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石墨烯中的临界曲率定位。II. 非局部挠曲电-介电耦合。

Critical curvature localization in graphene. II. Non-local flexoelectricity-dielectricity coupling.

作者信息

Kothari Mrityunjay, Cha Moon-Hyun, Lefevre Victor, 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. 2019 Jan;475(2221):20180671. doi: 10.1098/rspa.2018.0671. Epub 2019 Jan 30.

Abstract

As a sequel of part I (Kothari 2018 , 20180054), we present a general thermodynamic framework of flexoelectric constitutive laws for multi-layered graphene (MLG), and apply these laws to explain the role of crinkles in peculiar molecular adsorption characteristics of highly oriented pyrolytic graphite (HOPG) surfaces. The thermodynamically consistent constitutive laws lead to a non-local interaction model of polarization induced by electromechanical deformation with flexoelectricity-dielectricity coupling. The non-local model predicts curvature and polarization localization along crinkle valleys and ridges very close to those calculated by density functional theory (DFT). Our analysis reveals that the non-local model can be reduced to a simplified uc-local or e-local model (Kothari 2018 , 20180054) only when the curvature distribution is uniform or highly localized. For the non-local model, we calibrated and formulated the layer-number-dependent dielectric and intrinsic flexoelectric coefficients of MLGs. In addition, we also obtained layer-number dependent flexoelectric coefficients for uc-local and e-local models. Our DFT analysis shows that polarization-induced adsorption of neutral molecules at crinkle ridges depends on the molecular weight of the molecule. Furthermore, our detailed study of polarization localization in graphene crinkles enables us to understand previously unexplained self-organized adsorption of C buckyballs in a linear array on an HOPG surface.

摘要

作为第一部分(Kothari,2018,20180054)的续篇,我们提出了多层石墨烯(MLG)挠曲电本构定律的一般热力学框架,并应用这些定律来解释褶皱在高度取向热解石墨(HOPG)表面特殊分子吸附特性中的作用。热力学上一致的本构定律导致了一个由机电变形与挠曲电 - 介电耦合引起的极化非局部相互作用模型。该非局部模型预测的沿褶皱谷和脊的曲率和极化局域化与密度泛函理论(DFT)计算的结果非常接近。我们的分析表明,只有当曲率分布均匀或高度局域化时,非局部模型才能简化为简化的uc - 局部或e - 局部模型(Kothari,2018,20180054)。对于非局部模型,我们校准并制定了多层石墨烯与层数相关的介电系数和固有挠曲电系数。此外,我们还获得了uc - 局部和e - 局部模型的层数相关挠曲电系数。我们的DFT分析表明,褶皱脊处中性分子的极化诱导吸附取决于分子的分子量。此外,我们对石墨烯褶皱中极化局域化的详细研究使我们能够理解先前无法解释的HOPG表面上C巴基球在直线阵列中的自组织吸附现象。

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本文引用的文献

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Critical curvature localization in graphene. I. Quantum-flexoelectricity effect.石墨烯中的临界曲率定位。I. 量子挠曲电效应。
Proc Math Phys Eng Sci. 2018 Jun;474(2214):20180054. doi: 10.1098/rspa.2018.0054. Epub 2018 Jun 27.
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