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dc.contributor.authorJamwal, Gauraven_US
dc.contributor.authorKUMAR, ANKITen_US
dc.contributor.authorWarish, Mohd.en_US
dc.contributor.authorCHAKRAVARTY, SHRUTIen_US
dc.contributor.authorMuthiah, Saravananen_US
dc.contributor.authorKandasami, Asokanen_US
dc.contributor.authorNiazi, Asaden_US
dc.date.accessioned2023-05-31T09:02:39Z
dc.date.available2023-05-31T09:02:39Z
dc.date.issued2023-09en_US
dc.identifier.citationJournal of Alloys and Compounds, 954, 170182.en_US
dc.identifier.issn0925-8388en_US
dc.identifier.issn1873-4669en_US
dc.identifier.urihttps://doi.org/10.1016/j.jallcom.2023.170182en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/8009
dc.description.abstractThe low bandgap semiconductor, SnTe is receiving significant attention as a thermoelectric material be-cause of its low toxicity and environment-friendly nature. In this study, we report the effect of co-doping dilute concentrations of Ag and Cu ions in SnTe that suppresses the Sn vacancies leading to optimized thermoelectric properties. Samples of nominal chemical composition Sn1.03-2xAgxCuxTe (x = 0, 0.01, 0.02, 0.04) were prepared by the solid-state route. The Rietveld refinement of powder XRD of these compounds showed a fcc (Fm3 over bar m) structure with no other impurity phases. Diffuse reflectance IR spectroscopy showed an increase in the bandgap upon Ag-Cu co-doping in SnTe, associated with valence band convergence. Electronic band structure calculations confirmed an increase in the bandgap along with a reduction in the energy difference between light and heavy valence bands having maxima at the L and sigma points. Partial density of states (P-DOS) calculations showed that Ag-Cu doping in SnTe does not contribute towards the formation of resonant energy levels. The Seebeck coefficient S of the Sn1.01Ag0.01Cu0.01Te reached a max-imum value of similar to 95 mu V/K at 783 K, compared to 86 mu V/K of pure SnTe. The power factor increased with the doping concentration, reaching similar to 10.8 mu WK-2cm-1 at 783 K for x = 0.04. The lattice thermal conductivity L decreased on Ag-Cu co-doping, with L = 0.44 Wm 1K 1 above 750 K for x = 0.04, which is close to the Cahill model. The combination of higher power factor and reduced lattice thermal conductivity in the Ag-Cu co-doped samples resulted in enhanced ZT = 0.24-0.29 at 773 K.en_US
dc.language.isoenen_US
dc.publisherElsevier B.V.en_US
dc.subjectThermoelectricityen_US
dc.subjectAg-Cu co-doped SnTeen_US
dc.subjectBand structure calculationsen_US
dc.subjectBand convergenceen_US
dc.subjectReduced thermal conductivityen_US
dc.subjectFigure of meriten_US
dc.subject2023-MAY-WEEK4en_US
dc.subjectTOC-MAY-2023en_US
dc.subject2023en_US
dc.titleStructural, electronic and thermoelectric properties of SnTe with dilute co-doping of Ag and Cuen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleJournal of Alloys and Compoundsen_US
dc.publication.originofpublisherForeignen_US
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