Mutual influence of uniaxial tensile strain and point defect pattern on electronic states in graphene |
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Authors: | Iyor Yu. Sagalianov author-information" >,Taras M. Radchenko,Yuriy I. Prylutskyy author-information" >,Valentyn A. Tatarenko author-information" >,Pawel Szroeder author-information" > |
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Affiliation: | 1.Dept. of General Physics, Taras Shevchenko National University of Kyiv,Kyiv,Ukraine;2.Dept. of Metallic State Theory, G. V. Kurdyumov Institute for Metal Physics of N.A.S. of Ukraine,Kyiv,Ukraine;3.Dept. of Biophysics, Institute of Biology and Medicine, Taras Shevchenko National University of Kyiv,Kyiv,Ukraine;4.Institute of Physics, Kazimierz Wielki University,Bydgoszcz,Poland |
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Abstract: | The study deals with electronic properties of uniaxially stressed mono- and multi-layer graphene sheets with various kinds of imperfection: point defects modelled as resonant (neutral) adsorbed atoms or molecules, vacancies, charged impurities, and local distortions. The presence of randomly distributed defects in a strained graphene counteract the band-gap opening and even can suppress the gap occurs when they are absent. However, impurity ordering contributes to the band gap appearance and thereby re-opens the gap being suppressed by random dopants in graphene stretched along zigzag-edge direction. The band gap is found to be non-monotonic with strain in case of mutual action of defect ordering and zigzag deformation. Herewith, the minimal tensile strain required for the band-gap opening (≈12.5%) is smaller than that for defect-free graphene (≈23%), and band gap energy reaches the value predicted for maximal nondestructive strains in the pristine graphene. Effective manipulating the band gap in graphene requires balanced content of ordered dopants: their concentration should be sufficient for a significant sublattice asymmetry effect, but not so much that they may suppress the band gap or transform it into the “quasi- (or pseudo-) gap”. |
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