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 |