Abstract

Porous gold nanoparticles (PGNs) are very popular due to their high surface/volume ratio, moreover they have stronger plasmonic properties than their solid counterparts. These properties make the porous gold nanoparticles very useful for lots of applications, for instance chemical sensors, cancer therapy applications. For applications, however, it is indispensable that the resonance frequency (RF) of a plasmonic structure to be tuneable. In this work we show that the RF can be set in a wide range as desired by coating the PGNs by mixed oxide layers. By changing the composition of the coating layer, that is the mixture ratio, the RF can be shifted practically continuously in a wide range determined by the refractive index of the used oxides. As a demonstration, PGNs were coated with mixed alumina-titania oxide layers (5–7 nm) using plasma-enhanced atomic layer deposition method. The oxide layer, beside as a tuning tool, also stabilises the structure of the PGNs when are exposed to elevated temperature. This is shown by the influence of the temperature (from 350, ^{circ }hbox {C} up to 900, ^{circ }hbox {C}) on the morphology, and as a consequence the optical extinction spectra, of the oxide coated PGNs.

Highlights

  • Surface Plasmon (SP)[1] resonance is a collective oscillation of conduction electrons excited by the electromagnetic field of light

  • We showed that the resonance energy of the Porous gold nanoparticles (PGNs) can be continuously tuned in a simple, reproducible and cheap way by coating the PGNs with mixed metal-oxide layers

  • Very importantly this tuning can be realised without changing the base morphology of the PGNs, such as the size, the interparticle distance, pore or ligament size of the nanoparticles, which are much more difficult to plan and reproduce[19]

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Summary

Introduction

Surface Plasmon (SP)[1] resonance is a collective oscillation of conduction electrons excited by the electromagnetic field of light. In the case of metallic nanoparticles (NPs), the electron oscillations induced electric field around the NP opens the possibility to manipulate visible and near infrared light on the nanoscale[1, 2]. The resonance energy of these excitations are extremely sensitive to the composition, size, shape and the dielectric function of the surrounding medium of the NPs[7,8,9,10,11,12,13,14,15,16] Modifying these parameters one may tune the optical properties of the NPs[17]

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