Charge Transport and Thermoelectric Properties of Bornite with Fe-Site Off-Stoichiometry

The effects of Fe non-stoichiometry on crystal structure, microstructural evolution, and thermoelectric transport properties were systematically investigated in bornite (Cu<sub>5</sub>Fe<sub>1+y</sub>S<sub>4</sub>; -0.06 ≤ y ≤ 0.06) synthesized by mechanical alloying followed by hot pressing. X-ray diffraction analysis confirmed the formation of a single-phase orthorhombic bornite structure over the entire composition range. Anisotropic lattice distortion was observed with increasing Fe non-stoichiometry, manifested as contraction along the a-axis and expansion along the b- and c-axes, with a non-linear dependence on composition. Crystallite sizes estimated from Lorentzian peak fitting increased from 64.1 nm for the stoichiometric composition to 70.6-76.3 nm for Fe-deficient samples and 73.2-90.9 nm for Fe-excess samples. Hall-effect measurements revealed p-type semiconducting behavior for the stoichiometric composition, degenerate p-type transport with increased hole concentration under Fe-deficient conditions, and a transition to n-type behavior with reduced carrier mobility under Fe-excess conditions. While Fe-deficient samples retained high electrical conductivity and positive Seebeck coefficients, Fe-excess samples exhibited negative Seebeck coefficients at low temperatures with sign reversal at elevated temperatures. As a consequence, the power factor of Fe-deficient samples was enhanced by approximately 20-30% relative to the stoichiometric composition. In addition, the total thermal conductivity remained below 0.8 W·m<sup>-1</sup>·K<sup>-1</sup> for all samples, and Fe non-stoichiometry effectively suppressed lattice thermal conductivity. Consequently, the Cu<sub>5</sub>Fe<sub>0.94</sub>S<sub>4</sub> composition achieved a maximum dimensionless figure of merit of ZT = 0.61 at 673 K, representing a performance enhancement of approximately 30-70% compared with the stoichiometric composition (ZT = 0.36 at 673 K and 0.47 at 723 K).

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Journal
Materials
Published
2026-03-22
DOI
https://doi.org/10.3390/ma19061252
Primary Topic
Advanced Thermoelectric Materials and Devices
Type
article
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article

Charge Transport and Thermoelectric Properties of Bornite with Fe-Site Off-Stoichiometry

Seungmin Lee, Hyemin Oh, Hyeon-Sik O, Il-Ho Kim
Materials
Advanced Thermoelectric Materials and Devices
article

Charge Transport and Thermoelectric Properties of Bornite with Fe-Site Off-Stoichiometry

Seungmin Lee, Hyemin Oh, Hyeon-Sik O, Il-Ho Kim
article en

Abstract

The effects of Fe non-stoichiometry on crystal structure, microstructural evolution, and thermoelectric transport properties were systematically investigated in bornite (Cu<sub>5</sub>Fe<sub>1+y</sub>S<sub>4</sub>; -0.06 ≤ y ≤ 0.06) synthesized by mechanical alloying followed by hot pressing. X-ray diffraction analysis confirmed the formation of a single-phase orthorhombic bornite structure over the entire composition range. Anisotropic lattice distortion was observed with increasing Fe non-stoichiometry, manifested as contraction along the a-axis and expansion along the b- and c-axes, with a non-linear dependence on composition. Crystallite sizes estimated from Lorentzian peak fitting increased from 64.1 nm for the stoichiometric composition to 70.6-76.3 nm for Fe-deficient samples and 73.2-90.9 nm for Fe-excess samples. Hall-effect measurements revealed p-type semiconducting behavior for the stoichiometric composition, degenerate p-type transport with increased hole concentration under Fe-deficient conditions, and a transition to n-type behavior with reduced carrier mobility under Fe-excess conditions. While Fe-deficient samples retained high electrical conductivity and positive Seebeck coefficients, Fe-excess samples exhibited negative Seebeck coefficients at low temperatures with sign reversal at elevated temperatures. As a consequence, the power factor of Fe-deficient samples was enhanced by approximately 20-30% relative to the stoichiometric composition. In addition, the total thermal conductivity remained below 0.8 W·m<sup>-1</sup>·K<sup>-1</sup> for all samples, and Fe non-stoichiometry effectively suppressed lattice thermal conductivity. Consequently, the Cu<sub>5</sub>Fe<sub>0.94</sub>S<sub>4</sub> composition achieved a maximum dimensionless figure of merit of ZT = 0.61 at 673 K, representing a performance enhancement of approximately 30-70% compared with the stoichiometric composition (ZT = 0.36 at 673 K and 0.47 at 723 K).

MaterialsVol. 19(6)
Korea National University of Transportation (KR)
Openalex Percentile: Top 13%
Advanced Thermoelectric Materials and Devices
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