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DC Field | Value | Language |
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dc.contributor.author | Hegde, Vinay I. | |
dc.contributor.author | Shirodkar, Sharmila N. | |
dc.contributor.author | Tit, Nacir | |
dc.contributor.author | Waghmare, Umesh V. | |
dc.contributor.author | Yamani, Zain H. | |
dc.date.accessioned | 2017-02-21T09:03:22Z | - |
dc.date.available | 2017-02-21T09:03:22Z | - |
dc.date.issued | 2014 | |
dc.identifier.citation | Hegde, VI; Shirodkar, SN; Tit, N; Waghmare, UV; Yamani, ZH, First principles analysis of graphene and its ability to maintain long-ranged interaction with H2S. Surface Science 2014, 621, 168-174, http://dx.doi.org/10.1016/j.susc.2013.11.015 | en_US |
dc.identifier.citation | Surface Science | en_US |
dc.identifier.citation | 621 | en_US |
dc.identifier.issn | 0039-6028 | |
dc.identifier.uri | https://libjncir.jncasr.ac.in/xmlui/10572/2562 | - |
dc.description | Restricted Access | en_US |
dc.description.abstract | We determine the chemical activity of (a) carbon site of pristine graphene, (b) Stone-Wales (SW) defect site, and (c) BN-sites of BN-doped graphene towards adsorption of a toxic gas H2S, through comparative analysis based on first-principles density functional theoretical calculations incorporating van der Waals (vdW) interactions. While the adsorption of H2S is weak at both C and BN sites with a binding energy of 15 k J/mol, it is significantly stronger at the Stone-Wales defect site with a much higher binding energy of 26 k J/mol. This is clearly reflected in the contrasting orientation of H2S molecule in the relaxed geometries: the sulfur atom of H2S is closer to graphene (at a distance 3.14 angstrom) during physisorption at C and BN sites, while the molecule's H atoms come closer to graphene (at a distance 2.84 angstrom) during physisorption at the Stone-Wales defect site. The origin of the stronger binding interaction between H2S and a SW defect site is attributed to two possible reasons: (i) an increase in the vdW interaction; and (ii) the lowering of both energy of the HOMO level and the total energy of the H2S molecule in attaining a stable configuration. Our findings are compared to the available theoretical results and their technological relevance is further discussed. (C) 2013 Published by Elsevier B.V. | en_US |
dc.description.uri | 1879-2758 | en_US |
dc.description.uri | http://dx.doi.org/10.1016/j.susc.2013.11.015 | en_US |
dc.language.iso | English | en_US |
dc.publisher | Elsevier Science Bv | en_US |
dc.rights | @Elsevier Science Bv, 2014 | en_US |
dc.subject | Physical Chemistry | en_US |
dc.subject | Condensed Matter Physics | en_US |
dc.subject | Electronic Structure Of Graphene | en_US |
dc.subject | Impurity And Defect Levels | en_US |
dc.subject | Adsorption Kinetics | en_US |
dc.subject | Desorption Kinetics | en_US |
dc.subject | Carbon Nanotubes | en_US |
dc.subject | Complex Materials | en_US |
dc.subject | Simulations | en_US |
dc.subject | Graphite | en_US |
dc.subject | Hydrogen | en_US |
dc.subject | Vacancy | en_US |
dc.subject | Sensor | en_US |
dc.subject | Films | en_US |
dc.title | First principles analysis of graphene and its ability to maintain long-ranged interaction with H2S | en_US |
dc.type | Article | en_US |
Appears in Collections: | Research Articles (Umesh V. Waghmare) |
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