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Transport properties of doped wide band gap layered oxychalcogenide semiconductors Sr2GaO3CuCh, Sr2ScO3CuCh and Sr2InO3CuCh (Ch = S or Se)

Transport properties of doped wide band gap layered oxychalcogenide semiconductors Sr2GaO3CuCh, Sr2ScO3CuCh and Sr2InO3CuCh (Ch = S or Se)
Transport properties of doped wide band gap layered oxychalcogenide semiconductors Sr2GaO3CuCh, Sr2ScO3CuCh and Sr2InO3CuCh (Ch = S or Se)
The structural, electrical, and optical properties of a series of six layered oxychalcogenides with the general formula Sr2MO3CuCh, where M = Ga, Sc, or In and Ch = S or Se, have been investigated. From this set, we report the structure and properties of Sr2GaO3CuSe for the first time, as well as the full structural details of Sr2ScO3CuSe, which have not previously been available. A systematic study of the suitability of all of the Sr2MO3CuCh phases as p-type conductors has been carried out, after doping with both sodium and potassium to a nominal composition of A0.05Sr1.95MO3CuCh, (A = Na or K), to increase the hole carrier concentration. Density functional theory calculations were used to determine the electronic band structure and predict the transport properties, while optical properties were determined using UV–vis spectroscopy, and structures were confirmed using Rietveld refinement against powder X-ray diffraction data. Room-temperature conductivity measurements were carried out on both pristine samples and doped samples, 18 compositions in total, using four-point probe measurements. We found that the most conductive sample was K0.05Sr1.95GaO3CuSe, with a measured conductivity of 0.46 S cm–1, collected from a sintered pellet. We have also been able to identify a relationship between the conductivity and the geometry of the copper chalcogenide layer within the Sr2MO3CuCh series of compounds. As this geometry can be controlled through the material composition, the identification of this structure–property relationship highlights a route to the selection and identification of materials with even higher conductivities.
0897-4756
11326-11337
Malik, Zahida
22c12dcb-2345-4560-b427-b52d839a53d8
Kemp, Liam
82904c87-e2d8-410b-b338-aa823636fa11
Grosso, Bastien F.
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Davies, Daniel W.
0a08c978-3e9b-4633-8b71-a3c42b9cf5a7
Scanlon, David O.
23dbcc36-0b42-40dc-a3af-64c8bad7beb3
Hyett, Geoffrey
4f292fc9-2198-4b18-99b9-3c74e7dfed8d
Malik, Zahida
22c12dcb-2345-4560-b427-b52d839a53d8
Kemp, Liam
82904c87-e2d8-410b-b338-aa823636fa11
Grosso, Bastien F.
f6984502-7a4a-4dbc-8f78-d2f23e9b5fdb
Davies, Daniel W.
0a08c978-3e9b-4633-8b71-a3c42b9cf5a7
Scanlon, David O.
23dbcc36-0b42-40dc-a3af-64c8bad7beb3
Hyett, Geoffrey
4f292fc9-2198-4b18-99b9-3c74e7dfed8d

Malik, Zahida, Kemp, Liam, Grosso, Bastien F., Davies, Daniel W., Scanlon, David O. and Hyett, Geoffrey (2024) Transport properties of doped wide band gap layered oxychalcogenide semiconductors Sr2GaO3CuCh, Sr2ScO3CuCh and Sr2InO3CuCh (Ch = S or Se). Chemistry of Materials, 36 (22), 11326-11337. (doi:10.1021/acs.chemmater.4c02760).

Record type: Article

Abstract

The structural, electrical, and optical properties of a series of six layered oxychalcogenides with the general formula Sr2MO3CuCh, where M = Ga, Sc, or In and Ch = S or Se, have been investigated. From this set, we report the structure and properties of Sr2GaO3CuSe for the first time, as well as the full structural details of Sr2ScO3CuSe, which have not previously been available. A systematic study of the suitability of all of the Sr2MO3CuCh phases as p-type conductors has been carried out, after doping with both sodium and potassium to a nominal composition of A0.05Sr1.95MO3CuCh, (A = Na or K), to increase the hole carrier concentration. Density functional theory calculations were used to determine the electronic band structure and predict the transport properties, while optical properties were determined using UV–vis spectroscopy, and structures were confirmed using Rietveld refinement against powder X-ray diffraction data. Room-temperature conductivity measurements were carried out on both pristine samples and doped samples, 18 compositions in total, using four-point probe measurements. We found that the most conductive sample was K0.05Sr1.95GaO3CuSe, with a measured conductivity of 0.46 S cm–1, collected from a sintered pellet. We have also been able to identify a relationship between the conductivity and the geometry of the copper chalcogenide layer within the Sr2MO3CuCh series of compounds. As this geometry can be controlled through the material composition, the identification of this structure–property relationship highlights a route to the selection and identification of materials with even higher conductivities.

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Accepted/In Press date: 6 November 2024
e-pub ahead of print date: 13 November 2024
Published date: 14 November 2024

Identifiers

Local EPrints ID: 499378
URI: http://eprints.soton.ac.uk/id/eprint/499378
ISSN: 0897-4756
PURE UUID: 5950f217-5b61-43c7-8e0c-66f764f06138
ORCID for Zahida Malik: ORCID iD orcid.org/0000-0002-1212-6845
ORCID for Geoffrey Hyett: ORCID iD orcid.org/0000-0001-9302-9723

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Date deposited: 18 Mar 2025 17:41
Last modified: 19 Mar 2025 02:54

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Contributors

Author: Zahida Malik ORCID iD
Author: Liam Kemp
Author: Bastien F. Grosso
Author: Daniel W. Davies
Author: David O. Scanlon
Author: Geoffrey Hyett ORCID iD

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