2011
DOI: 10.1016/j.carbon.2010.08.042
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Bending modes, elastic constants and mechanical stability of graphitic systems

Abstract: The thermodynamic and mechanical properties of graphitic systems are strongly dependent on the shear elastic constant C44. Using state-of-the-art density functional calculations, we provide the first complete determination of their elastic constants and exfoliation energies. We show that stacking misorientations lead to a severe lowering of C44 of at least one order of magnitude. The lower exfoliation energy and the lower C44 (more bending modes) suggest that flakes with random stacking should be easier to exf… Show more

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Cited by 158 publications
(125 citation statements)
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“…[128] 1079 ± 5 124 ± 5 578 ± 2 The best functional for describing simultaneously the elastic constants of both graphite and diamond is the PBE+D3+BJ, although the other C 6 functionals perform reasonably well and the non-local functional perform worse, albeit giving an improved description compared to LDA. These results are in good agreement with other theoretical works [129,130]. …”
Section: Elastic Constantssupporting
confidence: 82%
“…[128] 1079 ± 5 124 ± 5 578 ± 2 The best functional for describing simultaneously the elastic constants of both graphite and diamond is the PBE+D3+BJ, although the other C 6 functionals perform reasonably well and the non-local functional perform worse, albeit giving an improved description compared to LDA. These results are in good agreement with other theoretical works [129,130]. …”
Section: Elastic Constantssupporting
confidence: 82%
“…(2) yields κ = (0.69 ± 0.01) eV per layer and C 44 = (5.8 ± 0.02) × 10 8 Pa. This value of C 44 is much lower than the experimental value of 5.03 × 10 9 Pa [39] due to the too small corrugation energy of LCBOPII which gives a difference of about 1.5 meV/atom against about 10 meV/atom [46,47]between AA and AB graphite stacking. As a consequence, the transverse modes of graphite for wavevectors parallel to the c-axis shown in the inset of Fig.…”
Section: Quadratic Za Dispersion and Bending Rigiditymentioning
confidence: 89%
“…The first one is due to the small overlaps between the electronic densities of the two subsystems, leading to a small covalence which is repulsive in the case of graphitic materials. [40][41][42] This contribution has been treated perturbatively, by expanding the wave-functions and consequently the operators with respect to the overlaps. The second contribution arises from the charge fluctuations in each subsystem, which generate quantum dipole-dipole interactions.…”
Section: B Interaction Energy and Van Der Waals Forcesmentioning
confidence: 99%