Microstructure optical fiber with large mode area
A technology of microstructured fiber and large mode field, applied in cladding fiber, multi-layer core/cladding fiber, optical waveguide light guide, etc. The effect of binding loss, simple structure, and low bending loss
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Embodiment 1
[0050] The cross-sectional structure of the fiber is as figure 1 Shown. The matrix material is pure quartz, and the hole material is doped quartz material. The hole period Λ of the cladding layer is 46μm, and the hole diameter d of the first type hole 2 2 It is 42 μm. Diameter d of the second type hole 3 and the third type hole 4 3 And d 3 Both are 23 μm. The refractive index of the first type hole 2, the second type hole 3 and the third type hole 4 are the same, which is 0.004 lower than that of the matrix material. When the transmission wavelength is 1064 nm, the fundamental mode field area in straight fiber is greater than 1800 μm 2 , When the bending radius is 20 cm, the mode field area of the fundamental mode reaches 1000 μm 2 -- the above. When the bending radius of the optical fiber reaches 5 cm, the fundamental mode loss is still less than 0.01 dB / m. In the case of straight fiber, the fundamental mode leakage loss is less than 0.01 dB / m, and the higher-order mode l...
Embodiment 2
[0052] The cross-sectional structure of the fiber is as figure 2 Shown. The matrix material is pure quartz, and the hole material is doped quartz material. The cladding hole period Λ is 46 μm, and the hole diameter d of the first type hole 2 2 It is 42 μm. Diameter d of the second type hole 3 and the third type hole 4 3 And d 4 Both are 23 μm. The refractive index of the first type hole 2, the second type hole 3 and the third type hole 4 are the same, which is 0.004 lower than the matrix material. Period Λ of the fourth type of hole 5 5 6 μm, hole diameter d 5 At 2 μm, the refractive index of the hole is 0.001 lower than that of the matrix material. When the transmission wavelength is 1064 nm, the fundamental mode field area of straight fiber can reach 1600 μm 2 Above; when the fiber bending radius is 50 cm, the mode field area of the fundamental mode is greater than 1500 μm 2 ; When the fiber bending radius is 30 cm, the mode field area of the fundamental mode still ex...
Embodiment 3
[0054] The cross-sectional structure of the fiber is as figure 2 Shown. The matrix material is pure quartz, and the hole material is doped quartz material. The cladding hole period Λ is 46 μm, and the hole diameter d of the first type hole 2 2 It is 42 μm. Diameter d of the second type hole 3 and the third type hole 4 3 And d 4 Respectively 28 μm and 23 μm, the refractive index of the first type hole 2, the second type hole 3 and the third type hole 4 are the same, which is 0.004 lower than that of the matrix material 1. Period Λ of the fourth type of hole 5 5 6 μm, hole diameter d 5 At 2 μm, the refractive index of the hole is 0.002 lower than that of the matrix material. When the transmission wavelength is 1064 nm, the fundamental mode field area in straight fiber can reach 1200 μm 2 the above. When the fiber bending radius is 15 cm, the mode field area of the fundamental mode is still 1200 μm 2 the above. In the case of straight fiber, the fundamental mode binding loss...
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