• Photonics Research
  • Vol. 6, Issue 9, 925 (2018)
Ting-Hui Xiao1、†, Ziqiang Zhao2、†, Wen Zhou3、†, Mitsuru Takenaka2, Hon Ki Tsang3, Zhenzhou Cheng1、*, and Keisuke Goda1、4、5
Author Affiliations
  • 1Department of Chemistry, The University of Tokyo, Tokyo 113-0033, Japan
  • 2Department of Electrical Engineering and Information Systems, The University of Tokyo, Tokyo 113-0033, Japan
  • 3Department of Electronic Engineering, The Chinese University of Hong Kong, Shatin, Hong Kong SAR, China
  • 4Department of Electrical Engineering, University of California, Los Angeles, California 90095, USA
  • 5e-mail: goda@chem.s.u-tokyo.ac.jp
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    DOI: 10.1364/PRJ.6.000925 Cite this Article Set citation alerts
    Ting-Hui Xiao, Ziqiang Zhao, Wen Zhou, Mitsuru Takenaka, Hon Ki Tsang, Zhenzhou Cheng, Keisuke Goda. High-Q germanium optical nanocavity[J]. Photonics Research, 2018, 6(9): 925 Copy Citation Text show less
    Schematic of the monolithically integrated on-chip MIR germanium device that contains a high-Q nanocavity, two suspended-membrane waveguides, and two focusing subwavelength grating couplers. The inset to the bottom left shows the design of the high-Q nanocavity. The inset to the bottom right shows a cross-sectional view of a suspended-membrane waveguide.
    Fig. 1. Schematic of the monolithically integrated on-chip MIR germanium device that contains a high-Q nanocavity, two suspended-membrane waveguides, and two focusing subwavelength grating couplers. The inset to the bottom left shows the design of the high-Q nanocavity. The inset to the bottom right shows a cross-sectional view of a suspended-membrane waveguide.
    SEM images of the MIR germanium device, including the high-Q nanocavity. (a) Top view of the device. Scale bar: 10 μm. (b) Top view of the high-Q nanocavity. Scale bar: 500 nm.
    Fig. 2. SEM images of the MIR germanium device, including the high-Q nanocavity. (a) Top view of the device. Scale bar: 10 μm. (b) Top view of the high-Q nanocavity. Scale bar: 500 nm.
    Experimental characterization of the MIR germanium device, including the high-Q nanocavity. (a) Measured transmission spectrum of the device (blue) and measured coupling efficiency of the focusing subwavelength grating couplers (red). (b) Lorentzian fitting of the measured nanocavity resonant mode. The inset shows the electric field magnitude distribution of the resonant mode.
    Fig. 3. Experimental characterization of the MIR germanium device, including the high-Q nanocavity. (a) Measured transmission spectrum of the device (blue) and measured coupling efficiency of the focusing subwavelength grating couplers (red). (b) Lorentzian fitting of the measured nanocavity resonant mode. The inset shows the electric field magnitude distribution of the resonant mode.
    GeometryWavelengthQ FactorCavity TypeReference
    Photonic crystal cavity2.5 μm18,000NanocavityThis work
    Photonic crystal cavity2.3 μm200Nanocavity[24]
    Racetrack microring5.3 μm20,000Microcavity[20]
    Racetrack microring3.8 μm5000Microcavity[28]
    Table 1. Comparison of MIR Germanium Cavities
    Ting-Hui Xiao, Ziqiang Zhao, Wen Zhou, Mitsuru Takenaka, Hon Ki Tsang, Zhenzhou Cheng, Keisuke Goda. High-Q germanium optical nanocavity[J]. Photonics Research, 2018, 6(9): 925
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