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, China2 University of Chinese Academy of Sciences, Beijing 100049, Chinashow less
Fig. 1. Wave vectors of incident and diffracted beams
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
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
Fig. 4. Microscopic image of FBG in 10/130 μm fiber
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
Fig. 6. Loss of FBGs with the same reflectivity as a function of refractive index modulation depth in FBGs
Fig. 7. Phase mask interference field contrast as a function of the diffraction efficiency of 0 order diffracted light
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
Fig. 9. Interference distance of ±1 order diffraction lights on z axis varied with incident angle of UV light
Diffracted order | 0 | +1 | -1 | +2 | -2 | +3 | -3 | +4 | -4 |
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Diffraction efficiency (± 0.3) /% | 0.9 | 39.5 | 36.7 | 3.9 | 4.6 | 4.1 | 3.5 | 3.0 | 3.7 |
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Table 1. Diffraction efficiency of phase mask