Peceros Katia E, Xu Xiaoda, Bulcock Shaun R, Cortie Michael B
Institute for Nanoscale Technology, University of Technology, Sydney, P.O. Box 123, Broadway, NSW 2007, Australia.
J Phys Chem B. 2005 Nov 24;109(46):21516-20. doi: 10.1021/jp0523470.
Red-shifting of the optical absorption spectra of aggregates of gold nanoparticles by dipole-dipole interactions is of considerable interest, both for theoretical reasons and because the phenomenon can be potentially exploited in various applications. A convenient and practical way to control the effect is to assemble the aggregated ensemble of n gold nanoparticles on the outer surface of larger dielectric spheres. Here, we show by experiment and calculation how the spectra of these structures can be systematically morphed from that of isolated gold particles, through the regime of broad absorption dominated by particle-particle interactions, and finally to the limiting case of a continuous nanoshell. The experimental data were produced using the process of deposition-precipitation, which provides a facile method to decorate polystyrene microspheres with gold nanoparticles. There is no need for prior functionalization of the microsphere surface in our method of deposition-precipitation. Calculations were carried out using a code based on the discrete dipole approximation (DDA). The spectra were dominated by three effects. These were a peak absorption at about 540 nm produced by the conventional plasmon resonance of spherical gold nanoparticles, a broad absorption in the range 600-900 nm caused by diverse dipole-dipole interactions between particles, which strengthened as the number of attached gold particles increased and finally, when n was large, an absorption peak due to the onset of nanoshell-like resonances. The experimental spectra could be successfully fitted by spectra calculated using combinations of these effects.
由于理论原因以及该现象在各种应用中具有潜在的可利用价值,金纳米颗粒聚集体的光吸收光谱红移备受关注。一种方便实用的控制该效应的方法是将 n 个金纳米颗粒的聚集整体组装在较大介电球体的外表面。在此,我们通过实验和计算展示了这些结构的光谱如何从孤立金颗粒的光谱开始,经过由颗粒间相互作用主导的宽吸收区域,最终演变为连续纳米壳的极限情况。实验数据是通过沉积沉淀过程产生的,该过程提供了一种用金纳米颗粒修饰聚苯乙烯微球的简便方法。在我们的沉积沉淀方法中,无需对微球表面进行预先功能化处理。计算是使用基于离散偶极近似(DDA)的代码进行的。光谱由三种效应主导。这些效应分别是:球形金纳米颗粒的传统等离子体共振在约 540 nm 处产生的峰值吸收;颗粒间各种偶极 - 偶极相互作用在 600 - 900 nm 范围内引起的宽吸收,随着附着金颗粒数量的增加而增强;最后,当 n 较大时,由于类似纳米壳共振的出现而产生的吸收峰。实验光谱可以通过使用这些效应组合计算得到的光谱成功拟合。