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Stacking stability of C(2)N bilayer nanosheet

In recent years, a 2D graphene-like sheet: monolayer C(2)N was synthesized via a simple wet-chemical reaction. Here, we studied the stability and electronic properties of bilayer C(2)N. According to a previous study, a bilayer may exist in one of three highly symmetric stacking configurations, namel...

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Detalles Bibliográficos
Autores principales: Dabsamut, Klichchupong, T-Thienprasert, Jiraroj, Jungthawan, Sirichok, Boonchun, Adisak
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6497902/
https://www.ncbi.nlm.nih.gov/pubmed/31048761
http://dx.doi.org/10.1038/s41598-019-43363-8
Descripción
Sumario:In recent years, a 2D graphene-like sheet: monolayer C(2)N was synthesized via a simple wet-chemical reaction. Here, we studied the stability and electronic properties of bilayer C(2)N. According to a previous study, a bilayer may exist in one of three highly symmetric stacking configurations, namely as AA, AB and AB′-stacking. For the AA-stacking, the top layer is directly stacked on the bottom layer. Furthermore, AB- and AB′-stacking can be obtained by shifting the top layer of AA-stacking by a/3-b/3 along zigzag direction and by a/2 along armchair direction, respectively, where a and b are translation vectors of the unit cell. By using first-principles calculations, we calculated the stability of AA, AB and AB′-stacking C(2)N and their electronic band structure. We found that the AB-stacking is the most favorable structure and has the highest band gap, which appeared to agree with previous study. Nevertheless, we furthermore examine the energy landscape and translation sliding barriers between stacking layers. From energy profiles, we interestingly found that the most stable positions are shifted from the high symmetry AB-stacking. In electronic band structure details, band characteristic can be modified according to the shift. The interlayer shear mode close to local minimum point was determined to be roughly 2.02 × 10(12) rad/s.