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Tin-Substituted Chalcopyrite: An n-Type Sulfide with Enhanced Thermoelectric Performance

[Image: see text] The dearth of n-type sulfides with thermoelectric performance comparable to that of their p-type analogues presents a problem in the fabrication of all-sulfide devices. Chalcopyrite (CuFeS(2)) offers a rare example of an n-type sulfide. Chemical substitution has been used to enhanc...

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Detalles Bibliográficos
Autores principales: Tippireddy, Sahil, Azough, Feridoon, Vikram, Tompkins, Frances Towers, Bhui, Animesh, Freer, Robert, Grau-Crespo, Ricardo, Biswas, Kanishka, Vaqueiro, Paz, Powell, Anthony V.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9281371/
https://www.ncbi.nlm.nih.gov/pubmed/35844633
http://dx.doi.org/10.1021/acs.chemmater.2c00637
Descripción
Sumario:[Image: see text] The dearth of n-type sulfides with thermoelectric performance comparable to that of their p-type analogues presents a problem in the fabrication of all-sulfide devices. Chalcopyrite (CuFeS(2)) offers a rare example of an n-type sulfide. Chemical substitution has been used to enhance the thermoelectric performance of chalcopyrite through preparation of Cu(1-x)Sn(x)FeS(2) (0 ≤ x ≤ 0.1). Substitution induces a high level of mass and strain field fluctuation, leading to lattice softening and enhanced point-defect scattering. Together with dislocations and twinning identified by transmission electron microscopy, this provides a mechanism for scattering phonons with a wide range of mean free paths. Substituted materials retain a large density-of-states effective mass and, hence, a high Seebeck coefficient. Combined with a high charge-carrier mobility and, thus, high electrical conductivity, a 3-fold improvement in power factor is achieved. Density functional theory (DFT) calculations reveal that substitution leads to the creation of small polarons, involving localized Fe(2+) states, as confirmed by X-ray photoelectron spectroscopy. Small polaron formation limits the increase in carrier concentration to values that are lower than expected on electron-counting grounds. An improved power factor, coupled with substantial reductions (up to 40%) in lattice thermal conductivity, increases the maximum figure-of-merit by 300%, to zT ≈ 0.3 at 673 K for Cu(0.96)Sn(0.04)FeS(2).