Potential thermoelectric material Tl<sub>3</sub>XS<sub>4</sub> (X = V, Nb, Ta) with ultralow lattice thermal conductivity

The demand for sustainable energy solutions has driven intensive research into advanced thermoelectric (TE) materials, to harness waste heat for efficient power generation. Recently, several studies have revealed that Tl<sub>3</sub>VS<sub>4</sub> possesses an ultralow lattice thermal conductivity, despite its simple body-centered cubic lattice structure. This paper focuses on the TE properties of Tl<sub>3</sub>XS<sub>4</sub> (X = V, Nb, Ta) compounds through a systematic exploration utilizing first-principles calculations and semiclassical Boltzmann transport theory. The results of the AIMD simulation and phonon calculation reveal the excellent dynamic stability and thermal stability of Tl<sub>3</sub>XS<sub>4</sub> at 300, 500, and 700 K. Moreover, we find that the Tl<sub>3</sub>XS<sub>4</sub> compounds present ultralow lattice thermal conductivity (<0.5 W m<sup>-1</sup> K<sup>-1</sup> at 300 K), and the nanostructure strategy is effective. Based on the outstanding Seebeck coefficient and ultralow lattice thermal conductivity, the optimal <i>ZT</i> values of Tl<sub>3</sub>VS<sub>4</sub>, Tl<sub>3</sub>NbS<sub>4</sub>, and Tl<sub>3</sub>TaS<sub>4</sub> at 300 K are determined to be 1.17 (p-type), 0.84 (n-type), and 0.65 (p-type), respectively. Additionally, at each considered temperature, the maximum <i>ZT</i> values of p-type (n-type) Tl<sub>3</sub>XS<sub>4</sub> follow the order: Tl<sub>3</sub>VS<sub>4</sub> > Tl<sub>3</sub>NbS<sub>4</sub> > Tl<sub>3</sub>TaS<sub>4</sub> (Tl<sub>3</sub>NbS<sub>4</sub> > Tl<sub>3</sub>VS<sub>4</sub> > Tl<sub>3</sub>TaS<sub>4</sub>). Our results demonstrate that Tl<sub>3</sub>XS<sub>4</sub> (X = V, Nb, Ta) compounds are promising thermoelectric materials. This exhaustive research enhanced our nuanced comprehension of the electronic, dynamic, and thermoelectric attributes of Tl<sub>3</sub>XS<sub>4</sub> (X = V, Nb, Ta), thereby offering valuable insights into the TE field.

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Publication Details

Journal
Physical Chemistry Chemical Physics
Published
2024-12-10
DOI
https://doi.org/10.1039/d4cp04000g
Citations
2
Primary Topic
Solid-state spectroscopy and crystallography
Type
article
Field-Weighted Citation Impact
0.23

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article

Potential thermoelectric material Tl3XS4 (X = V, Nb, Ta) with ultralow lattice thermal conductivity

Yao He, Guangzhao Wang, Xiefei Song, Ning Wang et al.
2 citations
Physical Chemistry Chemical Physics
Solid-state spectroscopy and crystallography
0.23
article

Potential thermoelectric material Tl3XS4 (X = V, Nb, Ta) with ultralow lattice thermal conductivity

Yao He, Guangzhao Wang, Xiefei Song, Ning Wang, Wenzhong Li, Siyu Gan, Dekun Ma, Yuhui Luo, Cai Yan
article en
2 citations

Abstract

The demand for sustainable energy solutions has driven intensive research into advanced thermoelectric (TE) materials, to harness waste heat for efficient power generation. Recently, several studies have revealed that Tl<sub>3</sub>VS<sub>4</sub> possesses an ultralow lattice thermal conductivity, despite its simple body-centered cubic lattice structure. This paper focuses on the TE properties of Tl<sub>3</sub>XS<sub>4</sub> (X = V, Nb, Ta) compounds through a systematic exploration utilizing first-principles calculations and semiclassical Boltzmann transport theory. The results of the AIMD simulation and phonon calculation reveal the excellent dynamic stability and thermal stability of Tl<sub>3</sub>XS<sub>4</sub> at 300, 500, and 700 K. Moreover, we find that the Tl<sub>3</sub>XS<sub>4</sub> compounds present ultralow lattice thermal conductivity (<0.5 W m<sup>-1</sup> K<sup>-1</sup> at 300 K), and the nanostructure strategy is effective. Based on the outstanding Seebeck coefficient and ultralow lattice thermal conductivity, the optimal <i>ZT</i> values of Tl<sub>3</sub>VS<sub>4</sub>, Tl<sub>3</sub>NbS<sub>4</sub>, and Tl<sub>3</sub>TaS<sub>4</sub> at 300 K are determined to be 1.17 (p-type), 0.84 (n-type), and 0.65 (p-type), respectively. Additionally, at each considered temperature, the maximum <i>ZT</i> values of p-type (n-type) Tl<sub>3</sub>XS<sub>4</sub> follow the order: Tl<sub>3</sub>VS<sub>4</sub> > Tl<sub>3</sub>NbS<sub>4</sub> > Tl<sub>3</sub>TaS<sub>4</sub> (Tl<sub>3</sub>NbS<sub>4</sub> > Tl<sub>3</sub>VS<sub>4</sub> > Tl<sub>3</sub>TaS<sub>4</sub>). Our results demonstrate that Tl<sub>3</sub>XS<sub>4</sub> (X = V, Nb, Ta) compounds are promising thermoelectric materials. This exhaustive research enhanced our nuanced comprehension of the electronic, dynamic, and thermoelectric attributes of Tl<sub>3</sub>XS<sub>4</sub> (X = V, Nb, Ta), thereby offering valuable insights into the TE field.

Physical Chemistry Chemical PhysicsVol. 27(1)
Xihua University (CN), Yunnan University (CN), Yangtze Normal University (CN), Zhaotong University (CN)
National Natural Science Foundation of China, Yunnan Provincial Department of Education
Openalex Percentile: Top 49%
Solid-state spectroscopy and crystallography
0.23
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