Metavalent Bonding in GeSe Leads to High Thermoelectric Performance

Sarkar, Debattam ; Roychowdhury, Subhajit ; Arora, Raagya ; Ghosh, Tanmoy ; Vasdev, Aastha ; Joseph, Boby ; Sheet, Goutam ; Waghmare, Umesh V. ; Biswas, Kanishka (2021) Metavalent Bonding in GeSe Leads to High Thermoelectric Performance Angewandte Chemie International Edition, 60 (18). pp. 10350-10358. ISSN 1433-7851

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Official URL: http://doi.org/10.1002/anie.202101283

Related URL: http://dx.doi.org/10.1002/anie.202101283

Abstract

Orthorhombic GeSe is a promising thermoelectric material. However, large band gap and strong covalent bonding result in a low thermoelectric figure of merit, zT≈0.2. Here, we demonstrate a maximum zT≈1.35 at 627 K in p-type polycrystalline rhombohedral (GeSe)0.9(AgBiTe2)0.1 , which is the highest value reported among GeSe based materials. The rhombohedral phase is stable in ambient conditions for x=0.8–0.29 in (GeSe)1−x(AgBiTe2)x . The structural transformation accompanies change from covalent bonding in orthorhombic GeSe to metavalent bonding in rhombohedral (GeSe)1−x(AgBiTe2)x . (GeSe)0.9(AgBiTe2)0.1 has closely lying primary and secondary valence bands (within 0.25–0.30 eV), which results in high power factor 12.8 μW cm−1 K−2 at 627 K. It also exhibits intrinsically low lattice thermal conductivity (0.38 Wm−1 K−1 at 578 K). Theoretical phonon dispersion calculations reveal vicinity of a ferroelectric instability, with large anomalous Born effective charges and high optical dielectric constant, which, in concurrence with high effective coordination number, low band gap and moderate electrical conductivity, corroborate metavalent bonding in (GeSe)0.9(AgBiTe2)0.1. We confirmed the presence of low energy phonon modes and local ferroelectric domains using heat capacity measurement (3–30 K) and switching spectroscopy in piezoresponse force microscopy, respectively.

Item Type:Article
Source:Copyright of this article belongs to John Wiley & Sons, Inc.
ID Code:128184
Deposited On:03 Nov 2022 05:51
Last Modified:03 Nov 2022 05:51

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