2013
DOI: 10.1063/1.4799673
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Graphene: Why buckling occurs?

Abstract: We report here the buckling phenomenon of a monolayer graphene with four free edges subjected to uniaxial tension by molecular dynamics simulations. We find that the buckling occurs when tension force is applied and is sufficiently large for both armchair and zigzag single layer graphene sheets. The maximum amplitude is increased and the maximum wavelength is decreased with increase in temperature.

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Cited by 14 publications
(9 citation statements)
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“…These simulations were based on abinitio, [26][27][28] tight-binding, [29][30][31][32] and empirical interatomic potentials. 9,[33][34][35][36] In most cases, carbon atoms were described as classical particles, which is reliable at relatively high temperatures (in the order of the Debye temperature of the material), but is not suitable to study thermodynamic variables at low temperature. To take into account the quantum nature of the atomic motion, pathintegral simulations are well-suited, since in this procedure nuclear degrees of freedom may be quantized, allowing one to include quantum and thermal fluctuations in many-body systems at finite temperatures.…”
Section: Introductionmentioning
confidence: 99%
“…These simulations were based on abinitio, [26][27][28] tight-binding, [29][30][31][32] and empirical interatomic potentials. 9,[33][34][35][36] In most cases, carbon atoms were described as classical particles, which is reliable at relatively high temperatures (in the order of the Debye temperature of the material), but is not suitable to study thermodynamic variables at low temperature. To take into account the quantum nature of the atomic motion, pathintegral simulations are well-suited, since in this procedure nuclear degrees of freedom may be quantized, allowing one to include quantum and thermal fluctuations in many-body systems at finite temperatures.…”
Section: Introductionmentioning
confidence: 99%
“…[17][18][19][20] Finite-temperature properties of graphene have been studied by molecular dynamics and Monte Carlo simulations using ab-initio, [21][22][23] tight binding, [24][25][26][27] and empirical interatomic potentials. 5,[28][29][30][31][32] In most applications of these methods, atomic nuclei were described as classical particles. To take into account the quantum character of the nuclei, path-integral (both, molecular dynamics and Monte Carlo) simulations turn out to be particularly suitable.…”
Section: Introductionmentioning
confidence: 99%
“…The reconstruction process (see Section 19.4) is analogous to, but different from, the formation of a Thrower-Stone-Wales (TSW) defect [111,112]: As illustrated in Fig. This in turn results in significant graphene buckling and thus emphasizes the "chemical" in addition to the physical ori- gin of this intriguing phenomenon [113]. This in turn results in significant graphene buckling and thus emphasizes the "chemical" in addition to the physical ori- gin of this intriguing phenomenon [113].…”
Section: Internal Edgesmentioning
confidence: 99%