2019
DOI: 10.1039/c8ra08076c
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Atomistic insights into the anisotropic mechanical properties and role of ripples on the thermal expansion of h-BCN monolayers

Abstract: 2D h-BCN is a novel planar semi-conducting material akin to graphene and h-BN with high thermal mechanical stability suitable for the design of h-BCN-based composite materials.

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Cited by 43 publications
(64 citation statements)
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“…35 The higher stability of configuration (a) was also previously reported on the basis of the computed electronic energy and relative cohesive energy. 34,38 Our cohesive energy calculations yielded a value of À8.38 eV per atom for the BCN unit cell of configuration (a), which is comparable to our calculated value of graphene (À8.9 eV). The reported value for graphene is around À8.1 eV.…”
Section: Computational Detailssupporting
confidence: 82%
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“…35 The higher stability of configuration (a) was also previously reported on the basis of the computed electronic energy and relative cohesive energy. 34,38 Our cohesive energy calculations yielded a value of À8.38 eV per atom for the BCN unit cell of configuration (a), which is comparable to our calculated value of graphene (À8.9 eV). The reported value for graphene is around À8.1 eV.…”
Section: Computational Detailssupporting
confidence: 82%
“…34 Apart from these features, BCN shows higher directional anisotropy than graphene, suggesting a lower barrier for ion diffusion. 38 Moreover, BCN has a smaller Young's modulus value and higher flexibility than graphene, which justifies its mechanical stability. 38 All of these properties suggest that the BCN monolayer may be a potential electrode material candidate.…”
Section: Introductionmentioning
confidence: 99%
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“…To analyze the mechanical features, we calculated the linear elastic constants using the energy‐strain method. [ 51–54 ] The computed elastic constants of both pristine and vacancy defect filled Ti 2 C and Ti 2 CT 2 (T = O − , F − ) MXenes are satisfying the relation: C11C12C122>0, C66>0, confirming that the structures are mechanically stable according to the Born–Huang criteria. [ 55,56 ] We also derived the in‐plane Young's moduli along the (100) and (010) directions (YM A and YM B ) using the relation: YM A = ( C 11 2 − C 12 2 )/ C 11 and YM B = ( C 22 2 − C 12 2 )/ C 22 .…”
Section: Resultsmentioning
confidence: 87%
“…These considerable anisotropic mechanical behaviors along the two different chiral orientations are very similar to other 2D systems. 22 , 42 , 43 The relative variation of computed stress along the armchair and zigzag directions can be explained using Figure 2 b,c. In the armchair orientation, six stress-conveying bonds are contained in every unit cell, among which four bonds have a comparative angle of 60° with the armchair orientation and the other two are parallel to the armchair orientation (shown in Figure 2 b).…”
Section: Resultsmentioning
confidence: 99%