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DC Field | Value | Language |
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dc.contributor.author | Jamwal, Gaurav | en_US |
dc.contributor.author | KUMAR, ANKIT | en_US |
dc.contributor.author | Warish, Mohd. | en_US |
dc.contributor.author | CHAKRAVARTY, SHRUTI | en_US |
dc.contributor.author | Muthiah, Saravanan | en_US |
dc.contributor.author | Kandasami, Asokan | en_US |
dc.contributor.author | Niazi, Asad | en_US |
dc.date.accessioned | 2023-05-31T09:02:39Z | |
dc.date.available | 2023-05-31T09:02:39Z | |
dc.date.issued | 2023-09 | en_US |
dc.identifier.citation | Journal of Alloys and Compounds, 954, 170182. | en_US |
dc.identifier.issn | 0925-8388 | en_US |
dc.identifier.issn | 1873-4669 | en_US |
dc.identifier.uri | https://doi.org/10.1016/j.jallcom.2023.170182 | en_US |
dc.identifier.uri | http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/8009 | |
dc.description.abstract | The 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.iso | en | en_US |
dc.publisher | Elsevier B.V. | en_US |
dc.subject | Thermoelectricity | en_US |
dc.subject | Ag-Cu co-doped SnTe | en_US |
dc.subject | Band structure calculations | en_US |
dc.subject | Band convergence | en_US |
dc.subject | Reduced thermal conductivity | en_US |
dc.subject | Figure of merit | en_US |
dc.subject | 2023-MAY-WEEK4 | en_US |
dc.subject | TOC-MAY-2023 | en_US |
dc.subject | 2023 | en_US |
dc.title | Structural, electronic and thermoelectric properties of SnTe with dilute co-doping of Ag and Cu | en_US |
dc.type | Article | en_US |
dc.contributor.department | Dept. of Physics | en_US |
dc.identifier.sourcetitle | Journal of Alloys and Compounds | en_US |
dc.publication.originofpublisher | Foreign | en_US |
Appears in Collections: | JOURNAL ARTICLES |
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