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Paper ID:IJSREM68322

Exploring Thermoelectric Properties Enhancement Through Creation of Defects and Doping

Stream/Area:

-

Subject:

-

Paper ID:

IJSREM68322

Volume:

10 |

10 |

Oct 2026

Pages:

1-10

Publication Frequency:

Monthly (12 issues per year)

DOI
Digital Object Identifier
10.55041/IJSREM68322

License:International Journal of Scientific Research in Engineering and Management follows the Creative Commons Attribution 4.0 (CC BY 4.0) License, allowing free use and distribution with proper attribution.

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Authors

ZSA

Zawwar Shabahat Ahmed

Science

American International School

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Abstract

Thermoelectric conversion provides a direct means of transforming a temperature difference into electrical energy and is therefore relevant to the recovery of otherwise unused heat. Copper sulfide (CuS) is an attractive thermoelectric host because it combines high electrical transport capability with relatively low thermal conductivity and a defect-rich crystal chemistry. In this work, selenium was introduced into CuS at nominal concentrations of 0.05, 0.10, and 0.15 to regulate both carrier transport and phonon propagation. The resulting Se–CuS materials were examined with respect to their crystal structure, microstrain, crystallite size, electrical conductivity, Seebeck coefficient, thermal conductivity, power factor, and thermoelectric figure of merit. X-ray diffraction confirmed that the characteristic CuS framework was retained after Se incorporation, while the progressive displacement and broadening of the diffraction peaks indicated lattice perturbation. Williamson–Hall analysis showed that the estimated microstrain increased from 4.9 × 10−5 to 8.8 × 10−5, whereas the corresponding crystallite size decreased from about 35.3 to 29.3 nm as the Se content increased. Among the investigated compositions, 0.10 Se–CuS delivered the most favorable combination of thermoelectric properties, giving a Seebeck coefficient of about 52 μV K−1, an electrical conductivity of 830.6 S cm−1, and a power factor of 224.6 μW m−1 K−2 at 300 K. The thermal conductivity was reduced from 2.80 W m−1 K−1 for pristine CuS to 1.85 W m−1 K−1 for the 0.10 composition at 300 K, leading to a calculated maximum ZT of approximately 0.143 at 500 K. Finite-element calculations in COMSOL Multiphysics were additionally used to visualize temperature, heat-flow, and electrical-potential distributions under thermoelectric operating conditions. The results indicate that controlled Se incorporation can introduce useful structural disorder while retaining sufficient electronic transport, thereby providing a route for balancing phononic and electronic contributions in CuS-based thermoelectric materials.

KEYWORDS

CuS; Se-doped CuS; thermoelectric materials; waste-heat recovery

Cite This Article

Zawwar Shabahat Ahmed, "Exploring Thermoelectric Properties Enhancement Through Creation of Defects and Doping," International Journal of Scientific Research in Engineering and Management, vol. 10, no. 10, pp. 1-10, Oct 2026. https://doi.org/10.55041/IJSREM68322

Full Article/Conclusion

Selenium incorporation provides an effective means of modifying the structural and thermoelectric response of CuS while preserving the characteristic host crystal framework. XRD measurements indicate that the CuS phase remains dominant across the investigated Se concentrations, whereas peak displacement and broadening reveal progressive lattice perturbation. Williamson–Hall analysis shows that the microstrain increases from approximately 4.9 × 10−5 to 8.8 × 10−5 while the crystallite size decreases from about 35.3 to 29.3 nm with increasing Se content. The structural disorder introduced by Se is accompanied by changes in both electronic and thermal transport. The 0.10 Se–CuS composition provides the most favorable overall response, with a Seebeck coefficient of approximately 52 μV K−1, electrical conductivity of 830.6 S cm−1, and power factor of 224.6 μW m−1 K−2 at 300 K. Its thermal conductivity is reduced to approximately 1.85 W m−1 K−1 at 300 K, and the calculated ZT reaches about 0.143 at 500 K. Finite-element simulations further show that the optimized Se–CuS element can sustain a substantial temperature gradient while developing an electrical potential, and the modeled Peltier configuration exhibits a corresponding electrothermal response. The lower performance of the 0.15 composition indicates that excessive dopant-induced disorder can begin to impair charge transport. Overall, the results demonstrate that controlled, rather than maximum, Se incorporation is beneficial for balancing electronic and phononic transport in CuS and provides a useful basis for further development of CuS-based thermoelectric materials.

References

[1]         H. Han et al., “Advancements in thermoelectric materials: optimization strategies for enhancing energy conversion,” J. Mater. Chem. A, vol. 12, no. 36, pp. 24041–24083, Sep. 2024, doi: 10.1039/D4TA03666B. [2]         M. Mukherjee, A. Srivastava, and A. K. Singh, “Recent advances in designing thermoelectric materials,” J. Mater. Chem. C, vol. 10, no. 35, pp. 12524–12555, Sep. 2022, doi: 10.1039/D2TC02448A. [3]         Y. Li et al., “Hierarchical MoS2/CuS photonic nanostructure accelerating photothermoelectric conversion of bacterial cellulose based phase change materials,” J. Colloid Interface Sci., vol. 702, p. 138863, Jan. 2026, doi: 10.1016/J.JCIS.2025.138863. [4]         E. Isotta and A. Zevalkink, “Chemical compensation meets bond engineering in skutterudites,” Joule, vol. 10, no. 2, p. 102321, Feb. 2026, doi: 10.1016/j.joule.2026.102321. [5]         P. Rawat and S. Kala, “A concise review on the progression of copper sulfide as a potential thermoelectric material: Synthesis and thermoelectric properties,” Nano Express, vol. 6, no. 1, p. 012001, Jan. 2025, doi: 10.1088/2632-959X/ADA6E7. [6]         M. S. Abdurrhaman, M. Diantoro, R. A. Pahlevi, A. N. R. Masruhah, and C. I. Yogihati, “Synthesis and Characterization of CuS-GO Nanocomposite as Thermoelectric Material,” AIP Conf. Proc., vol. 3197, no. 1, Feb. 2025, doi: 10.1063/5.0240589/3336453. [7]         K. V. Nabeela and P. P. Pradyumnan, “Reinforcement in thermoelectric properties of graphene nanoplatelets integrated covellite CuS nanocomposites for green heat harvesting applications,” J. Alloys Compd., vol. 1050, p. 185480, Jan. 2026, doi: 10.1016/J.JALLCOM.2025.185480. [8]         S. I. Basha, S. S. Shah, and D. Y. Yoo, “Advancements in thermoelectric properties of cement and geopolymer composites reinforced with carbon-based nanomaterials,” J. Build. Eng., vol. 104, p. 112312, Jun. 2025, doi: 10.1016/J.JOBE.2025.112312. [9]         Z. Li et al., “Plasticity of Bi2Te3-family thermoelectric crystals,” Nat. Commun. 2025 161, vol. 16, no. 1, pp. 5190-, Jun. 2025, doi: 10.1038/s41467-025-60465-2. [10]       E. S. Toberer, L. L. Baranowski, and C. Dames, “Advances in thermal conductivity,” Annu. Rev. Mater. Res., vol. 42, no. Volume 42, 2012, pp. 179–209, Aug. 2012, doi: 10.1146/ANNUREV-MATSCI-070511-155040/CITE/REFWORKS.

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Publication Date

10/26/2026

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