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Tuning the bandgap and introducing magnetism into monolayer BC3 by strain/defect engineering and adatom/molecule adsorption

Authors
Bafekry A.[Bafekry A.]Farjami Shayesteh S.[Farjami Shayesteh S.]Ghergherehchi M.[Ghergherehchi M.]Peeters F.M.[Peeters F.M.]
Issue Date
14-Oct-2019
Publisher
American Institute of Physics Inc.
Citation
Journal of Applied Physics, v.126, no.14
Indexed
SCIE
SCOPUS
Journal Title
Journal of Applied Physics
Volume
126
Number
14
URI
https://scholarworks.bwise.kr/skku/handle/2021.sw.skku/13490
DOI
10.1063/1.5097264
ISSN
0021-8979
Abstract
Using first-principles calculations, we study the structural, electronic, and optical properties of pristine BC 3. Our results show that BC 3 is a semiconductor which can be useful in optoelectronic device applications. Furthermore, we found that the electronic properties of BC 3 can be modified by strain and the type of edge states. With increasing thickness, the indirect bandgap decreases from 0.7 eV (monolayer) to 0.27 eV (bulk). Upon uniaxial tensile strain along the armchair and zigzag directions, the bandgap slightly decreases, and with increasing uniaxial strain, the bandgap decreases, and when reaching - 8 %, a semiconductor-to-metal transition occurs. By contrast, under biaxial strain, the bandgap increases to 1.2 eV in + 8 % and decreases to zero in - 8 %. BC 3 nanoribbons with different widths exhibit magnetism at the zigzag edges, while, at the armchair edges, they become semiconductor, and the bandgap is in the range of 1.0-1.2 eV. Moreover, we systematically investigated the effects of adatoms/molecule adsorption and defects on the structural, electronic, and magnetic properties of BC 3. The adsorption of various adatoms and molecules as well as topological defects (vacancies and Stone-Wales defects) can modify the electronic properties. Using these methods, one can tune BC 3 into a metal, half-metal, ferromagnetic-metal, and dilute-magnetic semiconductor or preserve its semiconducting character. © 2019 Author(s).
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