p–n Transition in Thermoelectric Semiconductor Eskebornite

Eskebornite (CuFeSe<sub>2</sub>) is a I-III-VI<sub>2</sub> semiconductor with a tetragonal crystal structure, known for its intriguing electrical and magnetic properties. However, experimental studies on this material remain scarce. In this study, Ni-doped eskebornite, Cu<sub>1-x</sub>Ni<sub>x</sub>FeSe<sub>2</sub> (x = 0.02-0.06), was synthesized via solid-state methods by substituting Ni<sup>2+</sup> for Cu<sup>+</sup>. Mechanical alloying was employed to prepare the compounds, followed by hot pressing. X-ray diffraction analysis revealed the eskebornite phase alongside a minor secondary phase, identified as penroseite (NiSe<sub>2</sub>) with a cubic crystal structure. Thermoelectric properties were measured over the temperature range of 323-623 K. The Seebeck coefficient exhibited p-type behavior at low temperatures but transitioned to n-type at higher temperatures, indicating a temperature-dependent p-n transition due to changes in the dominant charge carriers. With increasing Ni doping, the Seebeck coefficient increased positively at low temperatures and negatively at high temperatures, with the p-n transition temperature shifting to lower values. Electrical conductivity decreased with higher Ni doping levels, while its positive temperature dependence became more pronounced, reflecting non-degenerate semiconductor behavior. Thermal conductivity showed a negative temperature dependence but increased with higher Ni content. The highest thermoelectric performance was observed for Cu<sub>0.98</sub>Ni<sub>0.02</sub>FeSe<sub>2</sub>, achieving ZT<sub>p</sub> = 0.30 × 10<sup>-3</sup> at 523 K, and for Cu<sub>0.94</sub>Ni<sub>0.06</sub>FeSe<sub>2</sub>, achieving ZT<sub>n</sub> = 0.55 × 10<sup>-3</sup> at 623 K, where ZT<sub>p</sub> and ZT<sub>n</sub> represent the dimensionless figure of merit for p-type and n-type thermoelectric materials, respectively.

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Publication Details

Journal
Materials
Published
2025-03-02
DOI
https://doi.org/10.3390/ma18051129
Primary Topic
Advanced Thermoelectric Materials and Devices
Type
article
Field-Weighted Citation Impact
0.00

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article

p–n Transition in Thermoelectric Semiconductor Eskebornite

Il‐Ho Kim, JaeJong Ryu
Materials
Advanced Thermoelectric Materials and Devices
article

p–n Transition in Thermoelectric Semiconductor Eskebornite

Il‐Ho Kim, JaeJong Ryu
article en

Abstract

Eskebornite (CuFeSe<sub>2</sub>) is a I-III-VI<sub>2</sub> semiconductor with a tetragonal crystal structure, known for its intriguing electrical and magnetic properties. However, experimental studies on this material remain scarce. In this study, Ni-doped eskebornite, Cu<sub>1-x</sub>Ni<sub>x</sub>FeSe<sub>2</sub> (x = 0.02-0.06), was synthesized via solid-state methods by substituting Ni<sup>2+</sup> for Cu<sup>+</sup>. Mechanical alloying was employed to prepare the compounds, followed by hot pressing. X-ray diffraction analysis revealed the eskebornite phase alongside a minor secondary phase, identified as penroseite (NiSe<sub>2</sub>) with a cubic crystal structure. Thermoelectric properties were measured over the temperature range of 323-623 K. The Seebeck coefficient exhibited p-type behavior at low temperatures but transitioned to n-type at higher temperatures, indicating a temperature-dependent p-n transition due to changes in the dominant charge carriers. With increasing Ni doping, the Seebeck coefficient increased positively at low temperatures and negatively at high temperatures, with the p-n transition temperature shifting to lower values. Electrical conductivity decreased with higher Ni doping levels, while its positive temperature dependence became more pronounced, reflecting non-degenerate semiconductor behavior. Thermal conductivity showed a negative temperature dependence but increased with higher Ni content. The highest thermoelectric performance was observed for Cu<sub>0.98</sub>Ni<sub>0.02</sub>FeSe<sub>2</sub>, achieving ZT<sub>p</sub> = 0.30 × 10<sup>-3</sup> at 523 K, and for Cu<sub>0.94</sub>Ni<sub>0.06</sub>FeSe<sub>2</sub>, achieving ZT<sub>n</sub> = 0.55 × 10<sup>-3</sup> at 623 K, where ZT<sub>p</sub> and ZT<sub>n</sub> represent the dimensionless figure of merit for p-type and n-type thermoelectric materials, respectively.

MaterialsVol. 18(5)
Korea National University of Transportation (KR)
Ministry of Education - Singapore
Openalex Percentile: Top 97%
Advanced Thermoelectric Materials and Devices
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