2022
DOI: 10.1016/j.mtphys.2021.100590
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Achieving high average power factor in tetrahedrite Cu12Sb4S13 via regulating electron-phonon coupling strength

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Cited by 10 publications
(7 citation statements)
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“…This phenomenon could also be connected with the liquid-like nature of copper ions, which is more probable in Cu-rich tetrahedrite phases. As is often reported for the superionic argyrodites [24,60], as well as tetrahedrites [48,61,62], the migration of Cu ions can strongly disturb phonon propagation. To verify the TE performance of the investigated samples, the density of the state effective mass m * was calculated using the Kane band model.…”
Section: Samplementioning
confidence: 83%
“…This phenomenon could also be connected with the liquid-like nature of copper ions, which is more probable in Cu-rich tetrahedrite phases. As is often reported for the superionic argyrodites [24,60], as well as tetrahedrites [48,61,62], the migration of Cu ions can strongly disturb phonon propagation. To verify the TE performance of the investigated samples, the density of the state effective mass m * was calculated using the Kane band model.…”
Section: Samplementioning
confidence: 83%
“…Considering the practical application of TE materials, both the average power factor (PF ave ) and the average zT (zT ave ) are critical. [17,55] Here, PF ave and zT ave of Cu 3 SbS 4 /9 wt% CuAlS 2 and Cu 3 SbS 4 /9 wt% CuAlS 2 /1.5 wt% AgAlS 2 are shown in Figure 8b and Figure S28 (Supporting Information), respectively. It can be seen that PF ave and zT ave of Cu 3 SbS 4 /9 wt% CuAlS 2 reach 16.1 µW cm −1 K −2 and 0.73 in the temperature range of 400 to 773 K, respectively.…”
Section: Thermoelectric Performance Of Cu 3 Sbs 4 /9 Wt% Cuals 2 /Y W...mentioning
confidence: 99%
“…obtained a high average power factor of 12 µW cm −1 K −2 and a high zT of 1.1 at 723 K by manipulating electron–phonon coupling strength in Cu 12 Sb 4 S 13 . [ 17 ] Hu et al. fabricated Cu 12 Sb 4 S 13 with porous microstructure by adding BiI 3 and claimed a high zT of 1.15 at 723 K. [ 18 ] Kumar et al.…”
Section: Introductionmentioning
confidence: 99%
“…3 For the relevant parameters, κ was easily adjusted in comparison with the other parameters, and it can be optimized by microstructure and stepwise alloying design. 4 Illuminated by the idea of "crystallographic distortion" of diamondoid solid solutions, the stepwise alloying strategy is expected to create a different approach to depress thermal conductivity in solid solutions. 5,6 Theoretically, stepwise alloying strategies could adjust lattice thermal conductivity; for example, carrier pocket engineering, 7 interfacial effects, 8 and entropy engineering can synergistically tune the intrinsic phonon scattering.…”
Section: ■ Introductionmentioning
confidence: 99%
“…Thermoelectric (TE) materials have no moving parts and can convert waste heat into electrical energy, which makes them particularly appealing in power generation and waste heat recycling. , The conversion efficiency of thermoelectric materials is gauged by the dimensionless figure of merit zT , which is defined as italiczT = α 2 σ κ T , (where α, σ, α 2 σ, κ, and T are the Seebeck coefficient, electrical conductivity, power factor, thermal conductivity, and absolute temperature, respectively) . For the relevant parameters, κ was easily adjusted in comparison with the other parameters, and it can be optimized by microstructure and stepwise alloying design . Illuminated by the idea of “crystallographic distortion” of diamondoid solid solutions, the stepwise alloying strategy is expected to create a different approach to depress thermal conductivity in solid solutions. , Theoretically, stepwise alloying strategies could adjust lattice thermal conductivity; for example, carrier pocket engineering, interfacial effects, and entropy engineering can synergistically tune the intrinsic phonon scattering.…”
Section: Introductionmentioning
confidence: 99%