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Page 16 of 20 Hamawandi et al. Energy Mater. 2025, 5, 500065 https://dx.doi.org/10.20517/energymater.2024.204
Figure 10. Comparison of ZT values of sintered (A) Bi Te and (B) Sb Te samples with earlier reports on binary phases synthesized
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through different chemical routes. The temperature at which the reported ZT value is reached for the different samples is displayed on
the histograms.
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20-4,000 nm. XPS analysis revealed the presence of Sb , Bi , and Te , attributed to surface-bound oxide
layers in the form of Bi O , Sb O , and TeO . Detailed investigation of the local atomic structure in the
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synthesized Bi Te and Sb Te powder samples was conducted through synchrotron radiation XAS
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experiments. RDFs around absorbing atoms were reconstructed using RMC simulations, and effective force
constants for the nearest and distant coordination shells were subsequently determined from the
temperature dependencies of the MSRDs of the Sb(Bi)-Te, Sb(Bi)-Sb(Bi), and Te-Te atom pairs. The
observed differences in the effective force constants support high anisotropy of the thermal conductivity in
Bi Te and Sb Te in the directions along and across the QLs in their crystallographic structure. The as-made
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materials were consolidated via SPS, upon which texturing along the c-axis was observed in both samples.
Electrical and thermal transport properties were determined on the sintered pellets by measuring electrical
resistance and the S, while the thermal diffusivity was measured using the LFA system. The negative sign of
the S identifies the n-type character of Bi Te , while the positive sign indicates the p-type character of Sb Te .
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Promising σ values were obtained for both samples, though Seebeck values were slightly lower than those
reported in earlier works. It was found that due to the effective phonon scattering, attributed to
nanostructuring, the sintered TE materials exhibited low thermal conductivity, achieving the highest ZT
values of 0.7 (at 573 K) and 0.9 (at 523 K) for n-type Bi Te and p-type Sb Te , respectively. These results
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surpass those reported for these materials synthesized through many other wet-chemical synthetic routes.
The TE performance of the synthesized materials shows good batch-to-batch reproducibility, where the
highest ZT has shifted significantly to the high-temperature region, highlighting their potential for power
generation applications. The presented method is truly scalable and can easily be tailored for one-pot
synthesis of ternary and quaternary TE compositions in one-pot. The scalable, energy- and time-efficient
synthetic method developed, along with the demonstration of its potential for TE materials, creates
opportunities for broader use of these strategic materials while minimizing environmental impact.
DECLARATIONS
Acknowledgments
Hamawandi, B., Pudza, I., and Pudzs, K. thank the Latvian Council of Science for support through project
No. lzp-2023/1-0528. Toprak, M. S. acknowledges funding from the European Union's Horizon 2020
research and innovation program under grant agreement No. 863222. Ballikaya, S. acknowledges support
from the Scientific and Technological Research Council of Turkey (TUBITAK, 119N120). We acknowledge
DESY (Hamburg, Germany), a member of the Helmholtz Association HGF, for providing experimental
facilities. The experiment at the DESY PETRA III synchrotron was performed within proposal No. I-
20220381 EC. Institute of Solid State Physics, University of Latvia, as the Center of Excellence, has received
funding from the European Union's Horizon 2020 Framework Programme H2020-WIDESPREAD-01-
2016-2017-TeamingPhase2 under grant agreement No. 739508, project CAMART . Toprak, M. S. also
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