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Mechanical Properties and Atomic Explanation of Plastic Deformation for Diamond-Like BC(2)

Motivated by a recently predicted structure of diamond-like BC(2) with a high claimed hardness of 56 GPa (J. Phys. Chem. C 2010, 114, 22688–22690), we focus on whether this tetragonal BC(2) (t-BC(2)) is superhard or not in spite of such an ultrahigh theoretical hardness. The mechanical properties of...

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Detalles Bibliográficos
Autores principales: Zheng, Baobing, Zhang, Meiguang, Chang, Shaomei
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5456893/
https://www.ncbi.nlm.nih.gov/pubmed/28773636
http://dx.doi.org/10.3390/ma9070514
Descripción
Sumario:Motivated by a recently predicted structure of diamond-like BC(2) with a high claimed hardness of 56 GPa (J. Phys. Chem. C 2010, 114, 22688–22690), we focus on whether this tetragonal BC(2) (t-BC(2)) is superhard or not in spite of such an ultrahigh theoretical hardness. The mechanical properties of t-BC(2) were thus further extended by using the first principles in the framework of density functional theory. Our results suggest that the Young’s and shear moduli of t-BC(2) exhibit a high degree of anisotropy. For the weakest shear direction, t-BC(2) undergoes an electronic instability and structural collapse upon a shear strain of about 0.11, with its theoretically ideal strength of only 36.2 GPa. Specifically, the plastic deformation under shear strain along the (110)[001] direction can be attributed to the breaking of d1 B–C bonds.