CMOS-compatible multiple-wavelength oscillator for on-chip optical interconnects
By J. Levy, A. Gondarenko, M. Foster, A. Turner-Foster, Alexander Gaeta, Michal Lipson. 2010
1,011 citations recorded by the source corpus.
Subfields: Atomic and Molecular Physics, and Optics, Electrical and Electronic Engineering
View Paper: https://www.semanticscholar.org/paper/6b6f57dcdf85ad1e61d50382177a7b77477f5e5e
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In Atomic and Molecular Physics, and Optics
- Roberto Morandotti
- David J. Moss
- Xingyuan Xu
- Arnan Mitchell
- Jiayang Wu
- Mengxi Tan
- Brent E. Little
- Sai T. Chu
In Electrical and Electronic Engineering
- Roberto Morandotti
- David J. Moss
- Xingyuan Xu
- Arnan Mitchell
- Jiayang Wu
- Mengxi Tan
- Brent E. Little
- Sai T. Chu
Citations in the corpus
- Orthogonally Polarized RF Optical Single Sideband Generation and Dual-Channel Equalization Based on an Integrated Microring Resonator (2018, background): “More generally, MRRs with FSRs of 200 GHz and larger [47] can be realized, enabling even higher RF operation frequencies.”
- Photonic RF and microwave filters based on 49 GHz and 200 GHz Kerr microcombs (2020, methodology): “In 2008 new CMOS compatible platforms for nonlinear optics, including silicon nitride [35, 36] and Hydex [37-47] were introduced with negligible nonlinear absorption in the telecom band, a moderate nonlinear parameter and extremely high nonlinear figure of merit, which are ideal for micro-comb gener”
- Mode-locked dark pulse Kerr combs in normal-dispersion microresonators (2014, methodology): “The phase of each comb line was then compensated to form a transform-limited pulse train (see Methods) [11].”
- Micro-combs: A novel generation of optical sources (2017, methodology): “[11] employed a silicon nitride (Si3N4) two-portmicro-ring resonator geometry (i.”
- Spectral line-by-line pulse shaping of an on-chip microresonator frequency comb (2011, background): “Previous research [14] indicates that engineering o f the waveguide design for optimized dispersion, which has not yet been performed in our devices, is critical to achieving the widest comb bandwidth.”
- On-Chip Optical Squeezing (2013, methodology): “In order to obtain FWM gain and optical parametric oscillation, the dispersion is engineered to be anomalous at the pump wavelength to compensate for the Kerr nonlinear phase shift due to the pump [26,30].”
- Breaking the Loss Limitation of On-chip High-confinement Resonators (2016, background): “Low propagation loss silicon nitride (Si3N4) ring resonators are critical for a variety of photonic applications such as efficient and compact on-chip optical routing [1,2], low threshold frequency combs [3-5], optical clocks [6] and high precision sensing [7-11].”