Abstract

In this report, we propose and demonstrate an air-mode photonic crystal ring resonator (PhCRR) on silicon-on-insulator platform. Air mode is utilized to confine the optical field into photonic crystal (PhC) air holes, which is confirmed by the three-dimensional finite-difference time-domain simulation. PhCRR structure is employed to enhance the light-matter interaction through combining the whispering-gallery mode resonance of ring resonator with the slow-light effect in PhC waveguide. In the simulated and measured transmission spectra of air-mode PhCRR, nonuniform free spectral ranges are observed near the Brillouin zone edge of PhC, indicating the presence of the slow-light effect. A maximum group index of 27.3 and a highest quality factor of 14600 are experimentally obtained near the band edge. Benefiting from the strong optical confinement in the PhC holes and enhanced light-matter interaction in the resonator, the demonstrated air-mode PhCRR is expected to have potential applications in refractive index sensing, on-chip light emitting and nonlinear optics by integration with functional materials.

Highlights

  • In this report, we propose and demonstrate an air-mode photonic crystal ring resonator (PhCRR) on silicon-on-insulator platform

  • Air mode is utilized to confine the optical field into photonic crystal (PhC) air holes, which is confirmed by the three-dimensional finite-difference time-domain simulation

  • Distinct from the dielectric-mode PhCRR, optical field is strongly squeezed into the PhC holes and overlaps sufficiently with the analyte in the air-mode PhCRR, which further improves the sensitivity of PhCRR structure

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Summary

Results and Discussion

When approaching the Brillouin zone edge, the decrease in FSRs from 3.31 to 0.95 nm indicates the large group index dispersion and strong slow-light effect. From the above measured and simulated transmission spectra of the air-mode PhCRR in Fig. 2(b) and 3(a), the group index can be calculated by taking ng ≈ λ 2/(FSR·L), where ng is the group index, λ is the central wavelength between two adjacent resonances, and L is the round-trip path-length of the ring. We have proposed and demonstrated an air-mode PhCRR on silicon-on-insulator In such type of PhCRR, optical field can be strongly confined in PhC air holes, proven by the 3D FDTD simulated band-edge resonant mode profiles. As wavelength approaches the Brillouin zone edge, the transmission spectrum of the PhCRR exhibits a decreasing FSR, indicating the presence of the slow-light effect. The combination of the strong optical confinement in air holes, the slow-light effect and the WGM resonance would greatly enhance the light-matter interaction in air holes, which makes the air-mode PhCRR potential for applications in RI sensing, on-chip light emitting and nonlinear optics

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