Abstract
Interest in thermoelectric (TE) materials has revived in recent years because TE materials realize not only the utilization of distributed unused thermal energy, such as exhaust heat from automobiles and factories and solar heat, but also cold power generators and self-power supplies for wireless sensors. However, because the bandgap of low-temperature TE materials is relatively small, the precise calculation of its physical properties is difficult to achieve by first-principles calculations based on conventional density functional theory. The present study investigates the effects of isotropic strain and incorporation of isoelectronic impurities on the TE transport properties of extremely narrow-gap semiconducting α-SrSi2. By adopting the Gaussian–Perdew–Burke–Ernzerhof hybrid functional, the analysis clarifies the relationship between the lattice distortion and the electronic structure in α-Sr4–xAxBySi8–y (A = Mg, Ca, or Ba; B = C, Ge, Sn, or Pb) and elucidates the TE transport properties. In particular, an irregular bandgap expansion was observed in α-Sr4CSi7, suggesting that the TE performance can be maximized by appropriate tuning of the carrier concentration.
Highlights
One goal of materials science is realizing an energy-sustainable society
By adopting the Gaussian–Perdew–Burke–Ernzerhof hybrid functional, the analysis clarifies the relationship between the lattice distortion and the electronic structure in α-Sr4–xAxBySi8–y (A = Mg, Ca, or Ba; B = C, Ge, Sn, or Pb) and elucidates the TE transport properties
An irregular bandgap expansion was observed in α-Sr4CSi7, suggesting that the TE performance can be maximized by appropriate tuning of the carrier concentration
Summary
One goal of materials science is realizing an energy-sustainable society. The emerging global energy demand has intensified interest in efficient power generation. Thermoelectric (TE) conversion technology, which directly converts waste heat to electricity with no mechanical drive using so-called TE materials, has been revived for this purpose. A convenient measure of TE performance is the dimensionless figure of merit ZT = S2σT/(κel + κl), where S is the Seebeck coefficient; σ is the electrical conductivity; κel and κl are the electronic and lattice thermal conductivities, respectively; and T is the absolute temperature. The quantities S, σ, and κel depend on the electronic structure of the material, and κl is dominated by the lattice structure. To improve the ZT, the power factor (PF = S2σ) must be improved by optimizing the carrier concentration and lowering the values of κel and κl
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