Barr James W, Gomrok Saghar, Chaffin Elise, Huang Xiaohua, Wang Yongmei
Department of Chemistry, The University of Memphis, Memphis, Tennessee 38152, USA.
Freed-Hardeman University, Henderson, Tennessee 38340, USA.
J Phys Chem C Nanomater Interfaces. 2021 Mar 11;125(9):5260-5268. doi: 10.1021/acs.jpcc.1c01071. Epub 2021 Mar 2.
Coupling between plasmonic nanoparticles (NPs) in nanoparticle assemblies has been investigated extensively via far-field properties, such as absorption and scattering, but very rarely via near-field properties, and a quantitative investigation of near-field properties should provide great insight into the nature of the coupling. We report a numerical procedure to obtain reliable near-field spectra ( ) around spherical gold nanoparticles (Au NPs) using Discrete Dipole Approximation (DDA). The reliability of the method was tested by comparing from DDA calculations with exact results from the Mie theory. We then applied the method to examine Au NPs assembled in dimer, trimer, and up to pentamer in a linear arrangement. For the well-studied dimer system, we show that the enhancement, due to coupling in longitudinal mode, is much greater than the enhancement in . There is a linear correlation between the and peak positions, with the peak redshifted from the peak by an average of approximately 12 nm. In the case of the multimers, spectra from individual spheres were not always identical and become dependent on the sphere location. In the longitudinal model, the center sphere has the strongest spectra. For the transverse mode, we differentiate two different scenario, transverse-Y where both electric field () and light propagation vector () are perpendicular the chain axis, and transverse-X where is parallel to the chain axis. In transverse-Y mode, coupling leads to reduced spectra and the center sphere has the lowest intensity. In transverse-X mode, there is retardation effect from the front sphere to the back sphere. The from the front sphere is stronger than from the back sphere. In addition, due to the phase lag in -direction, the in transverse-X can differ quite significantly from transverse-Y for large particles. All these results could be understood when one considers how electric field from induced dipoles on neighboring NPs add on or subtract from the incident E-field. These results provide new insight into the coupling properties of Au NPs.
纳米颗粒组装体中,等离子体纳米颗粒(NPs)之间的耦合已通过远场特性(如吸收和散射)得到了广泛研究,但很少通过近场特性进行研究,而对近场特性的定量研究应能深入了解耦合的本质。我们报告了一种数值方法,使用离散偶极近似(DDA)来获得球形金纳米颗粒(Au NPs)周围可靠的近场光谱( )。通过将DDA计算得到的 与米氏理论的精确结果进行比较,测试了该方法的可靠性。然后,我们应用该方法研究了线性排列的二聚体、三聚体以及直至五聚体中的Au NPs。对于研究充分的二聚体系统,我们表明,由于纵向模式下的耦合, 的增强远大于 中的增强。 和 峰值位置之间存在线性相关性, 峰值相对于 峰值平均红移约12 nm。在多聚体的情况下,各个球体的 光谱并不总是相同的,并且变得依赖于球体位置。在纵向模式下,中心球体具有最强的 光谱。对于横向模式,我们区分了两种不同的情况,横向-Y,其中电场( )和光传播矢量( )都垂直于链轴,以及横向-X,其中 平行于链轴。在横向-Y模式下,耦合导致 光谱降低,并且中心球体具有最低的 强度。在横向-X模式下,从前球体到后球体存在延迟效应。前球体的 比后球体的更强。此外,由于 -方向上的相位滞后,对于大颗粒,横向-X中的 可能与横向-Y有很大差异。当考虑相邻NPs上感应偶极的电场如何与入射电场相加或相减时,所有这些结果都可以得到理解。这些结果为Au NPs的耦合特性提供了新的见解。