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金纳米棒的偶极子状静电不对称性。

Dipole-like electrostatic asymmetry of gold nanorods.

作者信息

Kim Ji-Young, Han Myung-Geun, Lien Miao-Bin, Magonov Sergei, Zhu Yimei, George Heather, Norris Theodore B, Kotov Nicholas A

机构信息

Department of Materials Science and Engineering, University of Michigan, Ann Arbor, MI 48109, USA.

Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, NY 11973, USA.

出版信息

Sci Adv. 2018 Feb 9;4(2):e1700682. doi: 10.1126/sciadv.1700682. eCollection 2018 Feb.

Abstract

The symmetry of metallic nanocolloids, typically envisaged as simple geometrical shapes, is rarely questioned. However, the symmetry considerations are so essential for understanding their electronic structure, optical properties, and biological effects that it is important to reexamine these foundational assumptions for nanocolloids. Gold nanorods (AuNRs) are generally presumed to have nearly perfect geometry of a cylinder and therefore are centrosymmetric. We show that AuNRs, in fact, have a built-in electrostatic potential gradient on their surface and behave as noncentrosymmetric particles. The electrostatic potential gradient of 0.11 to 0.07 V/nm along the long axes of nanorods is observed by off-axis electron holography. Kelvin probe microscopy, secondary electron imaging, energy-filtered transmission electron microscopy, and plasmon mapping reveal that the axial asymmetry is associated with a consistently unequal number of cetyltrimethylammonium bromide moieties capping the two ends of the AuNRs. Electrostatic field maps simulated for the AuNR surface reproduce the holography images. The dipole-like surface potential gradient explains previously puzzling discrepancies in nonlinear optical effects originating from the noncentrosymmetric nature of AuNRs. Similar considerations of symmetry breaking are applicable to other nanoscale structures for which the property-governing symmetry of the organic shell may differ from the apparent symmetry of inorganic core observed in standard electron microscopy images.

摘要

金属纳米胶体的对称性,通常被设想为简单的几何形状,很少受到质疑。然而,对称性考量对于理解其电子结构、光学性质和生物效应至关重要,因此重新审视这些关于纳米胶体的基本假设很重要。金纳米棒(AuNRs)通常被认为具有近乎完美的圆柱体几何形状,因此是中心对称的。我们表明,事实上,AuNRs在其表面具有内置的静电势梯度,并且表现为非中心对称粒子。通过离轴电子全息术观察到沿纳米棒长轴的静电势梯度为0.11至0.07 V/nm。开尔文探针显微镜、二次电子成像、能量过滤透射电子显微镜和等离子体映射表明,轴向不对称与覆盖AuNRs两端的十六烷基三甲基溴化铵部分数量始终不相等有关。为AuNR表面模拟的静电场图再现了全息图像。偶极状表面势梯度解释了先前源于AuNRs非中心对称性质的非线性光学效应中令人困惑的差异。类似的对称性破缺考量适用于其他纳米级结构,对于这些结构,有机壳层的性质决定对称性可能与标准电子显微镜图像中观察到的无机核的表观对称性不同。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9a67/5817923/9a9b38a7f5ac/1700682-F1.jpg

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