• Chinese Journal of Lasers
  • Vol. 49, Issue 1, 0101006 (2022)
Xian Feng*, Zhiyong Yang**, and Jindan Shi***
Author Affiliations
  • Jiangsu Key Laboratory of Advanced Laser Materials and Devices, School of Physics and Electronic Engineering, Jiangsu Normal University, Xuzhou, Jiangsu 221116, China
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    DOI: 10.3788/CJL202249.0101006 Cite this Article Set citation alerts
    Xian Feng, Zhiyong Yang, Jindan Shi. Progress in Chalcogenide Glass Photonic Crystal Fibers with Ultra-Large Mode Area[J]. Chinese Journal of Lasers, 2022, 49(1): 0101006 Copy Citation Text show less
    Summary of reported maximum incident CW laser damage threshold of ChG fibers[7-12]
    Fig. 1. Summary of reported maximum incident CW laser damage threshold of ChG fibers[7-12]
    Comparison of maximum resistable peak power density of silica, fluoride, fluorotellurite, and ChG fibers under irradiation of pulsed laser with various pulse durations[28-36]
    Fig. 2. Comparison of maximum resistable peak power density of silica, fluoride, fluorotellurite, and ChG fibers under irradiation of pulsed laser with various pulse durations[28-36]
    Fabrication flow of ULMA ChG PCF. (a)(c) Extruded chalcogenide glass rod and tubes for PCF fabrication; (d) preform composed by low-index rod and high-index tube using rod-in-tube method; (e) stacked ChG preform for ULMA PCF; (f) schematic of drawing all-solid ChG PCF
    Fig. 3. Fabrication flow of ULMA ChG PCF. (a)(c) Extruded chalcogenide glass rod and tubes for PCF fabrication; (d) preform composed by low-index rod and high-index tube using rod-in-tube method; (e) stacked ChG preform for ULMA PCF; (f) schematic of drawing all-solid ChG PCF
    Measured optical properties of host materials for ULMA ChG PCF and numerical simulations of single-mode ULMA ChG PCF. (a) Measured transmission and (b) refractive index curves of prepared Ge10As24S66 and Ge12As24Se64 glasses; (c) schematic of ULMA ChG PCF with two rings of low-index filling rods; calculated mode profiles of (d) LP01 and (e) LP11; calculated confinement losses (CL) of all-solid Ge-As-Se/Ge-As-S ULMA PCF with core diameter of 80 μm at the wavelength of 2 μm and 4 μm of the PCFs with (f) 2-ring structure and (g) 1-ring structure
    Fig. 4. Measured optical properties of host materials for ULMA ChG PCF and numerical simulations of single-mode ULMA ChG PCF. (a) Measured transmission and (b) refractive index curves of prepared Ge10As24S66 and Ge12As24Se64 glasses; (c) schematic of ULMA ChG PCF with two rings of low-index filling rods; calculated mode profiles of (d) LP01 and (e) LP11; calculated confinement losses (CL) of all-solid Ge-As-Se/Ge-As-S ULMA PCF with core diameter of 80 μm at the wavelength of 2 μm and 4 μm of the PCFs with (f) 2-ring structure and (g) 1-ring structure
    Measured guiding performances of fabricated single-mode ULMA ChG PCF. (a) Scanning electron microscope (SEM) photograph of single-mode ULMA ChG PCF; (b) near-field and (c) far-field mode profiles observed from ULMA ChG PCF output end at 4 μm; (d) measured loss spectra of unclad Ge12As24Se64 glass fiber in 29 μm and ULMA ChG PCF at 4 μm
    Fig. 5. Measured guiding performances of fabricated single-mode ULMA ChG PCF. (a) Scanning electron microscope (SEM) photograph of single-mode ULMA ChG PCF; (b) near-field and (c) far-field mode profiles observed from ULMA ChG PCF output end at 4 μm; (d) measured loss spectra of unclad Ge12As24Se64 glass fiber in 29 μm and ULMA ChG PCF at 4 μm
    Origin of bending loss in PCF with ultra-low NA. (a) Straight fiber; (b) bent fiber
    Fig. 6. Origin of bending loss in PCF with ultra-low NA. (a) Straight fiber; (b) bent fiber
    Microstructure and numerical simulation of dual-moded ULMA ChG PCF. (a) Schematic of dual-moded ULMA ChG PCF; (b) SEM image of fabricated dual-moded ULMA ChG PCF;(c)calculated CLs of LP01 and LP11 modes of the fabricated fiber (Λ=90 μm, d1/Λ=0.40, and d2/Λ=0.55) in the range of 28 μm, in comparison with the PCF with uniform d/Λ=0.40 (d1=d2) and Λ=90 μm;(d)calculated Aeff of LP01 and LP11 modes of the fabricated fiber (Λ=90 μm, d1/Λ=0.40, and d2/Λ=0.55) in the range of 28 μm, in comparison with the PCF with uniform d/Λ=0.40 (d1=d2) and Λ=90 μm
    Fig. 7. Microstructure and numerical simulation of dual-moded ULMA ChG PCF. (a) Schematic of dual-moded ULMA ChG PCF; (b) SEM image of fabricated dual-moded ULMA ChG PCF;(c)calculated CLs of LP01 and LP11 modes of the fabricated fiber (Λ=90 μm, d1/Λ=0.40, and d2/Λ=0.55) in the range of 28 μm, in comparison with the PCF with uniform d/Λ=0.40 (d1=d2) and Λ=90 μm;(d)calculated Aeff of LP01 and LP11 modes of the fabricated fiber (Λ=90 μm, d1/Λ=0.40, and d2/Λ=0.55) in the range of 28 μm, in comparison with the PCF with uniform d/Λ=0.40 (d1=d2) and Λ=90 μm
    Measured bending loss and fitting with exponential decay function of dual-moded ULMA ChG PCF with bending radius under different diameters of the incident 2-μm laser spot. (a) ~75 μm; (b) ~100 μm
    Fig. 8. Measured bending loss and fitting with exponential decay function of dual-moded ULMA ChG PCF with bending radius under different diameters of the incident 2-μm laser spot. (a) ~75 μm; (b) ~100 μm
    Measured optical homogeneity of Ge-As-Se chalcogenide glass with 100-mm aperture
    Fig. 9. Measured optical homogeneity of Ge-As-Se chalcogenide glass with 100-mm aperture
    Laser wavelength /μmFiber hostCore diameter /μmMaximum resisted power /WFiber typeRef.
    2As2S31212Few-moded fiber excited by LP01 mode[10]
    5.4As2S31000460Multimode fiber[7]
    10.6Ge-As-Se-Te4006.16Multimode fiber[12]
    Table 1. Reported maximum resisted mid-IR power of ChG fibers
    Fiber host materialLaser damage threshold /(GW·cm-2)Ref.
    Silica (SiO2)~0.8[28]
    Fluorotellurite (TeO2-BaF2-Y2O3)~0.07[34]
    Fluoride(ZrF4-based)~0.02[31]
    Chalcogenide (Ge-As-S)0.01-0.02[11]
    Table 2. Damage threshold of various glass fibers, including silica, fluoride, fluorotellurite, and ChG fibers under CW laser irradiation
    Xian Feng, Zhiyong Yang, Jindan Shi. Progress in Chalcogenide Glass Photonic Crystal Fibers with Ultra-Large Mode Area[J]. Chinese Journal of Lasers, 2022, 49(1): 0101006
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