• Advanced Photonics
  • Vol. 5, Issue 5, 056008 (2023)
Yu He1, Xingfeng Li1, Yong Zhang1, Shaohua An1, Hongwei Wang1, Zhen Wang1, Haoshuo Chen2, Yetian Huang3, Hanzi Huang3, Nicolas K. Fontaine2, Roland Ryf2, Yuhan Du1, Lu Sun1, Xingchen Ji4, Xuhan Guo1, Yingxiong Song3, Qianwu Zhang3, and Yikai Su1、*
Author Affiliations
  • 1Shanghai Jiao Tong University, Department of Electronic Engineering, State Key Laboratory of Advanced Optical Communication Systems and Networks, Shanghai, China
  • 2Nokia Bell Labs, Murray Hill, New Jersey, United States
  • 3Shanghai University, Key Laboratory of Specialty Fiber Optics and Optical Access Networks, Joint International Research Laboratory of Specialty Fiber Optics and Advanced Communication, Shanghai, China
  • 4Shanghai Jiao Tong University, School of Electronic Information and Electrical Engineering, John Hopcroft Center for Computer Science, Shanghai, China
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    DOI: 10.1117/1.AP.5.5.056008 Cite this Article Set citation alerts
    Yu He, Xingfeng Li, Yong Zhang, Shaohua An, Hongwei Wang, Zhen Wang, Haoshuo Chen, Yetian Huang, Hanzi Huang, Nicolas K. Fontaine, Roland Ryf, Yuhan Du, Lu Sun, Xingchen Ji, Xuhan Guo, Yingxiong Song, Qianwu Zhang, Yikai Su. On-chip metamaterial-enabled high-order mode-division multiplexing[J]. Advanced Photonics, 2023, 5(5): 056008 Copy Citation Text show less
    Planar-metamaterial-enabled refractive-index-distribution manipulation and GIM-enabled adiabatic coupling. (a) Conceptional illustration of a 1D metamaterial structure with a linearly decreasing duty cycle D(z), which can be regarded as a strip waveguide with a varying refractive index neq(z). (b) Schematic configuration of a GIM-based mode coupling process. The GIM waveguide is tailored with a linear duty cycle distribution D(z) along the propagation direction. (c) Simulated electric field distributions of GIM waveguides with different duty cycles. (d) Cross-section view of the GIM-based direction coupler. The Gaussian curves illustrate the power distributions of the modes supported by the GIM waveguide. (e) Calculated coupling coefficients for the tapered DC, GIM coupler, and conventional DC as functions of the propagation distance.
    Fig. 1. Planar-metamaterial-enabled refractive-index-distribution manipulation and GIM-enabled adiabatic coupling. (a) Conceptional illustration of a 1D metamaterial structure with a linearly decreasing duty cycle D(z), which can be regarded as a strip waveguide with a varying refractive index neq(z). (b) Schematic configuration of a GIM-based mode coupling process. The GIM waveguide is tailored with a linear duty cycle distribution D(z) along the propagation direction. (c) Simulated electric field distributions of GIM waveguides with different duty cycles. (d) Cross-section view of the GIM-based direction coupler. The Gaussian curves illustrate the power distributions of the modes supported by the GIM waveguide. (e) Calculated coupling coefficients for the tapered DC, GIM coupler, and conventional DC as functions of the propagation distance.
    GIM-based coupler for 16-channel MDM. (a) Schematic configuration of the GIM-based coupler designed for selective mode coupling. The duty cycle of the GIM waveguide D(z) linearly increases from 30% to 70% along the propagation direction for constructing a linear refractive index distribution. (b) Calculated coupling coefficients κab and κba and the normalized transmission responses for the TE5 mode in the strip waveguide (mode b) and the Bloch mode in the GIM waveguide (mode a), as a function of propagation distance. (c) Simulated electric field distribution for the TE5 mode demultiplexing. (d) Simulated TE15 mode demultiplexing process using GIM structure, conventional DC, and tapered DC, respectively, when the waveguide dimension varies.
    Fig. 2. GIM-based coupler for 16-channel MDM. (a) Schematic configuration of the GIM-based coupler designed for selective mode coupling. The duty cycle of the GIM waveguide D(z) linearly increases from 30% to 70% along the propagation direction for constructing a linear refractive index distribution. (b) Calculated coupling coefficients κab and κba and the normalized transmission responses for the TE5 mode in the strip waveguide (mode b) and the Bloch mode in the GIM waveguide (mode a), as a function of propagation distance. (c) Simulated electric field distribution for the TE5 mode demultiplexing. (d) Simulated TE15 mode demultiplexing process using GIM structure, conventional DC, and tapered DC, respectively, when the waveguide dimension varies.
    GIM-based couplers for 16-channel MDM. (a) Schematic configuration of the 16-channel mode MUX. (b) Microscope image and (c) SEM image of the 16-channel GIM-based mode MUX and deMUX. (d)–(f) Magnified SEM images of the coupling regions.
    Fig. 3. GIM-based couplers for 16-channel MDM. (a) Schematic configuration of the 16-channel mode MUX. (b) Microscope image and (c) SEM image of the 16-channel GIM-based mode MUX and deMUX. (d)–(f) Magnified SEM images of the coupling regions.
    (a)–(p) Measured transmission responses of the 16-channel mode deMUX. Each subplot shows the transmission and crosstalk recorded at 16 output ports for a selected input channel.
    Fig. 4. (a)–(p) Measured transmission responses of the 16-channel mode deMUX. Each subplot shows the transmission and crosstalk recorded at 16 output ports for a selected input channel.
    High-speed data transmission experiment. (a) Experimental setup for the high-speed transmission experiment of the 16-channel MDM chip. The insets show the photographs of the testing platform and the fiber array-based vertical coupling. (b) Monitored optical spectrum of the recombined signal at the receiver side. (c) Calculated BERs of 40-GBaud 16-QAM signals for 16 modes after MIMO-FFE and MLSD. All channels are below the 15% FEC threshold. (d) Recovered constellations for all the 16 modes.
    Fig. 5. High-speed data transmission experiment. (a) Experimental setup for the high-speed transmission experiment of the 16-channel MDM chip. The insets show the photographs of the testing platform and the fiber array-based vertical coupling. (b) Monitored optical spectrum of the recombined signal at the receiver side. (c) Calculated BERs of 40-GBaud 16-QAM signals for 16 modes after MIMO-FFE and MLSD. All channels are below the 15% FEC threshold. (d) Recovered constellations for all the 16 modes.
    Yu He, Xingfeng Li, Yong Zhang, Shaohua An, Hongwei Wang, Zhen Wang, Haoshuo Chen, Yetian Huang, Hanzi Huang, Nicolas K. Fontaine, Roland Ryf, Yuhan Du, Lu Sun, Xingchen Ji, Xuhan Guo, Yingxiong Song, Qianwu Zhang, Yikai Su. On-chip metamaterial-enabled high-order mode-division multiplexing[J]. Advanced Photonics, 2023, 5(5): 056008
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