Rare earth ion annular doping double-cladding optical fiber
A double-clad optical fiber, rare earth ion technology, applied in the direction of clad optical fiber, optical waveguide light guide, etc., can solve the problems of difficult to control the uniformity and consistency of the structure, deteriorating the quality of the laser output beam, complicated manufacturing process, etc. The effect of small laser transmission loss, reduced use length, and increased doping area
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Embodiment 1
[0015] Such as figure 1 As shown in a, the double-clad fiber includes: a core 1, a ring-shaped doped region 2, and an inner cladding 3. In this embodiment, the matrix of the core 1 is quartz, and doped with germanium ions to achieve a high refractive index. The radius of the core 1 is 3.5um, and the radius of the core 1 must ensure that the signal light can be transmitted in a single mode in the core 1. figure 1 B is the refractive index distribution diagram of the D-type inner cladding annular doped optical fiber of the present invention, the material of the annular doping region 2 is quartz-doped Yb rare earth ions, and the refractive index is lower than the core 1, so that the numerical aperture of the core 1 is 0.15 . The annular doped region 2 is in the shape of a circular ring surrounding the core, with an inner diameter of 7um and an outer diameter of 200um. The inner cladding 3 is made of high-purity quartz tube, the refractive index is lower than that of the annular...
Embodiment 2
[0017] image 3 Shown is the second embodiment of the present invention. In this embodiment, the matrix of the core 1 is quartz and doped with germanium ions to achieve a high refractive index. The radius of the core 1 is 3.5um. The material of the annular doped region 2 is quartz doped with Nd rare earth ions, and its refractive index is lower than that of the core 1, so that the numerical aperture of the core 1 is 0.1. The shape of the annular doped region 2 is a circular ring surrounding the core, with an inner diameter of 7um and an outer diameter of 160um. The inner cladding 3 is made of a high-purity quartz tube, the refractive index of which is lower than that of the annular doped region 2, and the shape is rectangular with a side length of 200um×300um.
Embodiment 3
[0019] Figure 4 Shown is the third embodiment of the present invention. In this embodiment, the matrix of the core 1 is quartz, and germanium ions are doped to achieve a high refractive index. The radius of the core 1 is 5 um. The material of the annular doped region 2 is quartz doped with Yb rare earth ions, and its refractive index is lower than that of the core 1, so that the numerical aperture of the core 1 is 0.15. The shape of the annular doped region 2 is a circular ring surrounding the core, with an inner diameter of 10um and an outer diameter of 240um. The inner cladding 3 is made of high-purity quartz tube, the refractive index of which is lower than that of the annular doped region 2, and the shape is circular with a radius of 350um.
[0020] Such as figure 2 As shown, when the present invention works normally: the pump light enters the inner cladding layer 3 and is continuously absorbed by the rare earth ions in the annular doped region 2, and the pump light th...
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