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    Journals >Chinese Journal of Lasers >Volume 49 >Issue 1 >Page 0101007 > Article
    • Chinese Journal of Lasers
    • Vol. 49, Issue 1, 0101007 (2022)
    Research Progress in Chalcogenide Glass Fibers for Infrared Laser Delivery
    Hao Zhang1、2, Haitao Guo1、*, Yantao Xu1、2, Man Li3, and Wenchao Ma3
    Author Affiliations
  • 1State Key Laboratory of Transient Optics and Photonics, Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi’an, Shaanxi 710119, China
  • 2University of Chinese Academy of Sciences, Beijing 100045, China
  • 3Science and Technology on Electro-Optical Information Security Control Laboratory, Tianjin 300308, China
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    DOI: 10.3788/CJL202249.0101007 Cite this Article Set citation alerts
    Hao Zhang, Haitao Guo, Yantao Xu, Man Li, Wenchao Ma. Research Progress in Chalcogenide Glass Fibers for Infrared Laser Delivery[J]. Chinese Journal of Lasers, 2022, 49(1): 0101007 Copy Citation Text show less
    Relationship between incident and transmitted laser powers of 2.053 μm laser through 20 cm length，12 μm core diameter, uncoated and AR-coated As40S60 single mode fibers [8]
    Fig. 1. Relationship between incident and transmitted laser powers of 2.053 μm laser through 20 cm length，12 μm core diameter, uncoated and AR-coated As40S60 single mode fibers [8]
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    Transmission of 5.4 μm CO CW laser through As40S60 and Ge10As30S60 fibers under forced air-cooling conditions [10]
    Fig. 2. Transmission of 5.4 μm CO CW laser through As40S60 and Ge10As30S60 fibers under forced air-cooling conditions [10]
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    Relationship between input and output powers of 10.6 μm CO2 laser through 100 cm long Ge15As25Se40Te20 fiber [14]
    Fig. 3. Relationship between input and output powers of 10.6 μm CO2 laser through 100 cm long Ge15As25Se40Te20 fiber [14]
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    Chalcogenide LMA-PCFs with different structural geometries [16]
    Fig. 4. Chalcogenide LMA-PCFs with different structural geometries [16]
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    Experiment and result of 2 μm CW laser transmission [18]. (a)(b)(c)Devices；(d)relationship between incident and output powers through 47 cm long fiber
    Fig. 5. Experiment and result of 2 μm CW laser transmission [18]. (a)(b)(c)Devices；(d)relationship between incident and output powers through 47 cm long fiber
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    Cross-sectional SEM images of hollow-core Bragg fiber at various magnifications [22]
    Fig. 6. Cross-sectional SEM images of hollow-core Bragg fiber at various magnifications [22]
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    Cross sections of fiber preform and hollow-core Bragg fiber[23]. (a) Fiber preform; (b) hollow-core Bragg fiber
    Fig. 7. Cross sections of fiber preform and hollow-core Bragg fiber[23]. (a) Fiber preform; (b) hollow-core Bragg fiber
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    Chalcogenide HC-PCFs with different structures [25]. (a) Hexagonal lattice cladding structure; (b) Kagome cladding structure
    Fig. 8. Chalcogenide HC-PCFs with different structures [25]. (a) Hexagonal lattice cladding structure; (b) Kagome cladding structure
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    Cross-sectional SEM image of chalcogenide negative curvature fiber [36]
    Fig. 9. Cross-sectional SEM image of chalcogenide negative curvature fiber [36]
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    Transmission performances of CO2 laser in chalcogenide negative curvature fiber [36]. (a) Measured optical loss spectrum; (b) intensity distribution of CO2 laser over fiber core
    Fig. 10. Transmission performances of CO2 laser in chalcogenide negative curvature fiber [36]. (a) Measured optical loss spectrum; (b) intensity distribution of CO2 laser over fiber core
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    Cross sections of fiber under different inner tube pressures [39] . (a) 0; (b) 3.5×103 Pa; (c) 4×103 Pa；(d) 4.5×103 Pa
    Fig. 11. Cross sections of fiber under different inner tube pressures [39] . (a) 0; (b) 3.5×103 Pa; (c) 4×103 Pa；(d) 4.5×103 Pa
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    Characterization of fiber performances[39]. (a) Cross section of arch-shape negative curvature fiber；(b) transmission band measured by FTIR
    Fig. 12. Characterization of fiber performances[39]. (a) Cross section of arch-shape negative curvature fiber；(b) transmission band measured by FTIR
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    Laser wavelength /μmLaserFiber materialCore diameter /μmFiber length /cmLaser transmission performanceYear
    2PLAs40S60160—Iin＝26.9 GW/cm21998
    2.94As40S601601000Eout>1 mJ1998
    As-Se-Te1000—Eout＝4.6 mJ2007
    2.053CWAs40S601220Pout＝10.3 W2018
    2.520Pout＝1 W
    4.10225Pout＝0.5 W
    5.4As-S10001000Pout＝59 W1985
    As40S6010001000Pout＝226 W1993
    Ge10As30S60Pout＝180 W
    10.6Se25Te30I45400100Pout＝0.82 W1991
    Ge-Se-Te450100Pout＝10.7 W1992
    Ge30As10Se30Te30270100Pout＝0.6 W1996
    Ge15As25Se40Te20400100Pout＝1.37 W2019
    Table 1. Laser transmission performances of different chalcogenide fibers [5-14]
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    Hao Zhang, Haitao Guo, Yantao Xu, Man Li, Wenchao Ma. Research Progress in Chalcogenide Glass Fibers for Infrared Laser Delivery[J]. Chinese Journal of Lasers, 2022, 49(1): 0101007
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