Abstract

Controlling the group velocity dispersion of silicon nanophotonic waveguides has been recognized as a key ingredient to enhance the development of various on-chip optical applications. However, the strong wavelength dependence of the dispersion in waveguides implemented on the high index contrast silicon-on-insulator (SOI) platform substantially hinders their wideband operation, which in turn, limits their deployment. In this work, we exploit the potential of non-resonant sub-wavelength grating (SWG) nanostructures to perform a flexible and wideband control of dispersion in SOI waveguides. In particular, we demonstrated that the overall dispersion of the SWG-engineered metamaterial waveguides can be tailored across the transparency window of the SOI platform, keeping easy-to-handle single-etch step manufacturing. The SWG silicon waveguides overcladded by silicon nitride exhibit significant reduction of wavelength dependence of dispersion, yet providing intriguing and customizable synthesis of various attractive dispersion profiles. These include large normal up to low anomalous operation regimes, both of which could make a great promise for plethora of emerging applications in silicon photonics.

Highlights

  • The silicon-on-insulator (SOI) has been established as a promising waveguide technology to realize key integrated nanophotonic components in various on-chip optical applications

  • Controlling the group velocity dispersion of silicon nanophotonic waveguides has been recognized as a key ingredient to enhance the development of various on-chip optical applications

  • We exploit the potential of non-resonant sub-wavelength grating (SWG) nanostructures to perform a flexible and wideband control of dispersion in SOI waveguides

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Summary

Introduction

The silicon-on-insulator (SOI) has been established as a promising waveguide technology to realize key integrated nanophotonic components in various on-chip optical applications. In a particular case of the dominant SOI platform, the dispersion can be readily controlled by adjusting cross-sectional dimensions of the waveguide [10,11,12,13], because of the high modal confinement offered by the high index contrast system. Apart from this straightforward approach, several different techniques have been explored, both theoretically and experimentally [14,15,16,17,18,19,20], allowing for variable dispersion engineering. This primarily includes the slot-assisted waveguide structure with horizontal and vertical geometries [14,15,16], conformal dielectric overlayers [17], multilayer guiding structures [18], double- and multi-cladded waveguides [19], or photonic crystal waveguides [20]

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