Chinese Optics Letters, Volume. 22, Issue 7, 071902(2024)

High-efficiency Brillouin lasing in a planar GeSbS spiral-ring resonator

Jingcui Song1, Yuhang Wei1, Chunxu Wang1,2, Shuixian Yang1, Yan Li1, Tianhua Feng3, Xiaojie Guo4,5、*, and Zhaohui Li1,6
Author Affiliations
  • 1Guangdong Provincial Key Laboratory of Optoelectronic Information Processing Chips and Systems and School of Electronics and Information Technology, Sun Yat-sen University, Guangzhou 510006, China
  • 2Peng Cheng Laboratory, Shenzhen 518000, China
  • 3Department of Electronic Engineering, College of Information Science and Technology, Jinan University, Guangzhou 510632, China
  • 4Guangdong Provincial Key Laboratory of Optical Fiber Sensing and Communications, Institute of Photonics Technology, Jinan University, Guangzhou 510632, China
  • 5College of Physics and Optoelectronic Engineering, Jinan University, Guangzhou 510632, China
  • 6Southern Marine Science and Engineering Guangdong Laboratory (Zhuhai), Zhuhai 519000, China
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    Figures & Tables(5)
    (a) Schematic of the Brillouin laser operation and the spiral-ring resonator design. (b) Conceptual illustration of the Brillouin lasing conditions. Brillouin lasing occurs when the free spectral range (FSR) of the cavity precisely matches the Brillouin frequency shift. (c) The simulated group index of the spiral-ring resonators as a function of the wavelength. The inset shows the fundamental TE mode profile of the SRR. (d) The dependence of the coupling coefficient on the SRR gap with a coupling length lcl of 80 µm. The inset depicts the diagram of the SRR coupling region with a coupling coefficient of K.
    (a) Microscope image of the GeSbS SRR device with a total length of ∼1.7 cm. The bending radius is 100 µm. (b) SEM image of the cross section of the resonator with 3.5-µm-thick SiO2 top cladding. The size of the waveguide core is 2.2 µm × 850 nm.
    (a) Optical transmission of the GeSbS SRR with a resonance linewidth of 190 MHz; (b) the total and intrinsic resonance linewidths of the SRR in the wavelength span from 1530 to 1600 nm. (c) The transmission of the GeSbS SRR redshifts slightly with the increasing temperature. (d) The resonance frequency experiences a 32-GHz blueshift with the temperature fluctuation ranging from 25°C to 41°C with a step of 2°C, illustrating a slope efficiency Δυ/ΔT of −2.023.
    Experimental setups to characterize (a) threshold and slope efficiency and (b) linewidth and phase noise of the Brillouin laser in the GeSbS SRR. ECDL, external cavity diode laser; EDFA, erbium-doped fiber amplifier; ISO, optical isolator; PC, polarization controller; CIR, circulator; DUT, device under test; PM, power meter; AOM, acousto-optical modulator; APD, avalanche photodetector; ESA, electrical spectrum analyzer.
    (a) First-order Stokes signal power versus on-chip pump power; (b) high-resolution optical spectrum of the back-reflected pump and the first-order Stokes signal; inset shows the recorded beat-note on the ESA between them. (c) Electrical power spectrum of the self-heterodyne signal for laser linewidth characterization; (d) single-sideband phase noise of the first-order Stokes emission at different output powers.
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    Jingcui Song, Yuhang Wei, Chunxu Wang, Shuixian Yang, Yan Li, Tianhua Feng, Xiaojie Guo, Zhaohui Li, "High-efficiency Brillouin lasing in a planar GeSbS spiral-ring resonator," Chin. Opt. Lett. 22, 071902 (2024)

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    Paper Information

    Category: Nonlinear Optics

    Received: Dec. 1, 2023

    Accepted: Mar. 12, 2024

    Posted: Mar. 12, 2024

    Published Online: Jul. 17, 2024

    The Author Email: Xiaojie Guo (xjguo@jnu.edu.cn)

    DOI:10.3788/COL202422.071902

    CSTR:32184.14.COL202422.071902

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