2016
DOI: 10.1038/nphoton.2016.163
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Integrated finely tunable microring laser on silicon

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Cited by 121 publications
(65 citation statements)
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“…4(c) presents the zoomed-in emission spectra as the substrate temperature was ramped up with the pump power doubling the lasing thresholds, offset vertically for clarity. The intensity ratio of TE 1,6 to TE 1,7 becomes larger at a higher temperature (P pump ¼ 2 Â P th ), because of the temperature redshift in the material gain. A high characteristic temperature, T 0 % 123 K in the range of 20-60 C was extracted for the TE 1,6 mode in Fig.…”
Section: -3mentioning
confidence: 99%
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“…4(c) presents the zoomed-in emission spectra as the substrate temperature was ramped up with the pump power doubling the lasing thresholds, offset vertically for clarity. The intensity ratio of TE 1,6 to TE 1,7 becomes larger at a higher temperature (P pump ¼ 2 Â P th ), because of the temperature redshift in the material gain. A high characteristic temperature, T 0 % 123 K in the range of 20-60 C was extracted for the TE 1,6 mode in Fig.…”
Section: -3mentioning
confidence: 99%
“…Although group-IV-based optical building blocks including silicon modulators, 2 microring resonators, 3 waveguides, 4 and germanium photodetectors 5 have demonstrated their techno-economic viability, an efficient Si-based laser source remains the most challenging component due to the indirect bandgap of Si. 6 Integrating high performance III-V lasers with Si has been considered a promising path to resolve this challenge. Wafer or die bonding has been shown as a successful approach, demonstrating impressive device performances, [7][8][9] and has gradually been adopted by industry.…”
mentioning
confidence: 99%
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“…To date, wafer bonding has achieved a dominance in Si photonic integration area [3], [22], [23], as it allows for the combination of light emitting capability of III-V materials with light routing of Si waveguide. Notably, smaller cavity length lasers have successfully been realized by using integrated mirrors, such as distributed Bragg reflectors [24], [25], reflective multimode interferometers [26] or ring structure, which allows for the formation of large number of channels, while, with reduced crosstalk between adjacent channels as well as laser cavity without the requirement for polishing facets [23]. In addition to wafer bonding, monolithic growth method is another rapid-growing research area due to its cost-effective and massive scalable integration merits.…”
Section: Introductionmentioning
confidence: 99%