Compounds (May 2023)

Interplay between Fe(II) and Fe(III) and Its Impact on Thermoelectric Properties of Iron-Substituted Colusites Cu<sub>26−<i>x</i></sub>Fe<i><sub>x</sub></i>V<sub>2</sub>Sn<sub>6</sub>S<sub>32</sub>

  • Alexey O. Polevik,
  • Alexey V. Sobolev,
  • Iana S. Glazkova,
  • Igor A. Presniakov,
  • Valeriy Yu. Verchenko,
  • Joosep Link,
  • Raivo Stern,
  • Andrei V. Shevelkov

DOI
https://doi.org/10.3390/compounds3020027
Journal volume & issue
Vol. 3, no. 2
pp. 348 – 364

Abstract

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Following the trend of finding better thermoelectric materials among synthetic analogs of copper–chalcogenide minerals, we have synthesized iron-bearing colusites of a general formula Cu26−xFexV2Sn6S32. They crystallize in the cubic space group P-43n with the unit cell parameter increasing linearly with the iron content. At a low iron concentration, the crystal structure features disorder manifested by an anti-site effect and a shift of a part of the tin atoms from their ideal positions, which is absent for higher iron contents. The magnetization and 57Fe/119Sn Mössbauer studies showed that, for x = 1, iron is present as Fe3+, whereas for x > 1, Fe2+ and Fe3+ coexist. Additionally, weak antiferromagnetic interactions between iron atoms and fast on the 57Fe Mössbauer time scale (107–109 s−1) electron transfer between adjacent Fe2+ and Fe3+ centers were revealed. Thermoelectric studies showed that iron-bearing colusites are p-type semiconductors with low thermal conductivity stemming from their complex crystal structure and structural disorder. The highest ZT of 0.78 at 700 K was found for the x = 1 iron content, where iron is present as Fe3+ only.

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