• Photonics Research
  • Vol. 5, Issue 3, 233 (2017)
Jiwen Cui1、*, Hong Dang1, Kunpeng Feng1, Wenlei Yang2, Tao Geng2, Yang Hu1、3, Yuanhang Zhang1, Dong Jiang1, Xudong Chen2, and Jiubin Tan1
Author Affiliations
  • 1Center of Ultra-precision Optoelectronic Instrument, Harbin Institute of Technology, Harbin 150080, China
  • 2Key Laboratory of In-Fiber Integrated Optics, Ministry of Education, Harbin Engineering University, Harbin 150001, China
  • 3VI Service Network Co., Ltd., Shanghai 201203, China
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    DOI: 10.1364/PRJ.5.000233 Cite this Article Set citation alerts
    Jiwen Cui, Hong Dang, Kunpeng Feng, Wenlei Yang, Tao Geng, Yang Hu, Yuanhang Zhang, Dong Jiang, Xudong Chen, Jiubin Tan. Stimulated Brillouin scattering evolution and suppression in an integrated stimulated thermal Rayleigh scattering-based fiber laser[J]. Photonics Research, 2017, 5(3): 233 Copy Citation Text show less
    Typical sketch of a tapered fiber, where w and D are diameters of the waist and conventional SMF, respectively; the repetition length Ltaper is the distance between two adjacent tapers; lwaist, ltrans, and ltaper are the lengths of the waist region, transition region, and tapered region.
    Fig. 1. Typical sketch of a tapered fiber, where w and D are diameters of the waist and conventional SMF, respectively; the repetition length Ltaper is the distance between two adjacent tapers; lwaist, ltrans, and ltaper are the lengths of the waist region, transition region, and tapered region.
    Simulation results: (a) Aeff and BFS versus core radius: (b) BGS versus waist, (c) total generated Stokes power versus waist, (d) BGS versus rtaper, and (e) total generated stokes power versus rtaper.
    Fig. 2. Simulation results: (a) Aeff and BFS versus core radius: (b) BGS versus waist, (c) total generated Stokes power versus waist, (d) BGS versus rtaper, and (e) total generated stokes power versus rtaper.
    Experimental results of SBS suppression method: (a) experimental setup; (b)–(e) theoretical/experimental power ratio between the SBS and Rayleigh scattering peaks versus rtaper when the waist is 105, 90, 75, and 60 μm, respectively; (f) optical power spectra of backward-scattered light in conventional SMF and tapered fibers (rtaper=0.02 and w=75 μm) with the same pump power.
    Fig. 3. Experimental results of SBS suppression method: (a) experimental setup; (b)–(e) theoretical/experimental power ratio between the SBS and Rayleigh scattering peaks versus rtaper when the waist is 105, 90, 75, and 60 μm, respectively; (f) optical power spectra of backward-scattered light in conventional SMF and tapered fibers (rtaper=0.02 and w=75  μm) with the same pump power.
    Variation tendency of the scattered optical power when the optical power of incident light changes.
    Fig. 4. Variation tendency of the scattered optical power when the optical power of incident light changes.
    Schematic diagram of the tunable STRS-based SLM laser with ultranarrow linewidth.
    Fig. 5. Schematic diagram of the tunable STRS-based SLM laser with ultranarrow linewidth.
    Spectra detected by delayed self-heterodyne method: (a) without secondary cavities, (b) with secondary cavities, (c) without linewidth compression device, and (d) with linewidth compression device.
    Fig. 6. Spectra detected by delayed self-heterodyne method: (a) without secondary cavities, (b) with secondary cavities, (c) without linewidth compression device, and (d) with linewidth compression device.
    Jiwen Cui, Hong Dang, Kunpeng Feng, Wenlei Yang, Tao Geng, Yang Hu, Yuanhang Zhang, Dong Jiang, Xudong Chen, Jiubin Tan. Stimulated Brillouin scattering evolution and suppression in an integrated stimulated thermal Rayleigh scattering-based fiber laser[J]. Photonics Research, 2017, 5(3): 233
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