Abstract

We describe wavelength tuning in a one dimensional (1D) silicon nitride nano-grating guided mode resonance (GMR) structure under conical mounting configuration of the device. When the GMR structure is rotated about the axis perpendicular to the surface of the device (azimuthal rotation) for light incident at oblique angles, the conditions for resonance are different than for conventional GMR structures under classical mounting. These resonance conditions enable tuning of the GMR peak position over a wide range of wavelengths. We experimental demonstrate tuning over a range of 375 nm between 500 nm˜875 nm. We present a theoretical model to explain the resonance conditions observed in our experiments and predict the peak positions with show excellent agreement with experiments. Our method for tuning wavelengths is simpler and more efficient than conventional procedures that employ variations in the design parameters of structures or conical mounting of two-dimensional (2D) GMR structures and enables a single 1D GMR device to function as a high efficiency wavelength filter over a wide range of wavelengths. We expect tunable filters based on this technique to be applicable in a wide range of fields including astronomy and biomedical imaging.

Highlights

  • Wide wavelength range tunable onedimensional silicon nitride nano-grating guided mode resonance filter based on azimuthal rotation

  • Wide wavelength range tunable one-dimensional silicon nitride nano-grating guided mode resonance filter based on azimuthal rotation

  • Only special cases of conical mounting have been reported in literature where, for example, the plane of incidence is rotated by 90o from the grating vector, known as full conical mounting.[16,17,18,19]

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Summary

Introduction

Wide wavelength range tunable onedimensional silicon nitride nano-grating guided mode resonance filter based on azimuthal rotation. We take this approach further and show that wavelength tuning in a 1D GMR structure can be achieved by azimuthally rotating it about the surface normal.

Results
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