CoTeO4 – a wide-bandgap material adopting the dirutile structure type
Weil, Matthias; Pramanik, Prativa; Maltoni, Pierfrancesco; Clulow, Rebecca; Rydh, Andreas; Wildner, Manfred; Blaha, Peter; King, Graham; Ivanov, Sergey A.; Mathieu, Roland; Singh, Harishchandra (2024-02-28)
Weil, Matthias
Pramanik, Prativa
Maltoni, Pierfrancesco
Clulow, Rebecca
Rydh, Andreas
Wildner, Manfred
Blaha, Peter
King, Graham
Ivanov, Sergey A.
Mathieu, Roland
Singh, Harishchandra
Royal society of chemistry
28.02.2024
Mater. Adv., 2024, 5, 3001-3013, https://doi.org/10.1039/D3MA01106B
https://creativecommons.org/licenses/by-nc/3.0/
© 2024 The Author(s). Published by the Royal Society of Chemistry . This article is licensed under a Creative Commons Attribution-NonCommercial 3.0 Unported Licence.
https://creativecommons.org/licenses/by-nc/3.0/
© 2024 The Author(s). Published by the Royal Society of Chemistry . This article is licensed under a Creative Commons Attribution-NonCommercial 3.0 Unported Licence.
https://creativecommons.org/licenses/by-nc/3.0/
Julkaisun pysyvä osoite on
https://urn.fi/URN:NBN:fi:oulu-202404092613
https://urn.fi/URN:NBN:fi:oulu-202404092613
Tiivistelmä
Abstract
High-quality crystals of CoTeO4 were grown by application of chemical vapor transport reactions in closed silica ampoules, starting from polycrystalline material in a temperature gradient 640 °C → 580 °C with TeCl4 as transport agent. Crystal structure analysis of CoTeO4 from single crystal X-ray data revealed a dirutile-type structure with CoII and TeVI atoms at crystallographically distinct sites, each with point group symmetry [1 with combining macron]. The statistical significance and accuracy of the previously reported structural model based on powder data with the ordered arrangement of Co and Te cations was noticeably improved. CoTeO4 does not undergo a structural phase transition upon heating, but decomposes stepwise (Co2Te3O8 as intermediate phase) to Co3TeO6 as the only crystalline phase stable above 770 °C. Temperature-dependent magnetic susceptibility and dielectric measurements suggest antiferromagnetic ordering at ∼50 K. Optical absorption spectroscopy and computational studies reveal wide-band semiconductive behavior for CoTeO4. The experimentally determined band gap of ∼2.42 eV is also found for CdS, which is frequently used in photovoltaic systems but is hazardous to the environment. Hence, CoTeO4 might be a possible candidate to replace CdS in this regard.
High-quality crystals of CoTeO4 were grown by application of chemical vapor transport reactions in closed silica ampoules, starting from polycrystalline material in a temperature gradient 640 °C → 580 °C with TeCl4 as transport agent. Crystal structure analysis of CoTeO4 from single crystal X-ray data revealed a dirutile-type structure with CoII and TeVI atoms at crystallographically distinct sites, each with point group symmetry [1 with combining macron]. The statistical significance and accuracy of the previously reported structural model based on powder data with the ordered arrangement of Co and Te cations was noticeably improved. CoTeO4 does not undergo a structural phase transition upon heating, but decomposes stepwise (Co2Te3O8 as intermediate phase) to Co3TeO6 as the only crystalline phase stable above 770 °C. Temperature-dependent magnetic susceptibility and dielectric measurements suggest antiferromagnetic ordering at ∼50 K. Optical absorption spectroscopy and computational studies reveal wide-band semiconductive behavior for CoTeO4. The experimentally determined band gap of ∼2.42 eV is also found for CdS, which is frequently used in photovoltaic systems but is hazardous to the environment. Hence, CoTeO4 might be a possible candidate to replace CdS in this regard.
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