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Abstract
Since its invention, optical frequency comb has revolutionized a broad range of subjects from metrology to spectroscopy. The recent development of microresonator-based frequency combs (microcombs) provides a unique pathway to create frequency comb systems on a chip. Indeed, microcomb-based spectroscopy, ranging, optical synthesizer, telecommunications and astronomical calibrations have been reported recently. Critical to many of the integrated comb systems is the broad coverage of comb spectra. Here, microcombs of more than two-octave span (450 nm to 2,008 nm) is demonstrated through χ(2) and χ(3) nonlinearities in a deformed silica microcavity. The deformation lifts the circular symmetry and creates chaotic tunneling channels that enable broadband collection of intracavity emission with a single waveguide. Our demonstration introduces a new degree of freedom, cavity deformation, to the microcomb studies, and our microcomb spectral range is useful for applications in optical clock, astronomical calibration and biological imaging.
Here, the authors demonstrate the use of chaos to obtain 2-octave comb generation. The deformation lifts the circular symmetry and creates chaotic tunneling channels that enable broadband collection of intracavity emission with a single waveguide, introducing a new degree of freedom to microcomb studies.
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1 Peking University, State Key Laboratory for Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319)
2 Peking University, State Key Laboratory for Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319); University of Virginia, Department of Electrical and Computer Engineering, Charlottesville, USA (GRID:grid.27755.32) (ISNI:0000 0000 9136 933X); California Institute of Technology, T. J. Watson Laboratory of Applied Physics, Pasadena, USA (GRID:grid.20861.3d) (ISNI:0000000107068890)
3 California Institute of Technology, T. J. Watson Laboratory of Applied Physics, Pasadena, USA (GRID:grid.20861.3d) (ISNI:0000000107068890)
4 Peking University, State Key Laboratory for Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Beijing, China (GRID:grid.11135.37) (ISNI:0000 0001 2256 9319); Collaborative Innovation Center of Quantum Matter, Beijing, China (GRID:grid.495569.2); Shanxi University, Collaborative Innovation Center of Extreme Optics, Taiyuan, China (GRID:grid.163032.5) (ISNI:0000 0004 1760 2008); Peking University Yangtze Delta Institute of Optoelectronics, Nantong, China (GRID:grid.163032.5)
5 University of Virginia, Department of Electrical and Computer Engineering, Charlottesville, USA (GRID:grid.27755.32) (ISNI:0000 0000 9136 933X); University of Virginia, Department of Physics, Charlottesville, USA (GRID:grid.27755.32) (ISNI:0000 0000 9136 933X)