Insight on the Coupling of Plasmonic Nanoparticles from Near-Field Spectra Determined via Discrete Dipole Approximations

通过离散偶极子近似法测定近场光谱,深入了解等离子体纳米粒子的耦合特性

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Abstract

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 (Q (NF)) around spherical gold nanoparticles (Au NPs) using Discrete Dipole Approximation (DDA). The reliability of the method was tested by comparing Q (NF) 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 Q (NF) enhancement, due to coupling in longitudinal mode, is much greater than the enhancement in Q (ext). There is a linear correlation between the Q (NF) and Q (ext) peak positions, with the Q (NF) peak redshifted from the Q (ext) peak by an average of approximately 12 nm. In the case of the multimers, Q (NF) 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 Q (NF) spectra. For the transverse mode, we differentiate two different scenario, transverse-Y where both electric field (E) and light propagation vector (k) are perpendicular the chain axis, and transverse-X where k is parallel to the chain axis. In transverse-Y mode, coupling leads to reduced Q (NF) spectra and the center sphere has the lowest Q (NF) intensity. In transverse-X mode, there is retardation effect from the front sphere to the back sphere. The Q (NF) from the front sphere is stronger than from the back sphere. In addition, due to the phase lag in k-direction, the Q (NF) 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.

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