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石墨烯中的临界曲率定位。I. 量子挠曲电效应。

Critical curvature localization in graphene. I. Quantum-flexoelectricity effect.

作者信息

Kothari Mrityunjay, Cha Moon-Hyun, Kim Kyung-Suk

机构信息

School of Engineering, Brown University, Providence, RI 02912, USA.

出版信息

Proc Math Phys Eng Sci. 2018 Jun;474(2214):20180054. doi: 10.1098/rspa.2018.0054. Epub 2018 Jun 27.

Abstract

Here, we report the discovery of a new, curvature-localizing, subcritical buckling mode that produces shallow-kink corrugation in multi-layer graphene. Our density functional theory (DFT) analysis reveals the mode configuration-an approximately 2 nm wide boundary layer of highly localized curvature that connects two regions of uniformly but oppositely sheared stacks of flat atomic sheets. The kink angle between the two regions is limited to a few degrees, ensuring elastic deformation. By contrast, a purely mechanical model of sandwich structures shows progressive supercritical curvature localization spread over a 50-100 nm wide boundary layer. Our effective-locality model of electromechanics reveals that coupling between atomic-layer curvature and electric-charge polarization, i.e. quantum flexoelectricity, leads to emergence of a boundary layer in which curvature is focused primarily within a 0.86 nm fixed band width. Both DFT and the model analyses show focused distributions of curvature and polarization exhibiting oscillating decay within the approximately 2 nm wide boundary layer. The results show that dipole-dipole interaction lowers the potential energy with such a distribution. Furthermore, this model predicts peak-polarization density approximately 0.12 e nm for 3° tilt angle. This high polarization concentration can be controlled by macroscopic deformation and is expected to be useful in studies of selective graphene-surface functionalization for various applications.

摘要

在此,我们报告发现了一种新的、曲率局部化的亚临界屈曲模式,该模式在多层石墨烯中产生浅扭结波纹。我们的密度泛函理论(DFT)分析揭示了模式构型——一个宽度约为2纳米的高度局部化曲率的边界层,它连接了两个均匀但方向相反的扁平原子片层堆叠区域。这两个区域之间的扭结角限制在几度以内,确保了弹性变形。相比之下,夹层结构的纯力学模型显示,渐进的超临界曲率局部化分布在一个宽度为50 - 100纳米的边界层上。我们的机电有效局部性模型表明,原子层曲率与电荷极化之间的耦合,即量子挠曲电效应,导致出现一个边界层,其中曲率主要集中在一个0.86纳米的固定带宽内。DFT和模型分析均表明,在约2纳米宽的边界层内,曲率和极化的分布呈集中状态,并表现出振荡衰减。结果表明,偶极 - 偶极相互作用通过这种分布降低了势能。此外,该模型预测对于3°倾斜角,峰值极化密度约为0.12 e/nm。这种高极化浓度可通过宏观变形来控制,预计在各种应用的选择性石墨烯表面功能化研究中会很有用。

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本文引用的文献

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Fundamentals of flexoelectricity in solids.固体的挠曲电基础。
Nanotechnology. 2013 Nov 1;24(43):432001. doi: 10.1088/0957-4484/24/43/432001. Epub 2013 Oct 2.
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