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The structure of graphene on graphene/C-60/Cu interfaces: a molecular dynamics study

机译:石墨烯/ C-60 / Cu界面上石墨烯结构:分子动力学研究

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Two experimental studies reported the spontaneous formation of amorphous and crystalline structures of C-60 molecules intercalated between graphene and a surface. The findings observed included interesting phenomena ranging from reaction between fullerene C(60)s ('C(60)s' stands for plural of C-60) under graphene to graphene sheets sagging between C(60)s and control of strain in these sheets. Motivated by this work, we performed fully atomistic reactive molecular dynamics simulations to investigate the formation and thermal stability of graphene sheet wrinkles as well as graphene attachment to and detachment from a surface when the sheet is laid over a previously distributed array of C-60 molecules on a copper surface at different temperatures. As graphene compresses the C(60)s against the surface, and graphene attachment to the surface in between C(60)s depends on the height of the wrinkles in the graphene sheet, configurations with both frozen and non-frozen fullerenes were investigated in the simulations in order to examine the experimental result of stable, sagged graphene sheets when the distance between C(60)s is about 4 nm and the height of the wrinkles in the sheet is about 0.8 nm. Below a distance of 4 nm between fullerenes, the graphene is predicted to become locally suspended and less strained. The simulations predict that this happens when the fullerenes can deform under the compressive action of the graphene sheet. If the fullerenes are kept frozen, spontaneous 'blanketing' of graphene is predicted only when the distance between neighbouring C(60)s is equal to or great than about 7 nm. These predictions agree with a mechanical model relating the rigidity of a graphene sheet to the energy of graphene-surface adhesion. This work further reveals the structure of intercalated molecules and the role of stability and sheet wrinkling on the preferred configuration of graphene. This study thus might assist in the development of two-dimensional confined nanoreactors for chemical reactions.
机译:两项实验研究报道了在石墨烯和表面之间嵌入的C-60分子的无定形和结晶结构的自发性形成。观察到的发现包括富勒烯C(60)s('C(60)'('c(60)'('c(60)')在石墨烯下的反应之间的有趣现象,以石墨烯片在C(60)S之间松下的石墨烯片和这些中的控制床单。通过这项工作的激励,我们进行了完全原子的反应性分子动力学模拟,以研究石墨烯片皱纹的形成和热稳定性以及当纸张被铺设在先前分布的C-60分子阵列上时与表面的拆卸在不同温度的铜表面上。作为石墨烯压在表面上的C(60)S压实,并且在C(60)S之间的表面上的石墨烯附着取决于石墨烯片中的皱纹的高度,研究了与冷冻和非冷冻富勒烯的构型当C(60)S的距离约为4nm并且片材中的皱纹的高度约0.8nm时,仿真仿真稳定的稳定的石墨烯片的实验结果。在富勒烯之间低于4nm的距离,预计石墨烯将变得局部悬浮并且减少紧张。模拟预测,当富勒烯可以在石墨烯片的压缩作用下变形时发生这种情况。如果富勒烯保持冷冻,则仅当相邻C(60)S之间的距离等于或大于约7nm时,才预测石墨烯的自发的“绘制”。这些预测与将石墨烯片的刚性相关的机械模型与石墨烯表面粘附的能量相关一致。这项工作进一步揭示了插层分子的结构和稳定性和片材皱折在石墨烯的优选构型中的作用。因此,该研究可能有助于开发二维狭窄纳米反应器进行化学反应。

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