Influence of surfactant, particle size and dispersion medium on surface plasmon resonance of silver nanoparticles

TL;DR

This study investigates how particle size, surfactants, and solvents influence the surface plasmon resonance of silver nanoparticles, revealing multiple peaks and solvent effects relevant for applications in sensing and photocatalysis.

Contribution

It provides new insights into the effects of particle size, surfactants, and dispersion medium on SPR features, including the first observation of multiple charge-transfer related peaks.

Findings

SPR peak shifts with particle size and solvent polarity

Multiple charge-transfer related peaks observed in polar and non-polar solvents

Drude model applicability limited to non-polar solvents

Abstract

Clear influence of particle size, surfactants and dispersion medium on surface plasmon resonance (SPR) features of Ag nanoparticles (NPs), synthesized in thermal decomposition method, in the broad range of ultraviolet (UV) radiation, critical for many potential applications such as a photocatalyst, UV-sensor and detector, has been demonstrated here. It involves adsorbate coverage, interparticle distance or agglomeration, surface charge density and solvent refractive index ({\mu}). NP agglomeration and surface charge density in solvents of varying {\mu} have been studied systematically through zeta-potential ({\zeta}) and hydrodynamic diameter (HD) using dynamic light scattering (DLS). The main SPR feature found at 316 nm in 31.5 nm NPs shifts to 320 nm in 15.1 nm NPs. The peak at 320 nm in air shifts to 259, 261 and 277 nm in polar solvent methanol, deionized water and ethanol, respectively and to 255, 275 and 282 nm in non-polar solvent n-hexane, benzene and toluene, respectively. In general, the decrease in particle size and increase in {\mu} of solvents show red-shift. Curiously, a number of peaks up to seven in these solvents that are attributed to charge-transfer mechanism and change in inter-particle interaction of the NPs turning from a single peak of SPR in air has been observed for the first time. A model for re-adjustment of Fermi level (E_F) of Ag NP and the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) to explain them has also been used. Moreover, the Drude model for shift in the position of SPR in these NPs is only applicable in non-polar solvents, not in polar solvents. Such novel features will be potential candidates for various applications.