Abstract

High-brightness light sources with nanoscale volume are required in nonlinear physics studies or various nanoscale engineering areas. Although several plasmonic devices, such as plasmonic nanofocusing, have been proposed for light concentration, the efficient enhancement of the nanofocusing device to get a bright light source is still limited owing to the inevitable Ohmic loss resulting from high field confinement on metallic surface. We propose the concept of dielectric nanofocusing by reversing the concept of conventional plasmonic nanofocusing and using a three-dimensional bowtie nanoaperture (3D BNA). The optical simulations demonstrate that the 3D BNA can achieve an intensity enhancement factor of 9.01 × 104. We calculate the dispersion relation for a tapered silver–SiNx–air waveguide to prove the possibility of focusing even for a high tapered angle. The theoretically calculated modal length can explain the origin of the high intensity enhancement by proving an energy flow from the dielectric layer to the air regime in dielectric nanofocusing. The performed optical and thermal simulations demonstrate that the 3D BNA can achieve a peak intensity of 6.21 PW/cm2 by avoiding the energy confinement around the metal. Our approach provides a new method for obtaining a high brightness light source.

Highlights

  • A high-brightness light source is required in technologies based on nonlinear physics, such as nonlinear scattering[1] and high-harmonic generation (HHG)[2]

  • The tapered structure of the 3D bowtie nano-aperture (BNA) can act as a concentrator without experiencing reflection or scattering if the variations in the effective index of the tapered MIAIM waveguide, defined as neff = (β/k0), are sufficiently small to be within the distance of one wavelength, similar to the anti-reflection structure based on gradient refractive index optics[16]

  • We have proposed a concept of dielectric nanofocusing by employing a tapered MIAIM structure

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Summary

Introduction

A high-brightness light source is required in technologies based on nonlinear physics, such as nonlinear scattering[1] and high-harmonic generation (HHG)[2]. As the optical energy inside the dielectric layer is transferred to the air channel at the tip of the aperture in a tapered MIAIM structure, dielectric nanofocusing leads to a high intensity enhancement as well as suppression of the intensity at the metallic surface, inducing a small Ohmic loss or heating effect.

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