Improved Thermoelectric Properties of SrTiO[sub.3] via Co-Doping: DFT Approach

This work considers the enhancement of the thermoelectric figure of merit, ZT, of SrTiO[sub.3] (STO) semiconductors by (La, Dy and N) co-doping. We have focused on SrTiO[sub.3] because it is a semiconductor with a high Seebeck coefficient compared to that of metals. It is expected that SrTiO[sub.3]...

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Bibliographic Details
Published in:Molecules (Basel, Switzerland) Switzerland), 2022-11, Vol.27 (22)
Main Authors: Sikam, Pornsawan, Thirayatorn, Ruhan, Kaewmaraya, Thanayut, Thongbai, Prasit, Moontragoon, Pairot, Ikonic, Zoran
Format: Article
Language:English
Subjects:
Analysis
Electric properties
Electrical conductivity
Hydrogen
Semiconductors
Thermoelectricity
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Summary:This work considers the enhancement of the thermoelectric figure of merit, ZT, of SrTiO[sub.3] (STO) semiconductors by (La, Dy and N) co-doping. We have focused on SrTiO[sub.3] because it is a semiconductor with a high Seebeck coefficient compared to that of metals. It is expected that SrTiO[sub.3] can provide a high power factor, because the capability of converting heat into electricity is proportional to the Seebeck coefficient squared. This research aims to improve the thermoelectric performance of SrTiO[sub.3] by replacing host atoms by La, Dy and N atoms based on a theoretical approach performed with the Vienna Ab Initio Simulation Package (VASP) code. Here, undoped SrTiO[sub.3], Sr[sub.0.875]La[sub.0.125]TiO[sub.3], Sr[sub.0.875]Dy[sub.0.125]TiO[sub.3], SrTiO[sub.2.958]N[sub.0.042], Sr[sub.0.750]La[sub.0.125]Dy[sub.0.125]TiO[sub.3] and Sr[sub.0.875]La[sub.0.125]TiO[sub.2.958]N[sub.0.042] are studied to investigate the influence of La, Dy and N doping on the thermoelectric properties of the SrTiO[sub.3] semiconductor. The undoped and La-, Dy- and N-doped STO structures are optimized. Next, the density of states (DOS), band structures, Seebeck coefficient, electrical conductivity per relaxation time, thermal conductivity per relaxation time and figure of merit (ZT) of all the doped systems are studied. From first-principles calculations, STO exhibits a high Seebeck coefficient and high figure of merit. However, metal and nonmetal doping, i.e., (La, N) co-doping, can generate a figure of merit higher than that of undoped STO. Interestingly, La, Dy and N doping can significantly shift the Fermi level and change the DOS of SrTiO[sub.3] around the Fermi level, leading to very different thermoelectric properties than those of undoped SrTiO[sub.3]. All doped systems considered here show greater electrical conductivity per relaxation time than undoped STO. In particular, (La, N) co-doped STO exhibits the highest ZT of 0.79 at 300 K, and still a high value of 0.77 at 1000 K, as well as high electrical conductivity per relaxation time. This renders it a viable candidate for high-temperature applications.
ISSN:1420-3049
1420-3049
DOI:10.3390/molecules27227923