Abstract

This work reports on the effects of layer eccentricity on the resonant properties of active cylindrical core-shell nano-particles excited by a near-by exterior magnetic line source. The core-shell particles consist of a silver core layered with a silica shell. For a fixed over-all radius of the nano-particle equal to 30 nm, we investigate designs with relatively small (radius equal to 6 nm) and large (radius equal to 24 nm) silver cores and we quantify their performance characteristics in terms of the near- and far-field properties. Our results show that the super-resonances, known to exist in the concentric version of these nano-particles, are significantly influenced by introducing eccentricity (through displacements of the silver core relative to the silica shell). In particular, their amplitude responses are found to diminish significantly for silver core displacements ≥ 3 nm for the small core case, and even for displacements ≥ 1 nm for the large core case. The present results are useful from the experimental point of view since slight displacements of the centers of the core and shell parts of the investigated nano-particles are likely to occur in standard fabrication processes.

Highlights

  • Recent years have witnessed a truly increased interest in passive and active nano-particle (NP) systems, and the fascinating plethora of their applications within the emerging areas of nano-photonics including nano-sensors and nano-antennas, lasers and spasers, as well as circuits and artificial material design at optical frequencies [1,2,3,4,5,6,7,8,9]

  • This work reports on the effects of layer eccentricity on the resonant properties of active cylindrical coreshell nano-particles excited by a near-by exterior magnetic line source

  • Our results show that the super-resonances, known to exist in the concentric version of these nano-particles, are significantly influenced by introducing eccentricity

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Summary

Introduction

Recent years have witnessed a truly increased interest in passive and active nano-particle (NP) systems, and the fascinating plethora of their applications within the emerging areas of nano-photonics including nano-sensors and nano-antennas, lasers and spasers, as well as circuits and artificial material design at optical frequencies [1,2,3,4,5,6,7,8,9]. A very successful outcome of this research field was the demonstration that specific electrically small and active coated NPs, based on plasmonic and dielectric materials, may possess highly resonant properties making them useful for many of the above mentioned applications, for the design of efficient nano-sensors, antennas and amplifiers. This is because of the enhanced light-matter interactions in these active NPs which physically are due to the surface plasmon resonances occurring at the interface between the plasmonic and dielectric parts of the NP. Spherical active coated NPs, consisting of a dielectric core impregnated with a canonical, constant frequency gain medium, layered with a plasmonic shell, were

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