Infrared and Laser Engineering, Volume. 52, Issue 5, 20230228(2023)

Progress on mid-infrared glass optical fiber materials and Raman laser source (invited)

Yadong Jiao, Zhixu Jia, Xiaohui Guo, Chengyun Zhang, Weiping Qin, and Guanshi Qin
Author Affiliations
  • State Key Laboratory of Integrated Optoelectronics, College of Electronic Science and Engineering, Jilin University, Changchun 130012, China
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    Figures & Tables(27)
    The output power and operating wavelength of near-infrared and mid-infrared Raman laser source in recent years[13-24]. (a) Raman fiber lasers; (b) Raman soliton laser source
    Raman spectra of fluorozirconate, fluoroindate and fluoroaluminate glasses[32]
    Experimental setup of nested cavity for 2231 nm Raman laser based on fluoride glass fiber[18]
    Output power of 2231 nm Raman laser versus launched pump power[18]
    Spectra of tunable Raman soliton based on InF3 glass fiber[19]. (a) Experimental measurement results; (b) Numerical simulation results
    Experimental setup for generation of mid-infrared Raman soliton in fluoride fiber[48]
    Spectra of Raman soliton from 2.39 to 3.17 μm. (a) Comparison between measured and computed spectral profiles; (b) Numerical simulation of the evolution of the spectrum along the 40 cm silica fiber followed by the 3.5 m ZBLAN fiber[48]
    Cascaded Raman shift spectra of 8 m long As-S optical fiber[64]
    Experimental setup of 3.77 μm As2S3-based cascaded RFL[20]
    The output power of 3.77 μm Raman laser versus launched pump power for output cascaded Stokes FBG with peak refluctivity of 98%, 92%, and 80%[20]
    (a) Cross section of the AsSe2-As2S3 MOF[70]; (b) Black line is the fundamental model refractive index and blue line is the calculated group velocity dispersion of the AsSe2-As2S3 MOF
    MID-IR SSFS and DW spectra at the pump wavelength of ~2.8 μm with the average pump powers of 55, 66, 81, 98, 112, and 144 mW[70]
    The calculated output spectra of the AsSe2-As2S5 fiber with a core diameter ranging from 4.5 μm to 6.5 μm[23]. (a) Use the 4.1 μm pump; (b) Use the 5.2 μm pump
    Raman gain coefficient profiles of TBZN glass[79]
    Simulated evolution of Raman soliton during propagation in tellurate microstructure fibers[22]
    Raman gain spectrum of TBY glass[89]
    Group velocity dispersion curve of fluorotellurite fibers. Inset: cross-sectional scanning electron micrograph of fluorotellurite fibers[89]
    Experimental results of third cascaded Raman shift based on fluorotellurtie fiber[89]. (a) Output spectra; (b) Output power
    Experimental results of fifth cascaded Raman shift[89]
    Experimental setup of cascaded Raman amplifier based on fluorotellurite fiber[90]
    The output of cascade Raman amplifier powers and corresponding conversion efficient versus the launched pump power[90]. (a) First-order amplifier; (b) Second-order cascaded amplifier; (c) Third-order cascaded amplifier
    Dependence of the spectrum from the fluorotellurite fiber on launched pump power in the amplifier[24]
    Simulation results of the spectra of the output pulses when pumping at 2.8 μm[23]
    Group velocity dispersion curves of LP01 modes propagating in the fulorotellurite fibers. Inset: cross-sectional scanning electron micrograph of fluorotellurite fibers[92]
    Experimental results[92]. (a) Measured spectral evolution of output signals from a 1 m long fluorotellurite fiber with the average power of the 1.98 μm femtosecond laser; (b) Simulated and measured spectra output from the fluorotellurite fiber for a same average pump power of ~1 W; (c) Simulated spectral evolution of output signals from a 1 m long fluorotellurite fiber with the average power of the 1.98 μm femtosecond laser
    • Table 1. Transparency windows and Raman gain characteristics of a few key near-infrared and mid-infrared glass optical fiber materials[9,11-12]

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      Table 1. Transparency windows and Raman gain characteristics of a few key near-infrared and mid-infrared glass optical fiber materials[9,11-12]

      GlassTransparency window/ μm Peak Raman gain at 2.0 μm/ ×10−13 m·W−1Peak Raman shift/ cm−1Nominal Raman gain bandwidth/ cm−1
      Silica0.35-20.5442200
      Fluoride0.22-4.50.57-2.157050
      Arsenic sulfide (As2S3) 1.5-6.521.5-28.534590
      Arsenic selenide (As2Se3) 1.5-9.5100-25522660
      Tellurite0.5-4.54.5-26750140
    • Table 2. Performance parameters of typical commercial chalcogenide optical fibers[52-54]

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      Table 2. Performance parameters of typical commercial chalcogenide optical fibers[52-54]

      IndexCoreActiveIRFlexArt Photonics
      P/NIRT-SUIRT-SEIRF-SIRF-SeIRF-SeGCIR
      Core/cladAs2S3As2Se3As2S3As2Se3As2Se3/GeAs2S3As2S3
      Transmission range/μm2-62-91.5-6.51.5-101.5-9.31.1-6.5
      Core refractibe index2.42.72.42.72.72.42
      Numerical aperture0.250.260.28-0.300.275-0.3500.760.25-0.30
      Typical loss/dB·m−10.15@2.7 μm 0.70@4.0 μm 0.20@6 μm 0.50@4.55 μm 0.05@2.8 μm0.21@2.59 μm0.32@2 μm0.20@2.5-4 μm
      Tensile strength/kpsi>15>15>15>15->70
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    Yadong Jiao, Zhixu Jia, Xiaohui Guo, Chengyun Zhang, Weiping Qin, Guanshi Qin. Progress on mid-infrared glass optical fiber materials and Raman laser source (invited)[J]. Infrared and Laser Engineering, 2023, 52(5): 20230228

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    Paper Information

    Category: Special issue—Frontiers in mid-infrared fiber optic materials and devices technology

    Received: Apr. 18, 2023

    Accepted: --

    Published Online: Jul. 4, 2023

    The Author Email:

    DOI:10.3788/IRLA20230228

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