dc.contributor.author |
Hegde, Vinay I.
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|
dc.contributor.author |
Shirodkar, Sharmila N.
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|
dc.contributor.author |
Tit, Nacir
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|
dc.contributor.author |
Waghmare, Umesh V.
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dc.contributor.author |
Yamani, Zain H.
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dc.date.accessioned |
2017-02-21T09:03:22Z |
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dc.date.available |
2017-02-21T09:03:22Z |
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dc.date.issued |
2014 |
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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 |
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dc.identifier.uri |
https://libjncir.jncasr.ac.in/xmlui/10572/2562 |
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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 |