• Acta Optica Sinica
  • Vol. 38, Issue 8, 0806002 (2018)
Di Wang1、2、*, Xuan Li1, Haoyang Pi1, Fei Yang1、*, Qing Ye1, and Haiwen Cai1、*
Author Affiliations
  • 1 Shanghai Key Laboratory of All Solid-State Laser and Applied Techniques, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2 University of Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.3788/AOS201838.0806002 Cite this Article Set citation alerts
    Di Wang, Xuan Li, Haoyang Pi, Fei Yang, Qing Ye, Haiwen Cai. Interference Field Behind Phase Mask and Its Influence on the Loss Characteristic in Fiber Bragg Gratings[J]. Acta Optica Sinica, 2018, 38(8): 0806002 Copy Citation Text show less
    Wave vectors of incident and diffracted beams
    Fig. 1. Wave vectors of incident and diffracted beams
    Intensity distribution produced inside the fiber core region during FBG fabrication using the phase mask technique. (a) ±1 and 0 diffraction orders; (b)±2, ±1 and 0 diffraction orders; (c)±3, ±2, ±1 and 0 diffraction orders; (d)±4, ±3, ±2, ±1 and 0 diffraction orders
    Fig. 2. Intensity distribution produced inside the fiber core region during FBG fabrication using the phase mask technique. (a) ±1 and 0 diffraction orders; (b)±2, ±1 and 0 diffraction orders; (c)±3, ±2, ±1 and 0 diffraction orders; (d)±4, ±3, ±2, ±1 and 0 diffraction orders
    Spatial spectra of the interfering light field over a fiber core mode field with a diameter of 10 μm. (a) ±1 and 0 diffraction orders; (b)±2, ±1 and 0 diffraction orders; (c)±3, ±2, ±1 and 0 diffraction orders; (d)±4, ±3, ±2, ±1 and 0 diffraction orders
    Fig. 3. Spatial spectra of the interfering light field over a fiber core mode field with a diameter of 10 μm. (a) ±1 and 0 diffraction orders; (b)±2, ±1 and 0 diffraction orders; (c)±3, ±2, ±1 and 0 diffraction orders; (d)±4, ±3, ±2, ±1 and 0 diffraction orders
    Microscopic image of FBG in 10/130 μm fiber
    Fig. 4. Microscopic image of FBG in 10/130 μm fiber
    Phase mask interference field contrast and refractive index modulation depth in FBGs as a function of the distance between the phase mask and the fiber core
    Fig. 5. Phase mask interference field contrast and refractive index modulation depth in FBGs as a function of the distance between the phase mask and the fiber core
    Loss of FBGs with the same reflectivity as a function of refractive index modulation depth in FBGs
    Fig. 6. Loss of FBGs with the same reflectivity as a function of refractive index modulation depth in FBGs
    Phase mask interference field contrast as a function of the diffraction efficiency of 0 order diffracted light
    Fig. 7. Phase mask interference field contrast as a function of the diffraction efficiency of 0 order diffracted light
    Spatial spectra of the interfering light field over a fiber core mode field diameter of 10 μm considering the ±4, ±3, ±2, ±1 and 0 diffraction orders. (a) z=100-110 μm; (b) z=1000-1010 μm; (c) z=2000-2010 μm
    Fig. 8. Spatial spectra of the interfering light field over a fiber core mode field diameter of 10 μm considering the ±4, ±3, ±2, ±1 and 0 diffraction orders. (a) z=100-110 μm; (b) z=1000-1010 μm; (c) z=2000-2010 μm
    Interference distance of ±1 order diffraction lights on z axis varied with incident angle of UV light
    Fig. 9. Interference distance of ±1 order diffraction lights on z axis varied with incident angle of UV light
    Diffracted order0+1-1+2-2+3-3+4-4
    Diffraction efficiency (± 0.3) /%0.939.536.73.94.64.13.53.03.7
    Table 1. Diffraction efficiency of phase mask
    Di Wang, Xuan Li, Haoyang Pi, Fei Yang, Qing Ye, Haiwen Cai. Interference Field Behind Phase Mask and Its Influence on the Loss Characteristic in Fiber Bragg Gratings[J]. Acta Optica Sinica, 2018, 38(8): 0806002
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