coefficients even at a high carrier concentration. The synergetic effects of doping and <i>m</i><sub>d</sub>* increase the peak power factor to exceed 50 μW cm<sup>–1</sup> K<sup>–2</sup>. Notably, due to the HPHT-modified microstructures, the hierarchy phonon scatterings are established to suppress the lattice thermal conductivity to as low as 1.29 W m<sup>–1</sup> K<sup>–1</sup> at 568 K; the Sb point defects, dislocations, and grain boundaries/pores can scatter the short-, medium-, and long-wavelength phonons, respectively. Ultimately, <i>zT</i> of the optimized Mg<sub>2</sub>(Si<sub>0.3</sub>Sn<sub>0.7</sub>)<sub>0.99</sub>Sb<sub>0.01</sub> sample increases significantly in the whole temperature region; the <i>zT</i> peak is 1.37 at 673 K, and a high <i>zT</i> plateau of ∼1.35 is realized between 568 and 723 K. Thus, the notable average <i>zT</i> over the range of 323–723 K is 1.08. Our work demonstrates that the high-pressure-induced defect concentration, effective doping, and microstructure modifications facilitate the thermoelectric property improvement in the Mg<sub>2</sub>(Si,Sn)-based compounds.

Publication Details

Journal
Figshare
Published
2025-03-26
DOI
https://doi.org/10.1021/acsami.5c00398.s001
Primary Topic
Advanced Thermoelectric Materials and Devices
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article

Achievinga High zTavg in n‑Type Sb-DopedMg2Si0.3Sn0.7 via High-Pressure-ModulatedMicrostructures

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Advanced Thermoelectric Materials and Devices
article

Achievinga High zTavg in n‑Type Sb-DopedMg2Si0.3Sn0.7 via High-Pressure-ModulatedMicrostructures

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Abstract

Mg<sub>2</sub>Si-based compounds are cost-effective and environmentally friendly thermoelectric materials. However, the current Mg<sub>2</sub>(Si,Sn) solid solutions still suffer from the low figure of merit <i>zT</i> (or the low energy conversion efficiency), especially the low averaged <i>zT</i> value (<i>zT</i><sub>avg</sub> < 1.0). In this study, we synthesize the Mg<sub>2</sub>(Si<sub>0.3</sub>Sn<sub>0.7</sub>)<sub>1–<i>x</i></sub>Sb<sub><i>x</i></sub> (<i>x</i> = 0, 0.5, 0.75, 1, and 1.5%) solid solutions through the combination of high-pressure, high-temperature (HPHT) synthesis and spark plasma sintering (SPS). The high-pressure instrument effectively inhibits the unfavorable oxidation of Mg. This HPHT + SPS methodology improves the defect formation efficiency of Sb-doped Mg<sub>2</sub>Si<sub>0.3</sub>Sn<sub>0.7</sub>, leading to an increased carrier concentration and enhanced electrical conductivity. Moreover, as a benefit from the pressure-induced conduction band convergence and Sb-flattened conduction band, the density of states’ effective mass (<i>m</i><sub>d</sub>*) significantly increases to ∼3.3<i>m</i><sub>e</sub>, maintaining high Seebeck coefficients even at a high carrier concentration. The synergetic effects of doping and <i>m</i><sub>d</sub>* increase the peak power factor to exceed 50 μW cm<sup>–1</sup> K<sup>–2</sup>. Notably, due to the HPHT-modified microstructures, the hierarchy phonon scatterings are established to suppress the lattice thermal conductivity to as low as 1.29 W m<sup>–1</sup> K<sup>–1</sup> at 568 K; the Sb point defects, dislocations, and grain boundaries/pores can scatter the short-, medium-, and long-wavelength phonons, respectively. Ultimately, <i>zT</i> of the optimized Mg<sub>2</sub>(Si<sub>0.3</sub>Sn<sub>0.7</sub>)<sub>0.99</sub>Sb<sub>0.01</sub> sample increases significantly in the whole temperature region; the <i>zT</i> peak is 1.37 at 673 K, and a high <i>zT</i> plateau of ∼1.35 is realized between 568 and 723 K. Thus, the notable average <i>zT</i> over the range of 323–723 K is 1.08. Our work demonstrates that the high-pressure-induced defect concentration, effective doping, and microstructure modifications facilitate the thermoelectric property improvement in the Mg<sub>2</sub>(Si,Sn)-based compounds.

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Achievinga High <i>zT</i><sub>avg</sub> in n‑Type Sb-DopedMg<sub>2</sub>Si<sub>0.3</sub>Sn<sub>0.7</sub> via High-Pressure-ModulatedMicrostructures · Figshare (2025) | TGRS Research Map | TGRS