• Advanced Photonics
  • Vol. 7, Issue 1, 016002 (2025)
Xuelin Zhang1, Jiangbing Du1,*, Ke Xu2, and Zuyuan He1
Author Affiliations
  • 1Shanghai Jiao Tong University, State Key Laboratory of Advanced Optical Communication Systems and Networks, Shanghai, China
  • 2Harbin Institute of Technology (Shenzhen), Department of Electronic and Information Engineering, Shenzhen, China
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    DOI: 10.1117/1.AP.7.1.016002 Cite this Article Set citation alerts
    Xuelin Zhang, Jiangbing Du, Ke Xu, Zuyuan He, "Waveguide superlattices with artificial gauge field toward colorless and low-crosstalk ultrahigh-density photonic integration," Adv. Photon. 7, 016002 (2025) Copy Citation Text show less
    Schematic of the waveguide superlattices with AGF.
    Fig. 1. Schematic of the waveguide superlattices with AGF.
    (a) Band-gap diagram (first two minibands) of a typical straight waveguide array for a=2.65 μm, w1=1 μm, w2=0.85 μm, Δn=0.31, λ=1.55 μm, and n0=1.450, where the propagation constant is plotted as a function of the Bloch wave number and the shaded regions represent the bands. (b) Ninth-order (J9) and tenth-order (J10) Bessel modulation of the first kind. J10 and J9 have the same sign in the marked red region.
    Fig. 2. (a) Band-gap diagram (first two minibands) of a typical straight waveguide array for a=2.65  μm, w1=1  μm, w2=0.85  μm, Δn=0.31, λ=1.55  μm, and n0=1.450, where the propagation constant is plotted as a function of the Bloch wave number and the shaded regions represent the bands. (b) Ninth-order (J9) and tenth-order (J10) Bessel modulation of the first kind. J10 and J9 have the same sign in the marked red region.
    Simulated normalized field evolution in (a) normal waveguides, (b) ordinary superlattice, (c) AGF waveguide array, and (d) AGF-enabled superlattice, where gap = 400 nm, L=200 μm. Schematic top views of the simulated structures are located at the corners of each subimage.
    Fig. 3. Simulated normalized field evolution in (a) normal waveguides, (b) ordinary superlattice, (c) AGF waveguide array, and (d) AGF-enabled superlattice, where gap = 400 nm, L=200  μm. Schematic top views of the simulated structures are located at the corners of each subimage.
    Simulated crosstalk in the designed waveguide array (gap = 400 nm, λ=700 to 1700 nm) when (a) fundamental TE mode and (b) fundamental TM mode are launched, respectively. The pink planes correspond to −28 and −25 dB, respectively.
    Fig. 4. Simulated crosstalk in the designed waveguide array (gap = 400 nm, λ=700 to 1700 nm) when (a) fundamental TE mode and (b) fundamental TM mode are launched, respectively. The pink planes correspond to 28 and 25  dB, respectively.
    (a) The top-view microscope image of the fabricated device on the Si3N4 platform (gap=400 nm, L=200 μm). (b) SEM image of the cross section of a waveguide (gap=400 nm, L=200 μm). (c) The top-view microscope image of the fabricated device on the Si3N4 platform (gap=500 nm, L=1 mm). (d) Experimentally recorded light trajectory in modulated samples for 850 nm.
    Fig. 5. (a) The top-view microscope image of the fabricated device on the Si3N4 platform (gap=400  nm, L=200  μm). (b) SEM image of the cross section of a waveguide (gap=400  nm, L=200  μm). (c) The top-view microscope image of the fabricated device on the Si3N4 platform (gap=500  nm, L=1  mm). (d) Experimentally recorded light trajectory in modulated samples for 850 nm.
    (a) Measured transmission spectra of the AGF-enabled superlattice (gap=400 nm). (b) Measured transmission spectra of the AGF-enabled superlattice (gap=500 nm). The pink planes correspond to −24 and −28 dB, respectively.
    Fig. 6. (a) Measured transmission spectra of the AGF-enabled superlattice (gap=400  nm). (b) Measured transmission spectra of the AGF-enabled superlattice (gap=500  nm). The pink planes correspond to 24 and 28  dB, respectively.
    Simulated crosstalk for AGF-enabled superlattice with (a) ΔA=−50 nm and (b) ΔA=+50 nm. The pink planes correspond to −20 dB.
    Fig. 7. Simulated crosstalk for AGF-enabled superlattice with (a) ΔA=50  nm and (b) ΔA=+50  nm. The pink planes correspond to 20  dB.
    Simulated crosstalk for AGF-enabled superlattice that widths of all waveguides (a) increase by 25 nm and (b) decrease by 25 nm. The pink planes correspond to −20 dB.
    Fig. 8. Simulated crosstalk for AGF-enabled superlattice that widths of all waveguides (a) increase by 25 nm and (b) decrease by 25 nm. The pink planes correspond to 20  dB.
    (a) Measured SNR profiles of the system after transmission through the waveguide array. (b) The bit allocation of 112-Gbit/s DMT signals. Inset: constellations of different subcarriers.
    Fig. 9. (a) Measured SNR profiles of the system after transmission through the waveguide array. (b) The bit allocation of 112-Gbit/s DMT signals. Inset: constellations of different subcarriers.
    Xuelin Zhang, Jiangbing Du, Ke Xu, Zuyuan He, "Waveguide superlattices with artificial gauge field toward colorless and low-crosstalk ultrahigh-density photonic integration," Adv. Photon. 7, 016002 (2025)
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