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Peierls-Type Instability and Tunable Band Gap in Functionalized Graphene

2010/04/30 by Dmitry A. Abanin, D. A. Abanin, A. V. Shytov +2 · 61 citations
Materials Science · Physics and Astronomy · #Band gap #Condensed matter physics #Doping #Effective mass (spring–mass system) #Electron #Electronic band structure #Graphene #Graphene research and applications #Instability #Materials science #Nanotechnology #Physics #Quantum and electron transport phenomena #Quantum mechanics #Scattering #Topological Materials and Phenomena #cond-mat.mes-hall

paper · pdf · doi:10.1103/physrevlett.105.086802

published in Physical Review Letters 105(8), 086802 (American Physical Society) · 6 pgs, 3 fgs

arxiv created 2010/08/10 · openalex publication_date 2010/08/18 · arxiv updated 2010/08/30 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05

Abstract

Functionalizing graphene was recently shown to have a dramatic effect on the electronic properties of this material. Here we investigate spatial ordering of adatoms driven by the RKKY-type interactions. In the ordered state, which arises via a Peierls-instability-type mechanism, the adatoms reside mainly on one of the two graphene sublattices. Bragg scattering of electron waves induced by sublattice symmetry breaking results in a band gap opening, whereby Dirac fermions acquire a finite mass. The band gap is found to be immune to the adatoms' positional disorder, with only an exponentially small number of localized states residing in the gap. The gapped state is stabilized in a wide range of electron doping. Our findings show that controlled adsorption of adatoms or molecules provides a route to engineering a tunable band gap in graphene.

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