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Metavalent Bonding in GeSe Leads to High Thermoelectric Performance
Author(s) -
Sarkar Debattam,
Roychowdhury Subhajit,
Arora Raagya,
Ghosh Tanmoy,
Vasdev Aastha,
Joseph Boby,
Sheet Goutam,
Waghmare Umesh V.,
Biswas Kanishka
Publication year - 2021
Publication title -
angewandte chemie international edition
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 5.831
H-Index - 550
eISSN - 1521-3773
pISSN - 1433-7851
DOI - 10.1002/anie.202101283
Subject(s) - materials science , orthorhombic crystal system , condensed matter physics , ferroelectricity , thermoelectric effect , band gap , phonon , seebeck coefficient , dielectric , thermoelectric materials , crystallography , thermal conductivity , crystal structure , chemistry , optoelectronics , thermodynamics , physics , composite material
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 (AgBiTe 2 ) 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 (AgBiTe 2 ) x . The structural transformation accompanies change from covalent bonding in orthorhombic GeSe to metavalent bonding in rhombohedral (GeSe) 1− x (AgBiTe 2 ) x . (GeSe) 0.9 (AgBiTe 2 ) 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 (AgBiTe 2 ) 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.