2019
DOI: 10.1080/00268976.2019.1567848
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The characterization of electronic defect states of single and double carbon vacancies in graphene sheets using molecular density functional theory

Abstract: Lischka (2019) The characterization of electronic defect states of single and double carbon vacancies in graphene sheets using molecular density functional theory, Molecular

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Cited by 12 publications
(9 citation statements)
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References 69 publications
(76 reference statements)
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“…line defect or planar defects). [31][32][33][34][35][36][37][38] Raman spectrum is another effective mean to characterize graphene lattice defects. Two typical Raman features, D and G bands, are excited in the spectra (Figure 4d-f).…”
Section: Resultsmentioning
confidence: 99%
“…line defect or planar defects). [31][32][33][34][35][36][37][38] Raman spectrum is another effective mean to characterize graphene lattice defects. Two typical Raman features, D and G bands, are excited in the spectra (Figure 4d-f).…”
Section: Resultsmentioning
confidence: 99%
“…Such defects change the material’s electronic properties. By the removal of carbon atoms from the regular honeycomb network, , dangling bonds are created, , which lead to an open-shell character of the defects and the induction of magnetism. The open-shell character of the electronic structure leads to the occurrence of low-lying electronic states and gives rise to complex geometric variations. In the case of a single carbon vacancy, one carbon atom is missing in the regular hexagon, and one dangling bond occurs in the relaxed structure.…”
Section: Introductionmentioning
confidence: 99%
“…Since graphene with vacancy is a complex system to analyze experimentally, the theoretical investigation based on the numerical approaches is highly anticipated to be useful. However, the estimated values by the ab-initio DFT calculations are rather widely distributed from 1.0µ B to 2.0µ B [1-5], depending on the use of different types of the exchange potential [6] as well as the treatment of the further corrections for the electron correlation [14,15]. Note also that the size of the free magnetic moment observed experimentally could not be simply estimated theoretically by the static one-body approximation because it fails to describe multiplet electronic structures and Kondo-like physics.…”
Section: Introducionmentioning
confidence: 99%