Discordant nature of Cd in GeTe enhances phonon scattering and improves band convergence for high thermoelectric performance. Issue 3 (20th December 2019)

• Record Type: Journal Article
• Authors: Nshimyimana, Evariste; Hao, Shiqiang; Su, Xianli; Zhang, Cheng; Liu, Wei; Yan, Yonggao; Uher, Ctirad; Wolverton, Chris; Kanatzidis, Mercouri G.; Tang, Xinfeng
• Is Part Of: Journal of materials chemistry. Volume 8:Issue 3(2020)
• Page Start: 1193
• Page End: 1204
• Publication Date: 2019-12-20
• Subjects: Materials -- Research -- Periodicals; Chemistry, Analytic -- Periodicals; Environmental sciences -- Research -- Periodicals; 543.0284
• DOI: 10.1039/c9ta10436d
• Languages: English
• ISSNs: 2050-7488

Abstract

Abstract : Alloying CdTe in GeTe promotes the band convergence and intensifies phonon scattering due to the discordant nature of Cd in GeTe. Upon optimizing carrier concentration via Sb doping, we obtain a peak ZT of 1.8 at 700 K and a high average ZT of 1.3. Abstract : GeTe-based thermoelectric materials tend to be naturally heavily hole doped because of Ge lattice vacancies, and this complicates efforts to improve the figure of merit ZT . Herein, we report that partial substitution of Cd for Ge and doping with Sb can synergistically reduce the density of holes and improve the thermoelectric transport properties of GeTe. Density functional theory electronic structure calculations suggest that when Cd partially substitutes for Ge and forms Cd x Ge1− x Te, the energy offset between the light and heavy valence bands in both rhombohedral and cubic structures is reduced, promoting multi-band conduction that increases the hole carrier effective mass from 1.44 m 0 for pristine GeTe to 2.32 m 0 for Cd0.05 Ge0.95 Te. The ensuing valence band convergence enhances the Seebeck coefficient and yields a high power factor of 44.5 μW cm −1 K −2 at 800 K. Moreover, DFT calculations show a downward energy profile, indicating that as Cd enters the GeTe lattice it tends to move towards a hypothetical octahedral center to make six equal Cd–Te bonds. Such a local distortion in combination with the large mass and size difference between Ge and Cd strongly intensifies phonon scattering by point defects, lowering the lattice thermal conductivity in Cd x Ge1− x Te. Subsequent Sb doping in Cd0.03 Ge0.97− y Sb y Te reduces the inherent high carrier concentration in GeTe, leading to a remarkable enhancement of the Seebeck coefficient and the power factor over a wide temperature range. Furthermore, doping with Sb in Cd0.03 Ge0.97− y Sb y Te introduces additional point defect phonon scattering that results in an extremely low lattice thermal conductivity ∼ 0.71 W m −1 K −1 at 700 K for the Cd0.03 Ge0.89 Sb0.08 Te sample. All those factors lead to a high thermoelectric figure of merit, ZT ∼ 1.8 at 700 K, and a high average ZT of 1.3 in the temperature interval of 400–800 K attained in Cd0.03 Ge0.89 Sb0.08 Te.