Large-effective-area single mode optical fiber amplifier based on change of refractive index distribution of cladding
A technology of cladding refractive index and effective area, which is applied in the field of single-mode fiber amplifier with large effective area, can solve the problem that the single-mode and high power of fiber amplifier cannot be combined, and achieve the reduction of maximum power per unit volume and reduction of normalization The effect of optimizing the frequency and reducing the loss
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Embodiment approach 1
[0026] Large effective area single-mode fiber amplifiers by changing the cladding refractive index distribution, such as figure 1 , 2 shown. The amplifier includes: an optical fiber and a pump source 3 .
[0027] The refractive index of the core 1 of the optical fiber is 1.6, and the refractive index of the cladding 2 is 1.4.
[0028] The annular region with an axial length of 1 mm is etched away with a hydrofluoric acid solution, the thickness of the ring is 50 μm, and it is filled with quartz having a refractive index of 1.5 to form a filled region 4 .
[0029] The radius of the core 1 is 8 microns, the thickness of the cladding 2 is 50 microns, and the axial length of the filling region 4 is 1 mm.
[0030] The pumping source 3 pumps the fiber end face.
Embodiment approach 2
[0032] A large effective area single-mode fiber amplifier with a D-shaped filling area by changing the refractive index distribution of the cladding, such as image 3 , 4 shown. The amplifier includes: an optical fiber and a pump source 3 .
[0033] The refractive index of the core 1 of the optical fiber is 1.9, and the refractive index of the cladding 2 is 1.7.
[0034] The shape is etched away with hydrofluoric acid solution to form a D shape with a chord height of 10 microns and an axial length of 10 mm, and is filled with quartz having a refractive index of 1.8 to form a filled region 4 .
[0035] The radius of the core 1 is 100 microns, and the thickness of the cladding 2 is 100 microns.
[0036] The pumping source 3 pumps the side of the optical fiber.
Embodiment approach 3
[0038] A large effective area single-mode fiber amplifier with a helical rectangular groove whose filling area changes the refractive index distribution of the cladding, such as Figure 5 shown. The amplifier includes: an optical fiber and a pump source 3 .
[0039] The refractive index of the core 1 of the optical fiber is 1.8, and the refractive index of the cladding 2 is 1.6.
[0040] The filling area 4 is etched away with a hydrofluoric acid solution to form a spiral rectangular groove with a width of 10 microns, a pitch of 100 microns, and a depth equal to the thickness of the cladding layer 2. The filling area 4 is formed by filling with quartz having a refractive index of 1.7.
[0041] The radius of the core 1 is 50 microns, and the thickness of the cladding 2 is 80 microns.
[0042] The pumping source 3 pumps the fiber end face.
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