Abstract
The observation of intrinsic magnetic order in graphene and graphene-based materials relies on the formation of magnetic moments and a sufficiently strong mutual interaction. Vacancies are arguably considered the primary source of magnetic moments. Here we present an in-depth density functional theory study of the spin-resolved electronic structure of (monoatomic) vacancies in graphene and bilayer graphene. We use two different methodologies: supercell calculations with the siesta code and cluster-embedded calculations with the alacant package. Our results are conclusive: The vacancy-induced extended π magnetic moments, which present long-range interactions and are capable of magnetic ordering, vanish at any experimentally relevant vacancy concentration. This holds for σ-bond passivated and unpassivated reconstructed vacancies, although, for the unpassivated ones, the disappearance of the π magnetic moments is accompanied by a very large magnetic susceptibility. Only for the unlikely case of a full σ-bond passivation, preventing the reconstruction of the vacancy, a full value of 1 μ B for the π extended magnetic moment is recovered for both monolayer and bilayer cases. Our results put on hold claims of vacancy-induced ferromagnetic or antiferromagnetic order in graphene-based systems, while still leaving the door open to σ-type paramagnetism. © 2012 American Physical Society.
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CITATION STYLE
Palacios, J. J., & Ynduráin, F. (2012). Critical analysis of vacancy-induced magnetism in monolayer and bilayer graphene. Physical Review B - Condensed Matter and Materials Physics, 85(24). https://doi.org/10.1103/PhysRevB.85.245443
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