2014
DOI: 10.1063/1.4873435
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Physical origins of weak H2 binding on carbon nanostructures: Insight from ab initio studies of chemically functionalized graphene nanoribbons

Abstract: We have performed ab initio density functional theory calculations, incorporating London dispersion corrections, to study the absorption of molecular hydrogen on zigzag graphene nanoribbons whose edges have been functionalized by OH, NH2, COOH, NO2, or H2PO3. We find that hydrogen molecules always preferentially bind at or near the functionalized edge, and display induced dipole moments. Binding is generally enhanced by the presence of polar functional groups. The largest gains are observed for groups with oxy… Show more

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Cited by 17 publications
(12 citation statements)
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“…This strategy is best justified if the dominant physical interaction is relatively short-range; examples include interactions with specific functional groups or substitutional defects that introduce polarization and/or partial charge transfer. 120 The actual material may incorporate many different types of functional groups or defects, which can be investigated within the fragment models. However, because this approach does not generate an integrated material model, one cannot utilize GCMC simulations to simulate isotherms over the full pressure range.…”
Section: 117mentioning
confidence: 99%
“…This strategy is best justified if the dominant physical interaction is relatively short-range; examples include interactions with specific functional groups or substitutional defects that introduce polarization and/or partial charge transfer. 120 The actual material may incorporate many different types of functional groups or defects, which can be investigated within the fragment models. However, because this approach does not generate an integrated material model, one cannot utilize GCMC simulations to simulate isotherms over the full pressure range.…”
Section: 117mentioning
confidence: 99%
“…This induced dipole on H 2 molecules signifies that it is the electrostatic interaction that binds the H 2 molecules to the COBN surface 48. This induced dipole on H 2 molecules signifies that it is the electrostatic interaction that binds the H 2 molecules to the COBN surface 48.…”
mentioning
confidence: 99%
“… 34 , as energetic H 2 molecules at the tail of the thermal distribution collide with the graphene surface, the proximity of their approach alleviates the need to overcome the H 2 high dissociation barrier (~4.12 eV) 34 as long as an energetically favourable defective binding site is present. The induced polarization of H 2 near defective sites may also assist in low-temperature dissociation 35 36 . Accordingly, the necessary energetics for dissociation H 2 on defective binding sites need only be on the order of the bond energy difference between H in H 2 and in defective graphene.…”
Section: Discussionmentioning
confidence: 99%