2014
DOI: 10.1134/s0021364014050051
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Bigraphene nanomeshes: Structure, properties, and formation

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Cited by 17 publications
(14 citation statements)
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“…In both cases the band gap tends to zero, because asymptotic limits of Dh and Rh correspond to geometries of metallic bilayered graphene and metallic armchair carbon nanotube (CNT), respectively. Note that in the earlier reports [41,42] bilayered graphene superlattices with rectangular unit cell were studied. All considered structures display semimetal properties besides noncovalent bonded bilayered nanomesh.…”
Section: Calculation Methodsmentioning
confidence: 99%
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“…In both cases the band gap tends to zero, because asymptotic limits of Dh and Rh correspond to geometries of metallic bilayered graphene and metallic armchair carbon nanotube (CNT), respectively. Note that in the earlier reports [41,42] bilayered graphene superlattices with rectangular unit cell were studied. All considered structures display semimetal properties besides noncovalent bonded bilayered nanomesh.…”
Section: Calculation Methodsmentioning
confidence: 99%
“…All considered structures display semimetal properties besides noncovalent bonded bilayered nanomesh. [42] It should be noted, however, that not only the structures with high values of Rh can have low values of the band gap. Decreasing of the size of the holes until point defects (vacancies) leads to an appearance of metallic properties without any dependence on the distance between the vacancies.…”
Section: Calculation Methodsmentioning
confidence: 99%
“…the lack of energy gap, which makes its use in electronics extremely limited. The band structure varies depending on the number of layers, their mutual orientation1 and the presence of periodically arranged holes234.…”
mentioning
confidence: 99%
“…The idea of band gap opening in graphene monolayer by formation of periodically arranged holes (antidots) got a second wind in the bigraphene case. Indeed, while the open edges of holes in a graphene single layer are reactive and require passivation, the edges of bigraphene holes are naturally self-passivated. The energy gain due to the hole active edges connection from both layers sufficiently overcomes the loss in graphene bending energy due to edges curving. Moreover, ab initio calculations predicted that connection of the edges even does not require overcoming any barrier , and, therefore, the hollow sp 2 -hybridized graphene structure forms spontaneously.…”
mentioning
confidence: 99%
“…The electronic properties of the perforated bilayered graphene , distinguish them from single-layered graphene or graphene ribbons, the edges of which induce stress and lead to carriers scattering . Therefore, control of the atomic structure of the hole edges in bigraphene is highly desirable and can yield a new class of carbon nanostructures with attractive electronic properties.…”
mentioning
confidence: 99%