• Advanced Photonics Nexus
  • Vol. 3, Issue 6, 066005 (2024)
Lei Zhang1, Xin Wang1, Yong Zhang1,2,*, Jian Shen1..., Chenglong Feng1, Jian Xu3, Min Liu3, Wei Wang4, Yongqiang Deng5, Yang Xu5, Yi Li5, Guofeng Yin6 and Yikai Su1|Show fewer author(s)
Author Affiliations
  • 1Shanghai Jiao Tong University, State Key Lab of Advanced Optical Communication Systems and Networks, Department of Electron Engineering, Shanghai, China
  • 2East China Normal University, State Key Laboratory of Precision Spectroscopy, Shanghai, China
  • 3Shanghai Jiao Tong University, Center for Advanced Electronic Materials and Devices, Shanghai, China
  • 4Shanghai Industrial μTechnology Research Institute, Shanghai, China
  • 5Beijing R&D Institute, VanJee Technology, Beijing, China
  • 6Wuhan Enlarging Photonics Technology Co. Ltd., Wuhan, China
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    DOI: 10.1117/1.APN.3.6.066005 Cite this Article Set citation alerts
    Lei Zhang, Xin Wang, Yong Zhang, Jian Shen, Chenglong Feng, Jian Xu, Min Liu, Wei Wang, Yongqiang Deng, Yang Xu, Yi Li, Guofeng Yin, Yikai Su, "Hybrid silicon-barium-titanate tunable racetrack resonators based on chemical solution deposition," Adv. Photon. Nexus 3, 066005 (2024) Copy Citation Text show less
    (a) Cross section of the hybrid Si-BTO waveguide. (b) Simulated mode profile of the hybrid Si-BTO waveguide. (c) Simulated light confinement factor and effective index as a function of the thickness of the silicon layer. (d). Simulated light confinement factor and effective index as a function of the thickness of BTO thin film. (e) Simulated light confinement factor and effective index as a function of the width of the silicon layer.
    Fig. 1. (a) Cross section of the hybrid Si-BTO waveguide. (b) Simulated mode profile of the hybrid Si-BTO waveguide. (c) Simulated light confinement factor and effective index as a function of the thickness of the silicon layer. (d). Simulated light confinement factor and effective index as a function of the thickness of BTO thin film. (e) Simulated light confinement factor and effective index as a function of the width of the silicon layer.
    (a) 3D schematic diagram of hybrid Si-BTO racetrack resonator. (b) Simulated cross-sectional static electric field distribution of hybrid Si-BTO racetrack resonator. (c) Simulated average electric field as a function of electrode gaps. (d) Simulated EO overlap factor as a function of the thicknesses of silicon layers and BTO films.
    Fig. 2. (a) 3D schematic diagram of hybrid Si-BTO racetrack resonator. (b) Simulated cross-sectional static electric field distribution of hybrid Si-BTO racetrack resonator. (c) Simulated average electric field as a function of electrode gaps. (d) Simulated EO overlap factor as a function of the thicknesses of silicon layers and BTO films.
    (a) Fabrication process of the hybrid Si-BTO devices using the CSD method. (b) SEM photo of the surface of the BTO thin film. (c) SEM photo of the cross section of the Si-BTO waveguide region. (d) AFM on the surface of the BTO thin film. (e) Measured surface roughness across different areas. (f) XRD spectrum of the deposited BTO thin film.
    Fig. 3. (a) Fabrication process of the hybrid Si-BTO devices using the CSD method. (b) SEM photo of the surface of the BTO thin film. (c) SEM photo of the cross section of the Si-BTO waveguide region. (d) AFM on the surface of the BTO thin film. (e) Measured surface roughness across different areas. (f) XRD spectrum of the deposited BTO thin film.
    (a) Measured transmission spectrum of the silicon racetrack resonator. (b) Lorentz fitting of a resonance dip of the silicon racetrack resonator. (c) Measured transmission spectrum of the hybrid Si-BTO racetrack resonator. (d) Lorentz fitting of a resonance dip of the hybrid Si-BTO racetrack resonator.
    Fig. 4. (a) Measured transmission spectrum of the silicon racetrack resonator. (b) Lorentz fitting of a resonance dip of the silicon racetrack resonator. (c) Measured transmission spectrum of the hybrid Si-BTO racetrack resonator. (d) Lorentz fitting of a resonance dip of the hybrid Si-BTO racetrack resonator.
    (a) Measured transmission spectra when applying different voltages. (b) Linear fitting of the resonance wavelengths as a function of the applied voltages. (c) Measured I-V hysteresis curve of the fabricated racetrack resonators. (d) Power consumption as a function of resonance wavelength shift.
    Fig. 5. (a) Measured transmission spectra when applying different voltages. (b) Linear fitting of the resonance wavelengths as a function of the applied voltages. (c) Measured I-V hysteresis curve of the fabricated racetrack resonators. (d) Power consumption as a function of resonance wavelength shift.
    (a) Experimental setup for high-speed test. EDFA, erbium-doped optical fiber amplifier; PC, polarization controller; EA, electric amplifier; DUT, device under test; PD, photodetector; DSO, digital storage oscilloscope. (b) Measured eye diagrams of NRZ signals at 30, 40, and 50 Gbps. (c) BER as a function of the received optical power.
    Fig. 6. (a) Experimental setup for high-speed test. EDFA, erbium-doped optical fiber amplifier; PC, polarization controller; EA, electric amplifier; DUT, device under test; PD, photodetector; DSO, digital storage oscilloscope. (b) Measured eye diagrams of NRZ signals at 30, 40, and 50 Gbps. (c) BER as a function of the received optical power.
    MethodThickness (nm)Surface roughness (nm)Crystallinereff (pm/V)Equipment costFabrication process
    RF sputtering191023.1Polycrystalline6HighComplex
    PLD18973.1Single-crystal37HighComplex
    MBE341700.4Single-crystal380HighComplex
    CSD1505.6Polycrystalline27.2LowSimple
    Table 1. Comparison between different deposition methods of BTO film.
    ReferenceDeposition processTuning mechanismTuning efficiency (pm/V)Power consumption (pm/nW)
    Silicon36TO0.0048
    Silicon34FCPD0.01
    SiN-AlN32SputteringPO0.20.2
    HfO2-Si31ALDPO8.47.69
    BTO-SiN11MBEEO2523.58
    LN-Si37BondingEO3
    This workCSDEO6.52.16
    Table 2. Performance comparison of the integrated tuning devices.
    Lei Zhang, Xin Wang, Yong Zhang, Jian Shen, Chenglong Feng, Jian Xu, Min Liu, Wei Wang, Yongqiang Deng, Yang Xu, Yi Li, Guofeng Yin, Yikai Su, "Hybrid silicon-barium-titanate tunable racetrack resonators based on chemical solution deposition," Adv. Photon. Nexus 3, 066005 (2024)
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