While most of the thermoelectric materials work well only at low and mid temperatures, high-temperature thermoelectric materials (T > 900 K) are equally important for the operation of deep-spacecraft missions, nuclear reactors, and high-temperature industrial reactors. To accomplish this demand, this work provides insights into wide band gap semiconducting RFeO 3 (rare-earth orthoferrites) for high-temperature thermoelectric applications. Using the first-principles density functional theory calculations, we have demonstrated the coexistence of extremely flat and corrugated flat bands near the Fermi region in a wide band gap material. The presence of such features enhances and sustains the thermopower, electrical conductivity, and power factor, which are the crucial factors for the efficiency of thermoelectric materials. Semiclassical Boltzmann formalism was then employed to study the transport properties of four orthorhombic RFeO 3 materials (R = Pr, Nd, Sm, and Gd). Our results reveal high Seebeck coefficients (thermopower) along with the large electrical conductivities over the high hole doping carrier concentration and in the high-temperature region (T > 900 K). Furthermore, significantly large power factors are obtained with very low theoretical minimum lattice thermal conductivity in the range 1.41−1.51 W m −1 K −1 . These huge power factors directly suggest the maximum power output in RFeO 3 , which we believe is a more appropriate performance index than the figure of merit, especially for hightemperature thermoelectric applications. We also emphasize that the outcomes of our work would be certainly useful for experimentalists in designing high-temperature thermoelectric materials.
With
recent thermoelectric studies concentrating too much on low- and mid-temperature
applications, an interesting question is, “are there any materials
suitable for high-temperature thermoelectric operations?” To
answer this, we have demonstrated in this work the viability of the
ternary ultrawide-band-gap materials GaB3N4 and
AlB3N4 for high-temperature thermoelectric applications
using the first-principles calculation method. Our accurate transport
calculations, considering both elastic and inelastic scattering mechanisms,
reveal the ultrahigh power factors as high as 1821 μW m–1 K–2 in GaB3N4 and 1876 μW m–1 K–2 in
AlB3N4 at 2000 K. The power factors are calculated
from the Seebeck coefficients and electrical conductivities for both
electron and hole carrier concentrations between 1018 and
1021 cm–3. For the figure-of-merit (ZT)
calculation, the obtained power factors along with the electronic
thermal conductivities determined from the definite Lorenz numbers
and the lattice thermal conductivities from the phonon vibrations
were used. The calculated ZT values seem to be appreciable for high-temperature
applications considering the materials’ stability factor and
the temperature range within the optimum electron carrier concentration
of 1021 cm–3. Although the lattice thermal
conductivities are higher, which decrease the values of ZT, considering
the ultrahigh power factors instead of the ZT factor could be the
right choice for high-temperature thermoelectric applications.
The tug-of-war between the thermoelectric power factor and the figure-of-merit complicates thermoelectric material selection, particularly for mid-to-high temperature thermoelectric materials. Approaches to reduce lattice thermal conductivity while maintaining a high-power...
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