2018
DOI: 10.1063/1.5025833
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Advanced photonic filters based on cascaded Sagnac loop reflector resonators in silicon-on-insulator nanowires

Abstract: We demonstrate advanced integrated photonic filters in silicon-on-insulator (SOI) nanowires implemented by cascaded Sagnac loop reflector (CSLR) resonators. We investigate mode splitting in these standing-wave (SW) resonators and demonstrate its use for engineering the spectral profile of on-chip photonic filters. By changing the reflectivity of the Sagnac loop reflectors (SLRs) and the phase shifts along the connecting waveguides, we tailor mode splitting in the CSLR resonators to achieve a wide range of filt… Show more

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Cited by 114 publications
(118 citation statements)
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“…As the input CW power was increased, the MRRs with both uniformly coated and patterned GO films exhibited a clear decrease in ER and Q, whereas the uncoated MRR did not. The propagation loss of the GO hybrid waveguides was obtained by using the scattering matrix method [ 52,53 ] to fit the ERs and Qs in Figure 3a–d, and is shown for 1−5 layers and 10−50 layers in Figure 3e,f, respectively. Note that the propagation loss obtained from the GO‐coated MRRs is different from that obtained from the GO‐coated waveguides [ 29,43 ] when considering the power‐dependent loss changes of the GO films, since the light intensity in the MRRs is significantly higher due to resonant enhancements.…”
Section: Device Fabrication and Characterizationmentioning
confidence: 99%
“…As the input CW power was increased, the MRRs with both uniformly coated and patterned GO films exhibited a clear decrease in ER and Q, whereas the uncoated MRR did not. The propagation loss of the GO hybrid waveguides was obtained by using the scattering matrix method [ 52,53 ] to fit the ERs and Qs in Figure 3a–d, and is shown for 1−5 layers and 10−50 layers in Figure 3e,f, respectively. Note that the propagation loss obtained from the GO‐coated MRRs is different from that obtained from the GO‐coated waveguides [ 29,43 ] when considering the power‐dependent loss changes of the GO films, since the light intensity in the MRRs is significantly higher due to resonant enhancements.…”
Section: Device Fabrication and Characterizationmentioning
confidence: 99%
“…As the input CW power was increased, the MRRs with both uniformly coated and patterned GO films exhibited a clear decrease in ER and Q, whereas the uncoated MRR did not. The propagation loss of the GO hybrid waveguides was obtained by using the scattering matrix method [52,53] Note that the propagation loss obtained from the GO-coated MRRs is different from that obtained from the GO-coated waveguides [29,43] when considering the power-dependent loss changes of the GO films, since the light intensity in the MRRs is significantly higher due to resonant enhancements. The low-power (W/O in Figures 3(e)) propagation loss of the uncoated waveguide and the waveguide with a monolayer of GO was ~0.26 dB/cm and ~1.27 dB/cm, respectively, corresponding to an excess propagation loss of ~1 dB/cm induced by the GO film.…”
Section: Device Fabrication and Characterizationmentioning
confidence: 99%
“…The measured TE and TM polarized transmission spectra of the uniformly GO-coated MRR are shown in Figures 4(a-i) and (a-ii), respectively, while the transmission spectra of the patterned MRR are shown in Figures 4(b-i) and (b-ii), all measured with the same doped silica MRR at a CW power of ~0 dBm. The resulting Q factors [31][32][33] and extinction ratios [34,35] are shown in Figure 5(a). The uncoated MRR had high extinction ratios (> 15 dB) and relatively high Q factors (180,000) (although significantly less than for buried waveguides) for both polarizations.…”
Section: Go-coated Polarization-selective Mrrsmentioning
confidence: 99%