The discovery of graphene, a single monolayer of graphite, has provided an experimental demonstration of stability of 2D crystals. Although thermal fluctuations of such crystals tend to destroy the long-range order in the system, the crystal can be stabilized by strong anharmonicity effects. This competition is the central issue of the crumpling transition, i.e., a transition between flat and crumpled phases. We show that anharmonicity-controlled fluctuations of a graphene membrane around equilibrium flat phase lead to unusual elastic properties. In particular, we demonstrate that stretching ξ of a flake of graphene is a nonlinear function of the applied tension at small tension: ξ ∝ σ η / ( 2 − η ) and ξ ∝ σ η / ( 8 − η ) for clean and strongly disordered graphene, respectively. Conventional linear Hooke’s law, ξ ∝ σ , is realized at sufficiently large tensions: σ ≫ σ * , where σ * depends both on temperature and on the disorder strength.
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Gornyi et al. (2016) studied this question.
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