Sorbonne Universités , UPMC Univ Paris 06, CNRS-UMR7588, Institut des Nano-Sciences de Paris (INSP), 4 Place Jussieu, 75005 Paris, France.
Sorbonne Universités, UPMC Univ Paris 06, UMR 8234 , PHENIX, F-75005 Paris, France.
ACS Nano. 2017 Jul 25;11(7):6728-6738. doi: 10.1021/acsnano.7b01132. Epub 2017 Jun 22.
We show that the use of oriented linear arrays of smectic A defects, the so-called smectic oily streaks, enables the orientation of gold nanorods (GNRs) for a large range of GNR diameters, ranging from 7 to 48 nm, and for various ligands. For the small GNRs it enables oriented end-to-end small chains of GNRs when the density is increased from around 2 GNRs/μm to around 6 GNRs/μm. We have characterized the orientation of single GNRs by spectrophotometry and two-photon luminescence (TPL). A strongly anisotropic absorption of the composites and an on-off switching of GNR luminescence, both controlled by incident light polarization, are observed, revealing an orientation of the GNRs mostly parallel to the oily streaks. A more favorable trapping of GNRs by smectic dislocations with respect to ribbon-like defects is thus demonstrated. The dislocations appear to be localized at a specific localization, namely, the summit of rotating grain boundaries. Combining plasmonic absorption measurements, TPL measurements, and simulation of the plasmonic absorption, we show that the end-to-end GNR chains are both dimers and trimers, all parallel to each other, with a small gap between the coupled GNRs, on the order of 1.5 nm, thus associated with a large red-shift of 110 nm of the longitudinal plasmonic mode. A motion of the GNRs along the dislocations appears as a necessary ingredient for the formation of end-to-end GNR chains, the gap value being driven by the balance between the attracting van der Waals interactions and the steric repulsion between the GNRs and leading to interdigitation of the neighboring ligands. We thus obtain electromagnetic coupling of nanorods controlled by light polarization.
我们表明,使用取向的 A 型向列相缺陷(即向列相油条纹)阵列能够使金纳米棒(GNR)取向,适用于各种配体和直径范围从 7nm 到 48nm 的 GNR。对于小直径的 GNR,当密度从大约 2 根/μm 增加到大约 6 根/μm 时,它可以使 GNR 形成末端相连的小链。我们通过分光光度法和双光子荧光(TPL)对单个 GNR 的取向进行了表征。观察到复合材料具有强烈各向异性的吸收,以及 GNR 发光的开-关切换,这两种现象都由入射光偏振控制,这表明 GNR 主要平行于油条纹取向。因此,向列相位错对 GNR 的捕获比带状缺陷更有利。这些位错似乎被局部化在特定的位置,即旋转晶界的顶点处。结合等离子体吸收测量、TPL 测量和等离子体吸收的模拟,我们表明末端相连的 GNR 链是二聚体和三聚体,它们彼此平行,耦合的 GNR 之间有一个小间隙,约为 1.5nm,因此与纵向等离子体模式的 110nm 红移相关。GNR 沿着位错的运动似乎是形成末端相连的 GNR 链的必要条件,间隙值由范德华吸引力和 GNR 之间的空间排斥之间的平衡驱动,导致相邻配体的交错。因此,我们获得了由光偏振控制的纳米棒的电磁耦合。