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DC Field | Value | Language |
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dc.contributor.author | Bhamu, K. C. | en_US |
dc.contributor.author | Haque, Enamul | en_US |
dc.contributor.author | Praveen, C. S. | en_US |
dc.contributor.author | Kumar, Nandha | en_US |
dc.contributor.author | Yumnam, G. | en_US |
dc.contributor.author | Hossain, Md. Anwar | en_US |
dc.contributor.author | SHARMA, GAUTAM | en_US |
dc.date.accessioned | 2021-03-30T09:16:37Z | |
dc.date.available | 2021-03-30T09:16:37Z | |
dc.date.issued | 2021-01 | en_US |
dc.identifier.citation | RSC Advances, 11(10), 5521-5528. | en_US |
dc.identifier.issn | 2046-2069 | en_US |
dc.identifier.uri | http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/5718 | - |
dc.identifier.uri | https://doi.org/10.1039/D0RA01840F | en_US |
dc.description.abstract | The next-generation indium-based lead-free halide material Cs2InAgCl6 is promising for photovoltaic applications due to its good air stability and non-toxic behavior. However, its wide bandgap (>3 eV) is not suitable for the solar spectrum and hence reduces its photoelectronic efficiency for device applications. Here we report a significant bandgap reduction from 2.85 eV to 0.65 eV via substitutional doping and its effects on the optoelectronic and opto-thermoelectric properties from a first-principles study. The results predict that Sn/Pb and Ga and Cu co-doping will enhance the density of states significantly near the valence band maximum (VBM) and thus reduce the bandgap via shifting the VBM upward, while alkali metals (K/Rb) slightly increase the bandgap. A strong absorption peak near the Shockley–Queisser limit is observed in the co-doped case, while in the Sn/Pb-doped case, we notice a peak in the middle of the visible region of the solar spectrum. The nature of the bandgap is indirect with Cu–Ga/Pb/Sn doping, and a significant reduction in the bandgap, from 2.85 eV to 0.65 eV, is observed in the case of Ga–Cu co-doping. We observe a significant increase in the power factor (PF) (2.03 mW m−1 K−2) for the n-type carrier after Pb-doping, which is ∼3.5 times higher than in the pristine case (0.6 mW m −1 K−2) at 500 K. | en_US |
dc.language.iso | en | en_US |
dc.publisher | Royal Society of Chemistry | en_US |
dc.subject | Chemistry | en_US |
dc.subject | 2021-MAR-WEEK2 | en_US |
dc.subject | TOC-MAR-2021 | en_US |
dc.subject | 2021 | en_US |
dc.title | Improving the optical and thermoelectric properties of Cs2InAgCl6 with heavy substitutional doping: a DFT insight | en_US |
dc.type | Article | en_US |
dc.contributor.department | Dept. of Physics | en_US |
dc.identifier.sourcetitle | RSC Advances | en_US |
dc.publication.originofpublisher | Foreign | en_US |
Appears in Collections: | JOURNAL ARTICLES |
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