• Photonics Research
  • Vol. 6, Issue 11, 987 (2018)
Liuqing He1、2, Yuhao Guo1、2, Zhaohong Han3, Kazumi Wada3、4, Jurgen Michel3, Anuradha M. Agarwal3, Lionel C. Kimerling3, Guifang Li1、2、5, and Lin Zhang1、2、*
Author Affiliations
  • 1Key Laboratory of Opto-electronic Information Technical Science of Ministry of Education, School of Precision Instruments and Opto-electronics Engineering, Tianjin University, Tianjin 300072, China
  • 2Key Laboratory of Integrated Opto-electronic Technologies and Devices in Tianjin, School of Precision Instruments and Opto-electronics Engineering, Tianjin University, Tianjin 300072, China
  • 3Department of Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
  • 4Department of Materials Engineering, University of Tokyo, Tokyo 113-8656, Japan
  • 5College of Optics and Photonics, CREOL and FPCE, University of Central Florida, Orlando, Florida 32816, USA
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    DOI: 10.1364/PRJ.6.000987 Cite this Article Set citation alerts
    Liuqing He, Yuhao Guo, Zhaohong Han, Kazumi Wada, Jurgen Michel, Anuradha M. Agarwal, Lionel C. Kimerling, Guifang Li, Lin Zhang. Broadband athermal waveguides and resonators for datacom and telecom applications[J]. Photonics Research, 2018, 6(11): 987 Copy Citation Text show less
    Structure of the proposed broadband athermal waveguide, which consists of a Si core, a TiO2 lower cladding, and a Si3N4 upper cladding.
    Fig. 1. Structure of the proposed broadband athermal waveguide, which consists of a Si core, a TiO2 lower cladding, and a Si3N4 upper cladding.
    Effective TOC of the proposed broadband athermal waveguide, with a small variation of ±1×10−6/K in the waveband of 1400 to 1700 nm. The insets show the norm of the electric field, |E|, of the waveguide mode at different wavelengths, 1450, 1550, 1650, and 1750 nm, respectively.
    Fig. 2. Effective TOC of the proposed broadband athermal waveguide, with a small variation of ±1×106/K in the waveband of 1400 to 1700 nm. The insets show the norm of the electric field, |E|, of the waveguide mode at different wavelengths, 1450, 1550, 1650, and 1750 nm, respectively.
    Shifts of effective TOC curves when the structural parameters are changed, with (a) varied W of ±10%, (b) varied H1 of ±50%, (c) varied H2 of ±5%, and (d) varied H3 of ±1%.
    Fig. 3. Shifts of effective TOC curves when the structural parameters are changed, with (a) varied W of ±10%, (b) varied H1 of ±50%, (c) varied H2 of ±5%, and (d) varied H3 of ±1%.
    (a) Optical loss of the proposed waveguide. It shows a low-loss performance in the bandwidth with a broadband athermal property. (b) Effective-TOC curves of the micro-ring resonators with different ring radii. (c) Bending loss with different radii. This shows a low-loss performance and a stable athermal property of the proposed broadband athermal micro-ring resonators.
    Fig. 4. (a) Optical loss of the proposed waveguide. It shows a low-loss performance in the bandwidth with a broadband athermal property. (b) Effective-TOC curves of the micro-ring resonators with different ring radii. (c) Bending loss with different radii. This shows a low-loss performance and a stable athermal property of the proposed broadband athermal micro-ring resonators.
    TDWS of the microring resonator with a radius of 30 μm using the proposed waveguide. The TDWS is ±0.5 pm/K in the wavelength range of 1400 to 1700 nm, corresponding to a wavelength shift of <15 pm with a temperature change of 30°C.
    Fig. 5. TDWS of the microring resonator with a radius of 30 μm using the proposed waveguide. The TDWS is ±0.5  pm/K in the wavelength range of 1400 to 1700 nm, corresponding to a wavelength shift of <15  pm with a temperature change of 30°C.
    Liuqing He, Yuhao Guo, Zhaohong Han, Kazumi Wada, Jurgen Michel, Anuradha M. Agarwal, Lionel C. Kimerling, Guifang Li, Lin Zhang. Broadband athermal waveguides and resonators for datacom and telecom applications[J]. Photonics Research, 2018, 6(11): 987
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