Geometric and electronic structures of monolayer hexagonal boron nitride with multi-vacancyopen access
- Authors
- Kim, Do-Hyun; Kim, Hag-Soo; Song, Min Woo; Lee, Seunghyun; Lee, Sang Yun
- Issue Date
- May-2017
- Publisher
- Springer | Korea Nano Technology Research Society
- Keywords
- Boron nitride; Vacancy; Defect; Deformation; Band structure
- Citation
- Nano Convergence, v.4, pp 1 - 8
- Pages
- 8
- Indexed
- SCIE
KCI
- Journal Title
- Nano Convergence
- Volume
- 4
- Start Page
- 1
- End Page
- 8
- URI
- https://scholarworks.bwise.kr/erica/handle/2021.sw.erica/12064
- DOI
- 10.1186/s40580-017-0107-0
- ISSN
- 2196-5404
- Abstract
- Hexagonal boron nitride (h-BN) is an electrical insulator with a large band gap of 5 eV and a good thermal conductor of which melting point reaches about 3000 degrees C. Due to these properties, much attention was given to the thermal stability rather than the electrical properties of h-BN experimentally and theoretically. In this study, we report calculations that the electronic structure of monolayer h-BN can be influenced by the presence of a vacancy defect which leads to a geometric deformation in the hexagonal lattice structure. The vacancy was varied from mono- to tri-vacancy in a supercell, and different defective structures under the same vacancy density were considered in the case of an odd number of vacancies. Consequently, all cases of vacancy defects resulted in a geometric distortion in monolayer h-BN, and new energy states were created between valence and conduction band with the Fermi level shift. Notably, B atoms around vacancies attracted one another while repulsion happened between N atoms around vacancies, irrespective of vacancy density. The calculation of formation energy revealed that multi-vacancy including more B-vacancies has much lower formation energy than vacancies with more N-vacancies. This work suggests that multi-vacancy created in monolayer h-BN will have more B-vacancies and that the presence of multi-vacancy can make monolayer h-BN electrically conductive by the new energy states and the Fermi level shift.
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