Cu3SbS4-based materials composed of nontoxic,
low-cost, and earth-abundant elements potentially exhibit favorable
thermoelectric performance. However, some key transport parameters
and thermal stability have not been reported. In this work, the effects
of Bi and Sn co-doping on thermoelectric properties and the thermal
stability of Cu3SbS4 were studied by experiment
and theoretical validation. Bi and Sn doping can effectively tune
the electrical properties and the electronic band structure. The Bi
and Sn doping leads to an increased carrier concentration from 6.4
× 1017 to 7.4 × 1020 cm–3 and a decreased optical band gap from 0.85 to 0.73 eV. The effective
mass was increased from ∼3.0 me for Bi-doped samples
to ∼4.0 me for Bi and Sn co-doped samples. An enhanced
power factor of 1398 μW m–1 K–2 at 623 K was obtained for Cu3Sb1–x–y
Bi
x
Sn
y
S4 (x =
0.06, y = 0.09). The measurements of elastic properties
exhibited a large Grüneisen parameter (γ ∼2) for
Cu3SbS4-based materials. Finally, a maximum
zT of 0.76 ± 0.02 at 623 K was achieved for Cu3Sb1–x–y
Bi
x
Sn
y
S4 (x = 0.06, y = 0.05) sample. In
addition, Cu3SbS4 materials possess excellent
thermal stability after thermal treatment in vacuum at 573 K for totally
500 h and dozens of heating–cooling thermal cycles (300–623–300
K). It indicates that Cu3SbS4 is a robust alternative
for Te-free thermoelectric materials at an intermediate temperature
range. This work provides feasible guidance to survey the thermal
stability of chalcogenides.
The n-type polycrystalline materials of Ba 8 Ga 16 Ge 30 bulks have been successfully synthesized via the high-temperature and high-pressure (HPHT) method, and their crystal structure has been characterized using the X-ray diffraction. Through the thermoelectric properties measurements and microstructure studies, we know that the improvement of the dimensionless thermoelectric figure-of-merit (ZT) benefits from the low lattice thermal conductivity due to the increased low, medium, and high wavelength phonon scattering by grain boundaries, nanostructures, nanoscale domains, and lattice defects, which are ubiquitous in the synthetic bulk material. As the temperature increases, the power factor (PF) obviously increases, and the thermal conductivity evidently decreases. A minimum thermal conductivity of 0.71 W m −1 K −1 was reached at 773 K for Ba 8 Ga 16 Ge 30 synthesized at 4 GPa. A good ZT value 1.14 was achieved, which was attributed to not only the enhanced PF but also the relative low thermal conductivity.
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