2017
DOI: 10.1063/1.4981392
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Micro-ring resonator quality factor enhancement via an integrated Fabry-Perot cavity

Abstract: We propose and experimentally demonstrate the enhancement in the filtering quality (Q) factor of an integrated micro-ring resonator (MRR) by embedding it in an integrated Fabry-Perot (FP) cavity formed by cascaded Sagnac loop reflectors. By utilizing coherent interference within the FP cavity to reshape the transmission spectrum of the MRR, both the Q factor and the extinction ratio (ER) can be significantly improved. The device is theoretically analyzed and practically fabricated on a silicon-on-insulator waf… Show more

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Cited by 132 publications
(99 citation statements)
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“…2(b). The device architecture used a vertical coupling scheme where the gap (approximately 200nm) could be controlled via film growth -a more accurate approach than lithographic techniques [40]. Other advantages of our platform for nonlinear optics include ultra-low linear loss (~0.06 dB•cm −1 ), a sufficient nonlinearity parameter (~233 W −1 •km −1 ), and most important, negligible nonlinear loss (up to ~25 GW•cm −2 [34][35]).…”
Section: Rf True Time Delays Based On Integrated Optical Frequency Combsmentioning
confidence: 99%
“…2(b). The device architecture used a vertical coupling scheme where the gap (approximately 200nm) could be controlled via film growth -a more accurate approach than lithographic techniques [40]. Other advantages of our platform for nonlinear optics include ultra-low linear loss (~0.06 dB•cm −1 ), a sufficient nonlinearity parameter (~233 W −1 •km −1 ), and most important, negligible nonlinear loss (up to ~25 GW•cm −2 [34][35]).…”
Section: Rf True Time Delays Based On Integrated Optical Frequency Combsmentioning
confidence: 99%
“…The sharpening of the filter shape can be attributed to coherent interference within the coupled resonant cavities, which could be useful for implementation of high-Q filters. 7,32 Figure 3 shows the calculated power transmission spectra of asymmetric CSLR resonators (N = 3) when L 1 L 2 . For comparison, we use the same field transmission coefficients [t 1 , t 2 , t 3 ] = [0.87, 0.77, 0.87] in the calculation.…”
Section: Device Configuration and Operation Principlementioning
confidence: 99%
“…., FPC N 1 ), similar to Bragg gratings. 30,31 To study the CSLR resonator based on the scattering matrix method, 32,33 we define the waveguide and coupler parameters of the CSLR resonator in Table I, and so the field transmission …”
Section: Introductionmentioning
confidence: 99%
“…Our device architecture uses a vertical coupling scheme where the gap can be controlled via film growth-a more accurate approach than lithographic techniques. 38,39 The gap between the bus waveguide and the MRR is approximately 200 nm. The compact integrated MRR has a radius of ∼135 µm with a relatively large free spectral range (FSR) of ∼1.6 nm, i.e., ∼200 GHz.…”
Section: Resultsmentioning
confidence: 99%