We study the electronic structure of graphene with a single substitutional vacancy using a combination of the density-functional, tight-binding and impurity Green's function approaches. Density-functional studies are performed with the all-electron spin-polarized linear augmented plane wave (LAPW) method. The three sp 2 dangling bonds adjacent to the vacancy introduce localized states (V ) in the mid-gap region, which split due to the crystal field and a Jahn-Teller distortion, while the p z states introduce a sharp resonance state (V ) in the band structure. For a planar structure, symmetry strictly forbids hybridization between the and the states, so that these bands are clearly identifiable in the calculated band structure. As to the magnetic moment of the vacancy, the Hund's rule coupling aligns the spins of the four localized V 1 , V 2 and V electrons, resulting in an S = 1 state, with a magnetic moment of 2 B , which is reduced by about 0.3 B due to the anti-ferromagnetic spin polarization of the band itinerant states in the vicinity of the vacancy. This results in the net magnetic moment of 1.7 B . Using the Lippmann-Schwinger equation, we reproduce the well-known 1/r decay of the localized V wave function with distance, and in addition, find an
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Nanda et al. (2012) studied this question.
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