Please use this identifier to cite or link to this item: https://dspace.iiti.ac.in/handle/123456789/9151
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dc.contributor.authorGarg, Priyankaen_US
dc.contributor.authorPathak, Biswarupen_US
dc.date.accessioned2022-03-17T01:00:00Z-
dc.date.accessioned2022-03-21T11:31:19Z-
dc.date.available2022-03-17T01:00:00Z-
dc.date.available2022-03-21T11:31:19Z-
dc.date.issued2017-
dc.identifier.citationGarg, P., Choudhuri, I., Mahata, A., & Pathak, B. (2017). Band gap opening in stanene induced by patterned B-N doping. Physical Chemistry Chemical Physics, 19(5), 3660-3669. doi:10.1039/c6cp07505cen_US
dc.identifier.issn1463-9076-
dc.identifier.otherEID(2-s2.0-85027247068)-
dc.identifier.urihttps://doi.org/10.1039/c6cp07505c-
dc.identifier.urihttps://dspace.iiti.ac.in/handle/123456789/9151-
dc.description.abstractStanene is a quantum spin Hall insulator and a promising material for electronic and optoelectronic devices. Density functional theory (DFT) calculations are performed to study the band gap opening in stanene by elemental mono-doping (B, N) and co-doping (B-N). Different patterned B-N co-doping is studied to change the electronic properties of stanene. A patterned B-N co-doping opens the band gap in stanene and its semiconducting nature persists under strain. Molecular dynamics (MD) simulations are performed to confirm the thermal stability of such a doped system. The stress-strain study indicates that such a doped system is as stable as pure stanene. Our work function calculations show that stanene and doped stanene have a lower work function than graphene and thus are promising materials for photocatalysts and electronic devices. © the Owner Societies 2017.en_US
dc.language.isoenen_US
dc.publisherRoyal Society of Chemistryen_US
dc.sourcePhysical Chemistry Chemical Physicsen_US
dc.titleBand gap opening in stanene induced by patterned B-N dopingen_US
dc.typeJournal Articleen_US
dc.rights.licenseAll Open Access, Green-
Appears in Collections:Department of Chemistry

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