• Photonics Research
  • Vol. 8, Issue 12, 1904 (2020)
Neetesh Singh1、2、*, Hamidu M. Mbonde3, Henry C. Frankis3, Erich Ippen2, Jonathan D. B. Bradley3、4, and Franz X. Kärtner1
Author Affiliations
  • 1Centre for Free Electron Laser Science (CFEL)-DESY and University of Hamburg, 22607 Hamburg, Germany
  • 2Research Laboratory of Electronics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
  • 3Department of Engineering Physics, McMaster University, Hamilton, Ontario L8S 4L7, Canada
  • 4e-mail: jbradley@mcmaster.ca
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    DOI: 10.1364/PRJ.400057 Cite this Article Set citation alerts
    Neetesh Singh, Hamidu M. Mbonde, Henry C. Frankis, Erich Ippen, Jonathan D. B. Bradley, Franz X. Kärtner. Nonlinear silicon photonics on CMOS-compatible tellurium oxide[J]. Photonics Research, 2020, 8(12): 1904 Copy Citation Text show less
    (a) Schematic of the waveguide fabrication steps with different layers. (b) Schematic of the waveguide cross section. (c) SEM image of the waveguide.
    Fig. 1. (a) Schematic of the waveguide fabrication steps with different layers. (b) Schematic of the waveguide cross section. (c) SEM image of the waveguide.
    (a) Calculated dispersion and effective index of the waveguide for the fundamental TE mode. (b) and (c) The mode profile at 1550 nm of the waveguide with and without tellurium oxide, respectively.
    Fig. 2. (a) Calculated dispersion and effective index of the waveguide for the fundamental TE mode. (b) and (c) The mode profile at 1550 nm of the waveguide with and without tellurium oxide, respectively.
    Experimental supercontinuum and third-harmonic generation spectra with an image of the third-harmonic generation along the length of the waveguide (inset). The vertical axis is on-chip power, and the dashed curve is the simulated spectrum shifted down for clarity.
    Fig. 3. Experimental supercontinuum and third-harmonic generation spectra with an image of the third-harmonic generation along the length of the waveguide (inset). The vertical axis is on-chip power, and the dashed curve is the simulated spectrum shifted down for clarity.
    (a) and (b) The supercontinuum and third-harmonic generation spectra at different pump powers. (c) Optical images, taken with a CMOS camera, of third-harmonic generation at different pump wavelengths with signal color of green (pump at 1600 nm), cyan (pump at 1550 nm), and blue (pump at 1460 nm). The input is at the left side of the images. The third-harmonic signal had larger scattering for the 1550 nm pump (inset), as the pump power was higher than for the others.
    Fig. 4. (a) and (b) The supercontinuum and third-harmonic generation spectra at different pump powers. (c) Optical images, taken with a CMOS camera, of third-harmonic generation at different pump wavelengths with signal color of green (pump at 1600 nm), cyan (pump at 1550 nm), and blue (pump at 1460 nm). The input is at the left side of the images. The third-harmonic signal had larger scattering for the 1550 nm pump (inset), as the pump power was higher than for the others.
    (a) Calculated anomalous dispersion of the waveguide and the mode profile for the fundamental TE mode (inset). Energy confined in silicon nitride is ∼30%. (b) Calculated supercontinuum generation along with the spectrogram (inset) for a 1 cm long waveguide at 1 kW of pump power at 1550 nm.
    Fig. 5. (a) Calculated anomalous dispersion of the waveguide and the mode profile for the fundamental TE mode (inset). Energy confined in silicon nitride is 30%. (b) Calculated supercontinuum generation along with the spectrogram (inset) for a 1 cm long waveguide at 1 kW of pump power at 1550 nm.
    Neetesh Singh, Hamidu M. Mbonde, Henry C. Frankis, Erich Ippen, Jonathan D. B. Bradley, Franz X. Kärtner. Nonlinear silicon photonics on CMOS-compatible tellurium oxide[J]. Photonics Research, 2020, 8(12): 1904
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